The DOI matches its Crossref record; 254 of the 257 references it cites were found in a registry or an index; 30 of the 187 sources its claims cite were checked for support.
Two-photon interference: the Hong–Ou–Mandel effect
Open accessAbstract
Nearly 30 years ago, two-photon interference was observed, marking the beginning of a new quantum era. Indeed, two-photon interference has no classical analogue, giving it a distinct advantage for a range of applications. The peculiarities of quantum physics may now be used to our advantage to outperform classical computations, securely communicate information, simulate highly complex physical systems and increase the sensitivity of precise measurements. This separation from classical to quantum physics has motivated physicists to study two-particle interference for both fermionic and bosonic quantum objects. So far, two-particle interference has been observed with massive particles, among others, such as electrons and atoms, in addition to plasmons, demonstrating the extent of this effect to larger and more complex quantum systems. A wide array of novel applications to this quantum effect is to be expected in the future. This review will thus cover the progress and applications of two-photon (two-particle) interference over the last three decades.
Overview
AI snapshot
Written from the paper’s full text.
TL;DR
This review covers the Hong–Ou–Mandel (HOM) effect, or two-photon/two-particle interference, over roughly three decades since its observation. It surveys the underlying beam-splitter theory and applications in precision measurement, quantum state analysis and engineering, communication, computation, multipartite interference, and non-photonic systems.
Key findings
- The HOM effect produces destructive interference of two-photon states exiting opposite output ports of a 50:50 beam splitter, giving the hallmark coincidence dip; for indistinguishable photons the output is \((|2_c\rangle - |2_d\rangle)/\sqrt{2}\).
- Precision applications include HOM timing measurements with reported average accuracy of 6 attoseconds and average precision of 16 attoseconds, and quantum optical coherence tomography with an improvement in resolution by a factor of 5 compared to OCT and detection of 1 µm features.
- Linear-optics Bell-state discrimination is limited to 50% success with one beam splitter and two detectors, but can be raised to 75% with ancillary entanglement and generally to \(1 - 2^{-N}\) with \(N\) interferences; KLM-type CZ and CNOT gates have success probabilities of 2/27 and 1/16, respectively.
- Non-photonic HOM interference has been observed with plasmons (initial visibility \(0.43 \pm 0.02\), later up to 0.95), phonons (\(0.52 \pm 0.03\)), collective atomic excitations (\(0.89 \pm 0.06\)), atoms (Rb bunching exceeding distinguishable-atom probability by 6 standard deviations; He visibility \(0.65 \pm 0.07\)), and electrons via anti-bunching/Pauli dips.
Methods
- Design: narrative review article, not a primary experimental study; it aggregates “the most prevalent uses of two-photon interference over the past three decades” into a coherent text.
- Data/sample: cited theoretical and experimental literature on HOM interference, including photonic, plasmonic, phononic, atomic, and electronic systems.
- Main analysis: thematic synthesis beginning with beam-splitter and two-photon interference theory, then covering precision measurements, quantum state analysis, quantum communication, quantum state engineering, quantum computation, multipartite/multimode generalizations, and non-photonic implementations.
Limitations
- The paper does not state a formal limitations section.
- Text-evident limitation: as a broad review, it does not provide a systematic search or selection protocol for the literature covered.
- Text-evident limitations in cited experiments include the initial plasmonic HOM dip visibility being below the classical limit, phonon results having statistical significance too small to exclude classical explanations with certainty, and QOCT facing challenges such as low signal and signal artifacts.
Model-written summary. Check it against the paper before relying on it.
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Cites
Statistics
Verification
Claims the paper makes
30 of 187 cited sources checked · 1 supported · 4 flagged · accuracy not yet measured
- Premisecitation
A two-phonon interference effect has been observed involving two trapped ions.
“Recently, such a two-phonon interference effect has been observed involving two trapped ions [181].”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites [181] Poem, 2012, Two-photon path-entangled states in multimode waveguides, Phys. Rev. Lett. source
The Abstract (page unavailable) describes an experiment on two-photon interference in multimode optical waveguides, not two-phonon interference involving trapped ions. The experimental-system passage describes laser light and photon-pair generation, rather than an ion-trap experiment. (LLM, conf=0.90)
Checked by a reasoning model — may be wrong.
Experimental — accuracy not yet measured
- Premisecitation
For the same bandwidth, QOCT benefits from an extra factor of 2 in resolution compared to classical OCT.
“Moreover, for the same bandwidth, QOCT benefits from an extra factor of 2 in resolution compared to classical OCT.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites [24] Dowling, 2008, Quantum optical metrology—the lowdown on high-N00N states, Contemp. Phys. source
Section 6, “Quantum Imaging and Sensing” (page not provided), reports a factor-of-two improvement in resolving power for quantum coherence tomography. It does not specify that the comparison with classical OCT is at the same bandwidth, so that qualifier is not established by our copy. (LLM, conf=0.83)
Experimental — accuracy not yet measured
- Findingcitation
A 3-dimensional QOCT image of onion-skin tissue coated with gold nanoparticles indicates a resolution of 1 μm.
“An example of a 3-dimensional image taken via QOCT for the skin of an onion coated in gold is shown in Fig. 3; this result indicates a resolution of 1 µm.”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites [33] Raymer, 2010, Interference of two photons of different color, Opt. Commun. source
The paper’s Conclusions discuss interference between photons of different colors and frequency conversion, not QOCT imaging. Searches for QOCT, onion skin, gold nanoparticles, and a 1 µm imaging resolution found no passage addressing the claimed image or resolution. (LLM, conf=0.78)
Experimental — accuracy not yet measured
- Premisecitation
The correlation noise properties at the outputs were found to be below the random partition noise (classically expected noise).
“the correlation noise properties at the outputs were studied and found to be below the random partition noise, i.e. classically expected noise (see Fig. 10a).”
Quote in the paperSubstantial claim1 of 1 sources checked- cites [199] Crespi, 2013, Integrated multimode interferometers with arbitrary designs for photonic boson sampling, Nat. Photon. source
The Experimental boson sampling section (pp. 3–4) reports output probability distributions for one-, two-, and three-photon experiments, but does not compare output correlation noise with random partition noise. Searches for those terms and for classical or distinguishable-particle noise comparisons found no passage establishing the claimed result. (LLM, conf=0.76)
Experimental — accuracy not yet measured
- Premisecitation
Actual plasmonic bunching was experimentally observed in 2013.
“actual plasmonic bunching was experimentally observed in 2013 [180].”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites [180] Lahini, 2012, Quantum walk of two interacting bosons, Phys. Rev. A source
The Figure 4 passage reports experimentally measured spatial bunching in thermal light, and the Abstract describes experiments in nonlinear photonic lattices. Neither passage identifies the effect as plasmonic or reports an observation in 2013, so those parts of the claim are unsupported. (LLM, conf=0.84)
Experimental — accuracy not yet measured
- Premisecitation
If one electron is delayed, a Pauli-dip of around 50% of the classical noise level was observed.
“If one electron is delayed, the noise properties change such that a Pauli-dip (analog to the HOM-dip for coincidences measurements) of around 50% of the classical noise level was observed.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites [199] Crespi, 2013, Integrated multimode interferometers with arbitrary designs for photonic boson sampling, Nat. Photon. source
The experimental-results section (p. 3) describes Hong–Ou–Mandel interference between photons, not delayed electrons or a Pauli dip. Searches for a delayed electron, Pauli dip, and a 50% classical noise level found no passage addressing the claimed observation. (LLM, conf=0.77)
Experimental — accuracy not yet measured
- Rests on an assumption: Fermions obey Fermi statistics, which leads to anti-bunching at a beam splitter.
- Premisecitation
Electrons can interfere in an HOM-like arrangement.
“it has been shown that not only bosons but also fermions in the form of electrons can interfere in an HOM-like arrangement.”
Quote in the paperNot a substantial claim2 of 3 sources checked- cites [196] Broome, 2013, Photonic boson sampling in a tunable circuit, Science source
The paper describes Hong–Ou–Mandel-style measurements with two input photons (p. 3) and reports two-photon interference (p. 4). Searches for electrons and fermionic HOM-like interference found no passage addressing the claimed electron result. (LLM, conf=0.78)
Experimental — accuracy not yet measured - cites [197] Spring, 2012, Boson sampling on a photonic chip, Science source
- cites [198] Tillmann, 2013, Experimental boson sampling, Nat. Photon. source
The Introduction (p. 1) describes Hong–Ou–Mandel interference between photons, and the Results (p. 3) report three-photon interference. Searches for electrons, fermions, and HOM-like electron interference found no passage in our copy addressing whether electrons can interfere in such an arrangement. (LLM, conf=0.75)
Experimental — accuracy not yet measured
- Findingnone given
Destructive and constructive interference can be adjusted by tailoring the symmetry of the overall input two-photon state.
“Nevertheless, destructive and constructive interference can be adjusted by tailoring the symmetry of the overall input two-photon state”
Quote in the paperSubstantial claim - Findingreasoning
For completely distinguishable qudit states, the two photons will bunch half of the time.
“While for completely distinguishable states, i.e. φ| ψ = 0, the two photons will bunch half of the time.”
Quote in the paperSubstantial claim - Findingreasoning
For the |Ψ+ Bell state input, the output photons always exit the BS together through the same output ports (bunching).
“For the |Ψ + state, we may notice that the output photons always exit the BS together through the same output ports, just as in the case of indistinguishable photons discussed previously, i.e. |1 a |1 b .”
Quote in the paperNot a substantial claim - Findingreasoning
For the Bell state |Ψ−_ab after a beam splitter, one photon is detected in each output port.
“In the second case, we have one photon per detector”
Quote in the paperSubstantial claim - Findingreasoning
The overall cloning fidelity of this scheme is F_cloning = 2/3 × 1 + 1/3 × 1/2 = 5/6.
“Overall, the cloning fidelity is then F cloning = 2 3 × 1 + 1 3 × 1 2 = 5 6”
Quote in the paperSubstantial claim - Findingreasoning
When the two qudit states are identical, there will be no coincidences.
“We note that when |φ and |ψ are identical there will be no coincidences and the last term in Eq (8) will vanish.”
Quote in the paperSubstantial claim - Findingreasoning
For distinguishable photons incident on a 50:50 BS, all classically expected outcomes are obtained.
“With no surprises, we obtain all the classically expected outcomes.”
Quote in the paperNot a substantial claim - Findingnone given
Maximal interference occurs when the input photons are indistinguishable at both input ports of the BS.
“In a two-photon interference experiment, maximal interference occurs when the input photons are indistinguishable at both input ports of the BS.”
Quote in the paperSubstantial claim - Findingcitation
If three indistinguishable photons are sent into the three input ports of a Bell-tritter, not all possible output distributions will be realized; bosonic coalescence leads to only 4 out of 10 possible output distributions.
“Analog to the two-photon HOM effect, if three indistinguishable photons are sent into the three input ports, not all possible output-distributions will be realized.As can be seen in Figure 7a for a three-dimensional Bell-port, bosonic coalescence leads to only 4 out of 10 possible output distributions.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [141] Navez, 2003, Cloning a real d-dimensional quantum state on the edge of the no-signaling condition, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
In MDI QKD implementations, attenuated laser pulses with the decoy state protocol were employed to achieve high secret key rates.
“In the aforementioned implementations of MDI QKD, to achieve high secret key rates, attenuated laser pulses were employed along with the decoy state protocol [101].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [101] Grice, 2011, Arbitrarily complete bell-state measurement using only linear optical elements, Phys. Rev. A source
- Premisecitation
Several realizations of the RRDPS protocol have been demonstrated experimentally using time-bin phase encoding and transverse spatial modes.
“Several realizations of the RRDPS protocol have recently been demonstrated experimentally using time-bin phase encoding [103][104][105][106] and using transverse spatial modes [107].”
Quote in the paperNot a substantial claim0 of 5 sources checked- cites [103] Pirandola, 2019, Advances in quantum cryptography source
A check is scheduled.
- cites [104] Wootters, 1982, A single quantum cannot be cloned, Nature source
- cites [105] Shor, 2000, Simple proof of security of the bb84 quantum key distribution protocol, Phys. Rev. Lett. source
A check is scheduled.
- cites [106] Zukowski, 1993, ‘Event-ready-detectors’ Bell experiment via entanglement swapping, Phys. Rev. Lett. source
A check is scheduled.
- cites [107] Bennett, 1993, Teleporting an unknown quantum state via dual classical and Einstein–Podolsky–Rosen channels, Phys. Rev. Lett. source
A check is scheduled.
- Premisecitation
The passive RRDPS protocol could also be extended to other high-dimensional QKD protocols.
“Finally, it has recently been shown that the passive RRDPS protocol could also be extended to other high-dimensional QKD protocols [108].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [108] Bennett, 1992, Communication via one- and two-particle operators on Einstein–Podolsky–Rosen states, Phys. Rev. Lett. source
- Premisecitation
Optimal 1→2 cloning of a qudit can be achieved with a fidelity F_cloning = 1/2 + 1/(d+1).
“Optimal 1 → 2 cloning (i.e. two clones of one original state) of a qudit can be achieved with a fidelity of F cloning = 1 2 + 1 d+1 [114][115][116][117].”
Quote in the paperNot a substantial claim0 of 4 sources checked- cites [114] Narla, 2016, Robust concurrent remote entanglement between two superconducting qubits, Phys. Rev. X source
Checked before — its earlier verdict is held back until a new check runs.
- cites [115] Sangouard, 2011, Quantum repeaters based on atomic ensembles and linear optics, Rev. Mod. Phys. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [116] Briegel, 1998, Quantum repeaters: the role of imperfect local operations in quantum communication, Phys. Rev. Lett. source
- cites [117] Fung, 2007, Phase-remapping attack in practical quantum-key-distribution systems, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Subpicosecond time intervals can be measured for photon pairs from parametric down-conversion, going far beyond the previous timing resolution of standard photodetectors (larger than 100 ps).
“Subpicosecond time intervals can now be measured for photon pairs from parametric down-conversion going far beyond the previous timing resolution of standard photodetectors, i.e. larger than 100 ps.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [4] Hong, 1987, Measurement of subpicosecond time intervals between two photons by interference, Phys. Rev. Lett. source
- Interpretationreasoning
The HOM effect can be used to perform precise timing measurements.
“Since then, several experiments have investigated the use of the HOM effect to perform precise timing measurements.”
Quote in the paperSubstantial claim - Premisenone given
The security of the RRDPS protocol is largely enhanced when considering large dimensions.
“In particular, the security of the RRDPS protocol is largely enhanced when considering large dimensions; therefore, it is worth exploring different implementations achieving larger dimensions.”
Quote in the paperSubstantial claim - Premisenone given
For two-qubit gates where interaction is required, the HOM effect is relied heavily upon.
“For twoqubit gates where interaction is required, the HOM effect is relied heavily upon.”
Quote in the paperNot a substantial claim - Premisecitation
In the passive RRDPS scheme, two-photon interference is exploited to achieve extremely large dimensions such as 10^5.
“In this scheme, the two-photon interference is exploited to achieve extremely large dimensions such as 10 5 .”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [85] Yuan, 2007, Synchronized independent narrow-band single photons and efficient generation of photonic entanglement, Phys. Rev. Lett. source
- Premisecitation
For a balanced beam splitter, simultaneous detections at the two output ports for two orthogonally polarized photons behaves like the singlet state, i.e., a Bell state measurement.
“they note that, for a balanced beam splitter, the simultaneous detections at the two output ports behaves like the singlet state for two orthogonally polarized photons, i.e., a Bell state measurement, as we know it today.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [3] Ou, 1987, Relation between input and output states for a beam splitter, Opt. Commun. source
- Premisecitation
The measurement-device-independent (MDI) QKD protocol removes all detector side channel attacks.
“In order to overcome the impracticality of this scheme, the measurement-device-independent (MDI) QKD protocol has been proposed [84], where all detector side channels attacks are now removed.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [84] Chaneliere, 2007, Quantum interference of electromagnetic fields from remote quantum memories, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationnone given
The HOM effect plays an essential role in quantum metrology.
“Finally, another field of research where the HOM effect plays an essential role for precision measurement is quantum metrology”
Quote in the paperNot a substantial claim - Premisecitation
Further experimental demonstrations of QOCT have reported detection of micron-sized features even for biological samples.
“Further experimental demonstrations of QOCT have also been reported, where micron-sized features are detected even for the case of biological samples [26][27][28].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [26] Zeilinger, 1998, Quantum entanglement: a fundamental concept finding its applications, Phys. Scr. T source
- cites [27] Nagali, 2009, Optimal quantum cloning of orbital angular momentum photon qubits through Hong–Ou–Mandel coalescence, Nat. Photon. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [28] Karimi, 2014, Exploring the quantum nature of the radial degree of freedom of a photon via Hong–Ou–Mandel interference, Phys. Rev. A source
- Interpretationreasoning
The HOM effect can be used as a highly precise timing measurement tool.
“Once again, the HOM effect is used as a highly precise timing measurement tool.”
Quote in the paperSubstantial claim - Premisecitation
Any input state of the beam splitter with one photon in each input port can be rewritten as a superposition of symmetric and antisymmetric Bell states.
“It is shown in [111] that this can be rewritten as a superposition of symmetric and antisym- metric Bell states”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [111] Guan, 2015, Experimental passive round-robin differential phase-shift quantum key distribution, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Discrimination of Bell states with linear optics and no ancillary modes is bound to a 50% discrimination success rate.
“For example, if we use exclusively linear optics and no other ancillary modes, we are bound to a 50% discrimination success rate [72].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [72] Okamoto, 2008, Beating the standard quantum limit: phase super-sensitivity of N-photon interferometers, New J. Phys. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
By considering limits dictated by statistical estimation theory, it is possible to push the time resolution of a HOM interferometer to sub-femtosecond resolutions.
“However, it has recently been shown that by considering the limits dictated by statistical estimation theory, it is possible to push the time resolution of a HOM interferometer to sub-femtosecond resolutions [20].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [20] Kim, 1999, Quantum interference by two temporally distinguishable pulses, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisenone given
The KLM linear optical implementation of the CNOT quantum gate plays the key role for achieving quantum state joining.
“The Knill-Laflamme-Milburn (KLM) linear optical implementation of the CNOT quantum gate, which will be discussed in detail in Sec.VI A, plays the key role for achieving quantum state joining.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [76] Kaltenbaek, 2006, Experimental interference of independent photons, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisenone given
Practical QKD implementations do not necessarily follow the assumptions made in security proofs.
“Nevertheless, practical implementations do not necessarily follow the assumptions made in the security proofs.”
Quote in the paperNot a substantial claim - Premisecitation
A CZ gate can be constructed using two 50:50 beam splitters and two nonlinear sign (NS) gates.
“It was found that a CZ gate can be constructed using two 50:50 BS and two so-called nonlinear sign (NS) gates [76], see Fig. 5a).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [76] Kaltenbaek, 2006, Experimental interference of independent photons, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationreasoning
When conditioning on coincidence detection between the two output ports, the HOM effect acts as a filter for the antisymmetric component for any arbitrary high-dimensional input state.
“Therefore, when conditioning on coincidence detection between the two output ports, the HOM effect acts as a filter for the antisymmetric component for any arbitrary high-dimensional input state.”
Quote in the paperSubstantial claim - Premisecitation
The entanglement swapping idea can be applied to entangle a pair of transmon qubits by interfering two microwave photons at a microwave beam splitter junction.
“This idea can be applied to other domains as well, for example to entangle a pair of transmon qubits by interfering two microwave photons at a microwave beam splitter junction [88].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [88] Bernien, 2012, Two-photon quantum interference from separate nitrogen vacancy centers in diamond, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisereasoning
An arbitrary polarization qubit can be optimally cloned using the HOM effect by interfering it on a beam splitter with an ancilla in a maximally mixed polarization state.
“For example, an arbitrary polarization qubit |1 s = α |1 H + β |1 V , where |α| 2 + |β| 2 = 1, can be optimally cloned using the HOM effect by interfering it on a beam splitter with an ancilla that is in a maximally mixed polarization state”
Quote in the paperSubstantial claim0 of 4 sources checked- cites [114] Narla, 2016, Robust concurrent remote entanglement between two superconducting qubits, Phys. Rev. X source
Checked before — its earlier verdict is held back until a new check runs.
- cites [115] Sangouard, 2011, Quantum repeaters based on atomic ensembles and linear optics, Rev. Mod. Phys. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [116] Briegel, 1998, Quantum repeaters: the role of imperfect local operations in quantum communication, Phys. Rev. Lett. source
- cites [117] Fung, 2007, Phase-remapping attack in practical quantum-key-distribution systems, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
A passive version of the RRDPS QKD was proposed to overcome difficulties in achieving stable variable-delay interferometers.
“In order to overcome the difficulties in achieving stable variable-delay interferometers, a passive version of the RRDPS QKD was proposed [85].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [85] Yuan, 2007, Synchronized independent narrow-band single photons and efficient generation of photonic entanglement, Phys. Rev. Lett. source
- Premisecitation
Security loopholes have been recognized to pose a threat to the security of realistic QKD implementations.
“Thus, security loopholes have, early on, been recognized to pose a threat to the security of realistic QKD implementations [91,92].”
Quote in the paperNot a substantial claim0 of 2 sources checked - Premisecitation
Dimensions ranging between 5 and 128 have been achieved in the time-bin configuration of RRDPS using interferometers with variable delays.
“Dimensions ranging between 5 and 128 have been achieved in the time-bin configuration using interferometers with variable delays.”
Quote in the paperNot a substantial claim - Premisecitation
QOCT has been proposed to exploit automatic dispersion cancellation involved in two-photon interference.
“In order to overcome the resolution limitations, a technique known as quantum optical coherence tomography (QOCT) has been proposed to exploit the automatic dispersion cancellation involved in the two-photon interference effect [24].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [24] Dowling, 2008, Quantum optical metrology—the lowdown on high-N00N states, Contemp. Phys. source
- Interpretationreasoning
The HOM effect is important in quantum metrology relying on entanglement of multi-photon states.
“Thus, one can already appreciate the importance of the HOM effect in quantum metrology relying on the entanglement of multi-photon states.”
Quote in the paperSubstantial claim - Interpretationreasoning
The ability to discriminate the |Ψ- Bell state, by taking advantage of its fermionic behaviour, is central to the concept of Bell state analysis.
“Hence, the ability to discriminate the |Ψ -Bell state, by taking advantage of its fermionic behaviour, is central to the concept of Bell state analysis”
Quote in the paperSubstantial claim - Premisenone given
The resolution in space and phase is enhanced by a factor of N, i.e. scales as 1/N, for N00N states.
“The resolution in space and phase is enhanced by a factor of N, i.e. scales as 1/N.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [12] Ou, 1989, Fourth-order interference technique for determining the coherence time of a light beam, J. Opt. Soc. Am. B source
- Premisecitation
For N=2, the N00N state is realized by two indistinguishable photons incident on both input ports of a 50:50 BS, resulting in HOM interference.
“For the case of N = 2 [36,37], we recognize the state from Eq. ( 5) where two indistinguishable photons are made incident onto both input ports of a 50:50 BS, resulting in HOM interference.”
Quote in the paperSubstantial claim0 of 2 sources checked- cites [36] Giovannini, 2015, Spatially structured photons that travel in free space slower than the speed of light, Science source
Checked before — its earlier verdict is held back until a new check runs.
- cites [37] Bouchard, 2016, Observation of subluminal twisted light in vacuum, Optica source
Checked before — its earlier verdict is held back until a new check runs.
- Premisenone given
The action of the beam splitter is at the heart of the two-photon interference effect, providing the mixing between the two input modes.
“The action of the beam splitter (BS) is at the heart of the two-photon interference effect, providing the mixing between the two input modes.”
Quote in the paperSubstantial claim - Interpretationcitation
It is possible to combine N interferences and raise the success rate to 1 - 2^-N.
“It is possible to combine N interferences and raise the success rate to 1 -2 -N .”
Quote in the paperNot a substantial claim - Interpretationreasoning
The HOM effect holds great potential for applications where dispersion can seriously limit optical applications.
“Thus, the two-photon interference effect holds great potential for applications where dispersion can seriously limit optical applications.”
Quote in the paperSubstantial claim - Premisecitation
Interfering photons emitted by two different trapped atoms at a beam splitter can perform a linear optical Bell state measurement that, if successful, swaps entanglement from being between each atom and its photon to being between the two atoms alone.
“If successful, this procedure has swapped the entanglement from being between each atom and its photon to being between the two atoms alone.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [86] Yuan, 2008, Experimental demonstration of a bdcz quantum repeater node, Nature source
- Premisecitation
In [20], an average accuracy and average precision of 6 attoseconds and 16 attoseconds were achieved, respectively.
“By doing so, an average accuracy and average precision of 6 attoseconds and 16 attoseconds were achieved, respectively.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [20] Kim, 1999, Quantum interference by two temporally distinguishable pulses, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationreasoning
HOM can be adopted as a powerful tool to directly measure the overlap between two single photon wavepackets.
“Thus, HOM can be adopted as a powerful tool to directly measure the overlap between two single photon wavepackets.”
Quote in the paperSubstantial claim - Premisenone given
The simplest implementation of Bell state discrimination uses only one interference at a single beam splitter and two detectors.
“The simplest implementation uses only one interference at a single beam splitter and two detectors.”
Quote in the paperNot a substantial claim - Premisecitation
The HOM visibility has been used to characterize the level of mode indistinguishability for a wide range of single photon sources.
“Indeed, the HOM visibility has been used to characterize the level of mode indistinguishability for a wide range of single photon sources, i.e. spontaneous parametric down-conversion [52,53], quantum dots [54][55][56][57][58], atomic vapours [59][60][61][62][63], nitrogen-vacancy centres in diamond [64][65][66], trapped ions [67], trapped neutral atoms [68,69], and molecules [70,71].”
Quote in the paperNot a substantial claim0 of 4 sources checked- cites [52] Lopez-Mago, 2012, Quantum-optical coherence tomography with collinear entangled photons, Opt. Lett. source
- cites [53] Erkmen, 2006, Phase-conjugate optical coherence tomography, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- cites [54] Banaszek, 2007, Blind dispersion compensation for optical coherence tomography, Opt. Commun. source
- cites [59] Giovannetti, 2011, Advances in quantum metrology, Nat. Photon. source
- Premisecitation
Most schemes for high photon number N00N states are in the spirit of two-photon or multi-photon interference set by the HOM effect.
“Several schemes have thus been proposed to achieve high photon number N00N states experimentally [38][39][40][41] along with experimental demonstrations [42][43][44][45][46][47][48][49][50][51], where most of these schemes are in the spirit of the two-photon, or more generally multi-photon, interference set by the HOM effect.”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [38] Lyons, 2018, How fast is a twisted photon?, Optica source
Checked before — its earlier verdict is held back until a new check runs.
- cites [42] Kim, 2017, Two-photon interference of polarization-entangled photons in a Franson interferometer, Sci. Rep. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [51] Nasr, 2009, Quantum optical coherence tomography of a biological sample, Opt. Commun. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Several side channel attacks have been demonstrated experimentally, showing the vulnerability of commercial QKD systems under study.
“For instance, several side channel attacks have been demonstrated experimentally, showing the vulnerability of the commercial QKD systems under study [93,94].”
Quote in the paperSubstantial claim0 of 2 sources checked- cites [93] Specht, 2011, A single-atom quantum memory, Nature source
Checked before — its earlier verdict is held back until a new check runs.
- cites [94] Kiraz, 2005, Indistinguishable photons from a single molecule, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
It is the even-order effects of dispersion, such as group-velocity dispersion, that are cancelled in two-photon interference.
“In particular, it is the even-order effects of dispersion, such as group-velocity dispersion, that are cancelled [22].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [22] Einstein, 1935, Can quantum-mechanical description of physical reality be considered complete?, Phys. Rev. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
A noncommon-path HOM interferometer can measure time shifts with resolutions on the order of a few femtoseconds.
“In the works mentioned above, a noncommon-path HOM interferometer is employed to measure time shifts with resolutions on the order of a few femto-seconds (micrometers), where the time shifts are obtained by assessing the shift of the HOM dip.”
Quote in the paperSubstantial claim0 of 3 sources checked- cites [16] Moschandreou, 2018, Experimental study of Hong–Ou–Mandel interference using independent phase randomized weak coherent states, J. Lightwave Technol. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [17] Kim, 2020, Hong–Ou–Mandel interference of two independent continuous-wave coherent photons, Photon. Res. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [18] Ferreira da Silva, 2013, Proof-of-principle demonstration of measurement-device-independent quantum key distribution using polarization qubits, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Quantum state joining has been achieved experimentally for the polarization state of two photons, transferring the information onto a third single photon by exploiting that a single particle can occupy different spatial modes and polarizations.
“Experimentally, quantum state joining has been achieved for the polarization state of two photons, in which the information was transferred onto a third single photon by exploiting the fact that a single particle can occupy different spatial modes and polarizations [120].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [120] Gerhardt, 2011, Full-field implementation of a perfect eavesdropper on a quantum cryptography system, Nat. Commun. source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationreasoning
To achieve the Heisenberg limit for phase sensitivity, one must consider high photon number N00N states.
“Thus, in order to achieve the fundamental quantum limit, also known as the Heisenberg limit, for phase sensitivity, one must consider high photon number N00N states.”
Quote in the paperSubstantial claim - Premisecitation
A Bell-tritter redistributes the three incoming photons to the three output ports in an unbiased way.
“which redistributes the three incoming photons to the three output ports in an unbiased way.”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [139] Zhao, 2014, Entangling different-color photons via time-resolved measurement and active feed forward, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [140] Peres, 2003, How the no-cloning theorem got its name, Fortschr. Phys. source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationcitation
This is a proof for atomic bunching.
“and as such a proof for atomic bunching [193].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [193] Tichy, 2013, Limits to multipartite entanglement generation with bosons and fermions, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisereasoning
The NS gate is probabilistic, with a success probability of p_NS = 1/4 for an arbitrary input state without feedforward.
“This post-selection process renders the NS gate to be probabilistic, with a success probability of p NS = 1/4 for an arbitrary input state without feedforward.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [76] Kaltenbaek, 2006, Experimental interference of independent photons, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationown data
The plasmonic result is an indication of two-plasmon quantum interference.
“the result is a nice indication of a two plasmons quantum interference.”
Quote in the paperSubstantial claim - Interpretationreasoning
The triad phase is a genuine three-photon interference effect with no analog in the standard HOM experiment.
“Thus, it has to be considered a genuine three-photon interference effect with no analog in the standard HOM experiment.”
Quote in the paperSubstantial claim - Premiseown data
For waiting times when the hopping probability of the phonons was 50%, bunching was observed.
“For waiting times when the hopping probability of the phonons was 50%, bunching was observed (see Fig. 8c and d).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [181] Poem, 2012, Two-photon path-entangled states in multimode waveguides, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Another recent experiment demonstrated additional features unique to multi-partite interferences.
“another recent experiment demonstrated that there are additional features unique to multi-partite interferences [144].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [144] De Martini, 2002, Experimental realization of the quantum universal not gate, Nature source
- Premisecitation
The probability of finding two indistinguishable atoms in one trap exceeded the probability for distinguishable atoms by 6 standard deviations.
“The resulting probability of finding two indistinguishable atoms in one trap exceeded the probability for distinguishable atoms by 6 standard deviations”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [190] Metcalf, 2013, Multiphoton quantum interference in a multiport integrated photonic device, Nat. Commun. source
- Premisecitation
The upper bound for the NS gate was found to be 1/2.
“The upper bound for the NS gate was found to be 1/2 [122].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [122] Acín, 2007, Device-independent security of quantum cryptography against collective attacks, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Calculating the output probability distribution for a sufficiently large number of photons interfering in a large multiport arrangement is exponentially hard to solve classically.
“It has been shown that calculating the output probability distribution for a sufficiently large number of photons interfering in a large multiport arrangement is exponentially hard to solve classically”
Quote in the paperNot a substantial claim0 of 2 sources checked - Premisereasoning
Three photons can interfere in a tritter if they are indistinguishable.
“Similar to the two photon HOM-interference, three photons can interfere in a tritter if they are indistinguishable.”
Quote in the paperNot a substantial claim - Premisecitation
A quantum walk with phonons has been demonstrated in a trapped ion crystal.
“A nice example recently demonstrated a quantum walk with phonons implemented in a trapped ion crystal [189].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [189] Tillmann, 2015, Generalized multiphoton quantum interference, Phys. Rev. X source
- Premisecitation
For three photons, an additional collective phase is required to describe the photons' scattering behaviour.
“For three photons for example, an additional collective phase is required to describe the photons' scattering behaviour [146][147][148].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [146] Vitelli, 2013, Joining the quantum state of two photons into one, Nat. Photon. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [147] Passaro, 2013, Joining and splitting the quantum states of photons, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- cites [148] Knill, 2003, Bounds on the probability of success of postselected nonlinear sign shifts implemented with linear optics, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
It is possible to implement the NS gate in the polarization basis, using polarization rotations instead of variable beam splitters, with a success probability of (3 - √2)/7.
“It is also possible to implement the NS gate in the polarization basis, wherein polarization rotations are used instead of the variable BS; this also has a success probability of (3 -√ 2)/7.”
Quote in the paperNot a substantial claim - Premisecitation
The deficiency was resolved by an improved experiment using two separate sources of single electrons emitted from a triggered quantum dot.
“Recently, this deficiency was resolved by an improved experiment, using two separate sources of single electrons emitted from a triggered quantum dot [197,198].”
Quote in the paperNot a substantial claim0 of 2 sources checked - Premisecitation
A multiphoton interference in a multiport has enabled the first quantum teleportation of a high-dimensional quantum state.
“a multiphoton interference in a multiport has enabled the first quantum teleportation of a high-dimensional quantum state [164].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [164] Weihs, 1996, Two-photon interference in optical fiber multiports, Phys. Rev. A source
- Premisenone given
The property of multiphoton interference is not limited to a 2-input/2-output beam splitter but can be generalized to more particles in more complicated beam splitter networks with multiple-input and multiple-output ports (multiports).
“However, the property of multiphoton interference is not limited to this rather simple (and yet powerful) case, but it can be generalized to more particles in more complicated beam splitter networks with multipleinput and multiple-output ports, i.e. so-called multiports.”
Quote in the paperNot a substantial claim - Premisecitation
In the experiment, a three-dimensional quantum state was teleported using one additional ancillary photon.
“In the experiment, a three-dimensional quantum state was teleported using one additional ancillary photon.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [164] Weihs, 1996, Two-photon interference in optical fiber multiports, Phys. Rev. A source
- Premisecitation
The first fermionic two-particle interference was studied in 1998 with a constant stream of colliding electrons produced in a two-dimensional electron gas.
“The first such interference was studied in 1998 with a constant stream of colliding electrons produced in a two-dimensional electron gas [196].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [196] Broome, 2013, Photonic boson sampling in a tunable circuit, Science source
- Premisenone given
It is possible to achieve useful quantum computation without a universal quantum computer, by having a device that performs a single algorithm.
“It is possible to achieve a useful quantum computation without resorting to a universal quantum computer.In this case, it is sufficient to have a device that performs a single algorithm.”
Quote in the paperNot a substantial claim - Interpretationreasoning
There is a full analogy between the HOM effect and the SWAP test.
“This is sufficient to conclude with a full analogy between the HOM effect and the SWAP test.”
Quote in the paperSubstantial claim - Interpretationreasoning
A destructive SWAP test can be implemented by measuring directly the two systems in the Bell basis.
“This suggests that one could also implement a destructive SWAP test by measuring directly the two systems in the Bell basis.”
Quote in the paperSubstantial claim - Premisecitation
Collective excitations have been tested with respect to interference effects in a recent experiment using a Rb ensemble.
“collective excitations have also been tested with respect to interference effects in a recent experiment using a Rb ensemble [182].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [182] Defienne, 2016, Two-photon quantum walk in a multimode fiber, Sci. Adv. source
- Premisecitation
The most efficient CZ gate has a success probability of 2/27, utilizing two single photon ancillary modes and only four beam splitters.
“The most efficient CZ gate has a success probability of 2/27, utilizing two single photon ancillary modes and only four BS [126].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [126] Yin, 2016, Measurement-device-independent quantum key distribution over a 404 km optical fiber, Phys. Rev. Lett. source
- Premisecitation
The trapped-atom results were extended to a complex quantum walk of atoms in a two-dimensional optical lattice.
“Shortly after this initial step, these results were extended to a complex quantum walk of atoms in a two-dimensional optical lattice [191].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [191] Ferreri, 2019, Temporally multimode four-photon Hong–Ou–Mandel interference, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Bunching was confirmed through a dip with visibility up to 0.89±0.06 in correlation measurements of two photons by varying distinguishability and splitting ratio.
“bunching was confirmed through a dip with a visibility up to 0.89±0.06 in the correlation measurements of the two photons (see Fig. 8f) by varying the distinguishability and splitting ratio.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [182] Defienne, 2016, Two-photon quantum walk in a multimode fiber, Sci. Adv. source
- Interpretationreasoning
This result is a clear indication for bunching of massive systems.
“which can be considered a clear indication for bunching of massive systems.”
Quote in the paperSubstantial claim - Premisecitation
In one experiment, two laser-cooled Rb atoms trapped in an optical tweezer were perfectly controlled in all internal and external degrees of freedom, making them indistinguishable.
“two laser-cooled Rb atoms trapped in an optical tweezer were perfectly controlled in all internal and external degrees of freedom, thereby making them indistinguishable [190].”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [190] Metcalf, 2013, Multiphoton quantum interference in a multiport integrated photonic device, Nat. Commun. source
- Premisecitation
The complex interference of multiple photons in multiports enables the generation of multi-partite entanglement.
“The complex interference of mutliple photon in multiports cannot only be used in teleportation schemes, it also enables the generation of multi-partite entanglement [165].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [165] Ou, 2007 source
- Premisenone given
In general, the output probability distribution of three photons in a tritter depends on the input distribution as well as the exact unitary transformation of the tritter.
“In general, the output probability distribution of the three photons depends on the input distribution as well as the exact unitary transformation of the tritter.”
Quote in the paperNot a substantial claim - Premisecitation
The implementation of the CNOT gate requires two NS gates and two additional 50:50 beam splitters acting on the target qubit.
“The implementation of the CNOT gate is similar to that of the CZ gate in that it requires two NS gates; however, two additional 50:50 BS are required acting on the target qubit [127], as shown in Fig. 5.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [127] Lo, 2005, Decoy state quantum key distribution, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Using a stimulating Raman pulse as a beam splitter, collective excitations can be interfered and bunched together in either of two Zeeman states.
“Using a stimulating Raman pulse that acts as a beam splitter, the excitations can be interfered and bunched together in either of the two Zeeman states (see Fig. 8e).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [182] Defienne, 2016, Two-photon quantum walk in a multimode fiber, Sci. Adv. source
- Premisecitation
After appropriate postselection, the three-dimensional quantum state was found to be teleported to the photon that was initially a part of the entangled pair.
“After appropriate postselection, the three-dimensional quantum state was found to be teleported to the photon, which was initially a part of the entangled pair.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [164] Weihs, 1996, Two-photon interference in optical fiber multiports, Phys. Rev. A source
- Premiseown data
The phonon experiment's statistical significance of fidelity was too small to exclude classical explanations with certainty (0.52±0.03).
“Although the statistical significance of the fidelity was too small to exclude classical explanations with certainty (0.52±0.03)”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [181] Poem, 2012, Two-photon path-entangled states in multimode waveguides, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationreasoning
The CNOT gate is a probabilistic process with success probability p_CNOT = p_NS^2 = 1/16.
“Again, since the CNOT gate is based around the NS gate, it is a probabilistic process with success probability p CNOT = p 2 NS = 1/16.”
Quote in the paperNot a substantial claim - Premisecitation
HOM interference was further applied to study an electron gas in the integer quantum Hall regime at filling factor 2.
“the HOM interference was further applied to study an electron gas in the integer quantum Hall regime at a filling factor of 2”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [200] Spagnolo, 2014, Experimental validation of photonic boson sampling, Nat. Photon. source
- Premisecitation
Two recent experiments have shown a two-atom HOM interference.
“two recent experiments, both using very different approaches, have shown exactly this: a two-atom HOM interference.”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [190] Metcalf, 2013, Multiphoton quantum interference in a multiport integrated photonic device, Nat. Commun. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [192] Luo, 2019, Quantum teleportation in high dimensions, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisecitation
Similar concepts and results, such as a zero-transmission law for various output distributions, can be generalized to n bosons sent in the n ports of a Bell-multiport.
“Furthermore, similar concepts and results, such as a zero-transmission law for various output distributions, can also be generalized to n bosons sent in the n ports of a Bell-multiport [149][150][151][152].”
Quote in the paperNot a substantial claim0 of 4 sources checked- cites [149] Raplh, 2001, Simple scheme for efficient linear optics quantum gates, Phys. Rev. A source
- cites [150] Zou, 2002, Teleportation implementation of nondeterministic quantum logic operations by using linear optical elements, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- cites [151] Scheel, 2004, Quantum gates and decoherence source
Checked before — its earlier verdict is held back until a new check runs.
- cites [152] Knill, 2002, Quantum gates using linear optics and postselection, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- Interpretationreasoning
Since two NS gates are required, the total success probability of the CZ gate is p_CZ = p_NS^2.
“Since two NS gates are required, the total success probability of this CZ gate is p CZ = p 2 NS .”
Quote in the paperSubstantial claim - Premisecitation
The HOM effect is an optical implementation of the (destructive) SWAP test.
“Perhaps surprisingly, the analogy between them goes all the way down to formal equivalence: the HOM effect is an optical implementation of the (destructive) SWAP test [135].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [135] Islam, 2019, Scalable high-rate, high-dimensional time-bin encoding quantum key distribution, Quantum Sci. Technol. source
Checked before — its earlier verdict is held back until a new check runs.
- Premisereasoning
If the two input states are identically equal, the second term in the last line of Eq. (17) vanishes and the outcome of the measurement must be |'0' with probability 1.
“Equivalently in terms of the states |φ and |ψ , if they are identically equal, the second term in the last line of Eq. ( 17) vanishes and the outcome of the measurement must be |'0' with probability 1.”
Quote in the paperSubstantial claim - Premisereasoning
The visibility of leviton interference is significantly higher than that of the electronic HOM interference described in the last paragraph.
“Because levitons are propagating with less disturbance, the visibility of the interference is significantly higher than the one of the electronic HOM interference described in the last paragraph (see Fig. 10b)).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [201] Bentivegna, 2015, Experimental scattershot boson sampling, Sci. Adv. source
- Premisecitation
From noise measurements, a g(2) value up to 1 was deduced if both levitons were emitted simultaneously, which is a signature for antibunching.
“From the noise measurements, a g (2) value up to 1 was deduced if both levitons were emitted simultaneously, which is a signature for antibunching.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [201] Bentivegna, 2015, Experimental scattershot boson sampling, Sci. Adv. source
- Rests on an assumption: Fermions obey Fermi statistics, which leads to anti-bunching at a beam splitter.
- Premisecitation
Two-particle interference still inspires physicists to study its connection to novel systems such as magnons, Bogoliubov quasiparticles, massless Dirac fermions in topological insulators and graphene, or to transfer the idea to analog situations with bright solitons.
“it still inspires physicists to study its connection to novel systems such as quantized spin waves, i.e. magnons [207], Bogoliubov quasiparticles [208], massless Dirac fermions in topological insulators and graphene [209] or to transfer the idea to analog situations, e.g. with bright solitons [210].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [207] Wang, 2012, Hong–Ou–Mandel interference mediated by the magnetic plasmon waves in a three-dimensional optical metamaterial, Opt. Express source
- cites [208] Heeres, 2013, Quantum interference in plasmonic circuits, Nat. Nanotechnol. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [209] Toyoda, 2015, Hong-Ou-Mandel interference of two phonons in trapped ions, Nature source
- Interpretationnone given
Two-particle interferences has led to many fundamental demonstrations in non-photonic systems such as plasmons, phonons, atoms and electrons.
“it has also led to many fundamental demonstrations in non-photonic systems such as plasmons, phonons, atoms and electrons.”
Quote in the paperNot a substantial claim
- It may state two separate claims as one. 59
- Probably not a substantial claim. 54
It may state two separate claims as one.
PremisecitationDifferent plasmonic experiments achieved visibilities far beyond the classical limit up to 0.95, fully certifying the quantumness of two-plasmon interferences.
“different experiments using different plasmonic configurations, and off-chip photon detection schemes achieved visibilities far beyond the classical limit up to 0.95 [183][184][185][186], thus fully certifying the quantumness of the two plasmon interferences.”
Quote in the paperSubstantial claim3 of 4 sources checked- cites [183] Politi, 2009, Integrated quantum photonics, IEEE J. Select. Top. Quantum Electron. source
- cites [184] Peruzzo, 2010, Quantum walks of correlated photons, Science source
The 'Quantum walks of correlated particles' section (pp. 2, 5) describes off-chip photon detection and two-photon correlations that violate a classical limit by up to 76 standard deviations. It studies photons in a waveguide chip, not plasmons in plasmonic configurations, and does not report interference visibility of 0.95. (LLM, conf=0.88)
Experimental — accuracy not yet measured - cites [185] Poulios, 2014, Quantum walks of correlated photon pairs in two-dimensional waveguide arrays, Phys. Rev. Lett. source
The Fig. 4 passage (indexed under Abstract; page unavailable) reports 96.8 ± 2.5% visibility, and the discussion of Fig. 3 reports violations of a classical limit. But this is an experiment with photon pairs in fused-silica waveguides, not two-plasmon interference in plasmonic configurations; it also does not report a maximum visibility of 0.95. (LLM, conf=0.88)
Experimental — accuracy not yet measured - cites [186] Owens, 2011, Two-photon quantum walks in an elliptical direct-write waveguide array, New J. Phys. source
Section 4, “Two-photon walks” (page not provided), reports photon interference visibility of 38 ± 2%, not 0.95, in a waveguide array rather than a plasmonic configuration. Section 5, “Discussion” (page not provided), explicitly says the resulting probability distributions did not exhibit a conclusively quantum signature, contrary to the claim of full certification. (LLM, conf=0.90)
Checked by a reasoning model — may be wrong.
Experimental — accuracy not yet measured
It may state two separate claims as one.
PremisecitationAlthough tritters have been used to demonstrate quantum features in the two-photon regime, only recently have three photon HOM coalescences been observed.
“Although tritters have been used to demonstrate quantum features in the two-photon regime [138,142,143], only recently have three photon HOM coalescences been observed [141,144].”
Quote in the paperNot a substantial claim4 of 5 sources checked- cites [138] Zhang, 2016, Engineering two-photon high-dimensional states through quantum interference, Sci. Adv. source
The Introduction and Results report two-photon HOM interference and quantum-state measurements, supporting the two-photon aspect of the cited clause. But Materials and Methods identify the device as a 50:50 beamsplitter, not a tritter; this paper therefore does not support the claim that tritters were used. (LLM, conf=0.84)
Experimental — accuracy not yet measured - cites [142] Nagali, 2010, Experimental optimal cloning of four-dimensional quantum states of photons, Phys. Rev. Lett. source
The experimental-layout passage reports HOM interference between two photons at a balanced beam splitter, and the Fig. 2 and Fig. 3 captions likewise identify two-photon coalescence. Searches for tritters and three-photon HOM coalescence found no passage in our copy addressing either attributed claim; the paper's two-photon result does not establish a tritter experiment. (LLM, conf=0.76)
Experimental — accuracy not yet measured - cites [143] Bouchard, 2017, High-dimensional quantum cloning and applications to quantum hacking, Sci. Adv. source
The citation is attached to the claim about observed three-photon HOM coalescence. The Results (Fig. 1) describe HOM coalescence curves for two photons, and Materials and Methods specifies a two-photon interference experiment at a 50:50 beam splitter; this paper reports a two-photon observation, not a three-photon one. (LLM, conf=0.88)
Checked by a reasoning model — may be wrong.
Experimental — accuracy not yet measured - cites [141] Navez, 2003, Cloning a real d-dimensional quantum state on the edge of the no-signaling condition, Phys. Rev. A source
The Introduction and Discussion and Conclusion discuss quantum cloning and no-signaling, not tritters or photon interference. Searches for tritters, two-photon experiments, and three-photon Hong–Ou–Mandel coalescence found no passage addressing the claim. (LLM, conf=0.78)
Experimental — accuracy not yet measured - cites [144] De Martini, 2002, Experimental realization of the quantum universal not gate, Nature source
Probably not a substantial claim. The paper’s conclusions may not depend on it. It may state two separate claims as one.
PremisecitationBell-ports have been experimentally realized with fused optical fibers and more recently with passive and active integrated waveguide circuits.
“They have also been experimentally realized with fused optical fibers [138] and more recently with passive [141] and active integrated waveguide circuits [142].”
Quote in the paperNot a substantial claim3 of 3 sources checked- cites [138] Zhang, 2016, Engineering two-photon high-dimensional states through quantum interference, Sci. Adv. source
The citation [142] is attached to the claim about active integrated waveguide circuits. Materials and Methods (page unavailable) describes this paper’s experimental apparatus as a beamsplitter-and-mirrors filter with Dove prisms and spatial light modulators, rather than an integrated waveguide circuit. The paper therefore does not describe the realization attributed to it. (LLM, conf=0.84)
Checked by a reasoning model — may be wrong.
Experimental — accuracy not yet measured - cites [141] Navez, 2003, Cloning a real d-dimensional quantum state on the edge of the no-signaling condition, Phys. Rev. A source
The Introduction and Discussion and Conclusion address quantum cloning fidelity and no-signaling, not experimental Bell-port implementations. Searches for Bell-ports, fused optical fibers, and integrated waveguide circuits found no relevant passage in our copy. (LLM, conf=0.76)
Experimental — accuracy not yet measured - cites [142] Nagali, 2010, Experimental optimal cloning of four-dimensional quantum states of photons, Phys. Rev. Lett. source
The experimental-layout section describes single-mode fibers used to deliver and detect photons, and beam splitters used in a ququart-cloning experiment. It does not describe Bell-ports realized with fused optical fibers. Searches for “Bell-ports” and “fused optical fibers” found no passage addressing the realization attributed to this source; the waveguide-circuit claims carry separate citations. (LLM, conf=0.74)
Experimental — accuracy not yet measured
It may state two separate claims as one.
PremisecitationHigher Bell state discrimination success rates can be achieved with nonlinear optics, entanglement in auxiliary modes, or feed-forward techniques.
“Higher success rates can be achieved with nonlinear optics [73], entanglement in auxiliary modes [74,75], or feed-forward techniques [76].”
Quote in the paperNot a substantial claim3 of 4 sources checked- cites [73] Nagata, 2007, Beating the standard quantum limit with four-entangled photons, Science source
The paper’s discussion of the four-photon interferometer and its results (main text, Fig. 3; page not provided) concerns phase sensitivity, not Bell-state discrimination. Its discussion of distinguishing two four-photon input states (main text, Fig. 2, and Additional information; pages not provided) does not address whether auxiliary-mode entanglement improves Bell-state discrimination success rates. Searches for Bell-state discrimination, auxiliary modes, nonlinear optics, and feed-forward found no passage supporting the attributed point. (LLM, conf=0.76)
Experimental — accuracy not yet measured - cites [74] Afek, 2010, High-N00N states by mixing quantum and classical light, Science source
- cites [75] Zhou, 2017, Superresolving phase measurement with short-wavelength noon states by quantum frequency up-conversion, Phys. Rev. Appl. source
Only the nonlinear-optics portion of the citing sentence is attributed to this source [73]. The paper’s experimental passages describe sum-frequency up-conversion and NOON-state phase measurements, but do not address whether nonlinear optics increases Bell-state discrimination success rates. A Bell-state measurement appears in the References, not as a finding of this paper. (LLM, conf=0.76)
Experimental — accuracy not yet measured - cites [76] Kaltenbaek, 2006, Experimental interference of independent photons, Phys. Rev. Lett. source
The Abstract reports interference between photons from independent sources, and the experimental description reports interference visibility, not Bell-state discrimination success rates. Searches for nonlinear optics, auxiliary-mode entanglement, and feed-forward techniques found no passage in our copy linking them to higher discrimination success rates. (LLM, conf=0.76)
Experimental — accuracy not yet measured
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationFull device independent QKD allows security to be proven without any knowledge of the devices used in the implementation.
“One such solution is known as the full device independent QKD [95,96], where the security can be proven without any knowledge of the devices used in the implementation.”
Quote in the paperNot a substantial claim2 of 2 sources checked- cites [95] Lettow, 2010, Quantum interference of tunably indistinguishable photons from remote organic molecules, Phys. Rev. Lett. source
The paper’s Abstract describes an experiment on two-photon interference from remote organic molecules, not device-independent QKD. Searches for device-independent quantum key distribution, security without knowledge of devices, and related QKD terms found no passage addressing the claim. (LLM, conf=0.78)
Experimental — accuracy not yet measured - cites [96] Calsamiglia, 2001, Maximum efficiency of a linear-optical Bell-state analyzer, Appl. Phys. B source
The Introduction and Conclusions discuss photonic Bell-state measurements and the efficiency of a linear-optical analyzer, not QKD security. Searches for device-independent QKD and security without knowledge of implementation devices found no passage addressing that claim. (LLM, conf=0.76)
Experimental — accuracy not yet measured
It may state two separate claims as one.
PremisecitationQOCT was experimentally demonstrated, achieving an improvement in resolution by a factor of 5 compared to OCT.
“Not long after its proposal, QOCT was experimentally demonstrated, achieving an improvement in resolution by a factor of 5 compared to OCT [25].”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites [25] Kok, 2007, Linear optical quantum computing with photonic qubits, Rev. Mod. Phys. source
The Abstract and VI. OUTLOOK: BEYOND LINEAR OPTICS discuss experiments in linear optical quantum computing, not QOCT. Searches for QOCT, quantum optical coherence tomography, and the claimed fivefold resolution improvement found no passage in our copy addressing the claim; page numbers were unavailable. (LLM, conf=0.76)
Experimental — accuracy not yet measured
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationSuch bi-partite quantum walks can be used to perform quantum simulations.
“can be used to perform quantum simulations [159,160]”
Quote in the paperNot a substantial claim2 of 2 sources checked- cites [159] O’brien, 2009, Photonic quantum technologies, Nat. Photon. source
The Quantum information processing section (p. 2) discusses photonic quantum computing and optical networks, but not bipartite quantum walks or their use in quantum simulation. Searches for “quantum walks,” “bipartite quantum walk simulation,” and “quantum simulation” found no passage in our copy addressing that use. (LLM, conf=0.74)
Experimental — accuracy not yet measured - cites [160] Wang, 2020, Integrated photonic quantum technologies, Nat. Photon. source
It may state two separate claims as one.
PremisecitationSeveral specific quantum optical implementations rely on the HOM effect, including solving systems of linear equations, computation on encrypted data, computing discrete and fractional Fourier transform, and computations on a single spatial mode using temporal modes.
“There are several examples of specific quantum optical implementations that rely on the HOM effect, to list a few: solving systems of linear equations [128,129], computation on encrypted data [130], computing discrete and fractional Fourier transform [131], and computations on a single spatial mode (using temporal modes) [132].”
Quote in the paperNot a substantial claim4 of 4 sources checked- cites [128] Pirandola, 2015, High-rate measurement-device-independent quantum cryptography, Nat. Photon. source
The Discussion (p. 5) describes a continuous-variable quantum cryptography protocol, and the experimental setup (p. 16) describes optical modes combined for a Bell measurement. Searches for single-spatial-mode computation and temporal modes found no passage addressing that cited part of the sentence or its claimed reliance on the HOM effect. (LLM, conf=0.76)
Experimental — accuracy not yet measured - cites [129] Sasaki, 2014, Practical quantum key distribution protocol without monitoring signal disturbance, Nature source
The Abstract describes a quantum key distribution protocol using laser pulse trains, and the practical-implementation description in Additional information describes interference between delayed pulses. Neither passage addresses the HOM effect or computations on a single spatial mode using temporal modes. Searches for HOM-based computation, linear equations, encrypted data, and Fourier transforms found no supporting passage in our copy. (LLM, conf=0.76)
Experimental — accuracy not yet measured - cites [130] Takesue, 2015, Experimental quantum key distribution without monitoring signal disturbance, Nat. Photon. source
Citation [132] is attached to the example of computations on a single spatial mode using temporal modes. The experimental-setup passage describes temporally delayed interferometers for quantum key distribution, but does not address that computational implementation or its reliance on the HOM effect. Searches for single-spatial-mode computation and HOM-based temporal-mode computation found no supporting passage in our copy. (LLM, conf=0.75)
Experimental — accuracy not yet measured - cites [131] Wang, 2015, Experimental demonstration of a quantum key distribution without signal disturbance monitoring, Nat. Photon. source
The citation is attached to the claim about solving systems of linear equations. The paper’s discussion of its variable-delay interferometer for quantum key distribution does not address that computation or connect it to the HOM effect. Searches for linear equations and HOM interference found no supporting passage in our copy (page numbers unavailable). (LLM, conf=0.77)
Experimental — accuracy not yet measured
It may state two separate claims as one.
FindingcitationUpon exiting the beam splitter, the symmetric component Ψ+ of the input state results in two photons being detected in one of the output ports, while the antisymmetric component Ψ− results in one photon being detected in each output port.
“Upon exiting the beam splitter, the symmetric component, Ψ + i j , of the input state will reseult in two photons being detected in one of the output ports, while the antisymmetric component, Ψ - i j , will result in one photon being detected in each output port.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [111] Guan, 2015, Experimental passive round-robin differential phase-shift quantum key distribution, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
FindingreasoningWhen the two photons exit through the same port in this cloning scheme, 2/3 of the time they will have the same polarization state, and 1/3 of the time they will have orthogonal polarization states.
“When the two photons exit through the same port, 2/3 of the time they will have the same polarization state; while 1/3 of the time, they will have orthogonal polarization states, |1 s |1 s ⊥ .”
Quote in the paperSubstantial claimIt may state two separate claims as one.
FindingreasoningFor fermionic particles, the creation operators anti-commute, implying that ĉ† d† = -d† ĉ†, and fermions will exit through different output ports.
“In the case of fermionic particles, say electrons, the creation operators will anti-commute, implying that ĉ † d † = -d † ĉ † . Therefore, |1 a |1 b BS -→ |1 c |1 d and the fermions will exit through different output ports.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
FindingreasoningFor indistinguishable photons incident on a 50:50 BS, destructive interference occurs for two-photon states corresponding to photons exiting opposite output ports, and constructive interference occurs for photons exiting through the same output ports.
“In this case, we observe destructive interference of the two-photon states corresponding to photons exiting opposite output ports, and constructive interference of the two-photon states corresponding to photons exiting through the same output ports.”
Quote in the paperSubstantial claimIt may state two separate claims as one.
FindingreasoningFor the Bell states |Φ±_ab after a beam splitter, both photons end up in the same detector with the same polarization.
“in the last case they also reach the same detector, but they have the same polarizations”
Quote in the paperSubstantial claimIt may state two separate claims as one.
FindingreasoningFrom Eq. (17), the probability for passing the SWAP test is (1 + |⟨φ|ψ⟩|^2)/2, and the probability of failing is (1 - |⟨φ|ψ⟩|^2)/2.
“From Eq. ( 17), we can find the probability for passing the test is 1 + | φ| ψ | 2 /2, and consequently the probability of failing the test is 1 -| φ| ψ | 2 /2.”
Quote in the paperSubstantial claimProbably not a substantial claim. The paper may give no reason why it holds.
Interpretationnone givenTwo-photon interference has no classical analogue.
“two-photon interference has no classical analogue”
- Also stated in: § I. INTRODUCTION · boosted
“with absolutely no analogue in classical physics”
Quote in the paperNot a substantial claim- Also stated in: § I. INTRODUCTION · boosted
Probably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
Interpretationnone givenThe HOM effect is fundamental to a plethora of quantum information tasks.
“As will be discussed in the upcoming sections, the two-photon interference is fundamental to a plethora of quantum information tasks.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationThe MDI QKD protocol has been experimentally demonstrated using time-bin phase encoding and polarization encoding.
“The MDI QKD protocol has been experimentally demonstrated using time-bin phaseencoding [97], and polarization encoding [98].”
Quote in the paperNot a substantial claim0 of 2 sources checkedProbably not a substantial claim.
Premisenone givenQuantum state joining requires a particle to have enough degrees of freedom to accommodate the information of both incoming states.
“We thus require a particle to have enough degrees of freedom to accommodate the information of both incoming states.”
Quote in the paperSubstantial claimIt may state two separate claims as one.
PremisecitationThis quantum state joining process is probabilistic and requires an ancilla state, with a success probability of 1/32, or 1/8 if a suitable feed-forward is used.
“This process is probabilistic and requires an ancilla state, with a success probability of 1/32, or 1/8 if a suitable feed-forward is used.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [120] Gerhardt, 2011, Full-field implementation of a perfect eavesdropper on a quantum cryptography system, Nat. Commun. source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
InterpretationreasoningThe passive RRDPS QKD configuration typically yields larger security, better stability, and faster communications.
“As a result, such a configuration typically yields larger security, better stability, and faster communications.”
Quote in the paperSubstantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
Interpretationnone givenThe experimental realization of indistinguishable single photon sources with high purity is a crucial component for engineering large-scale entangled quantum states from independent sources.
“The experimental realization of indistinguishable single photon sources with high purity is a crucial component for engineering large-scale entangled quantum states from independent sources, as will be seen in forthcoming sections.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it. It may state two separate claims as one.
PremisecitationThe Heisenberg uncertainty principle and the no-cloning theorem are the basis of security when encoding information on single photons, because any type of eavesdropping results in disturbances of the photonic quantum states.
“The Heisenberg uncertainty principle and the no-cloning theorem [79] are the basis of security when encoding information on single photons, since any type of eavesdropping results in disturbances of the photonic quantum states.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [79] Flagg, 2010, Interference of single photons from two separate semiconductor quantum dots, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds. It may state two separate claims as one.
Premisenone givenThis quantum state joining scheme relies on the interaction of two photons, which would require nonlinear optics.
“This scheme relies on the interaction of two photons, which would require nonlinear optics.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationThe inverse process to joining states, quantum state splitting, splits the information on a ququart state onto two photonic qubits.
“The inverse process to joining states, known as quantum state splitting, is such that the information on a ququart state (for the above experiment) is split onto two photonic qubits [121].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [121] Mayers, 1998
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds. It may state two separate claims as one.
Premisenone givenMDI QKD still necessitates the assumptions that Alice's and Bob's state generation are perfect, which is still reasonable for current implementations.
“In contrast to the full device independent scheme, MDI QKD protocol still necessitates the assumptions of Alice's and Bob's states generation to be perfect, which is still reasonable for current implementations.”
Quote in the paperNot a substantial claimProbably not a substantial claim. It may be too vague to check against evidence. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
Interpretationnone givenThe measurement of HOM visibility is an invaluable diagnostic tool to characterize single photon sources and states.
“In particular, the measurement of the HOM visibility is an invaluable diagnostic tool to characterize single photon sources and states.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
Interpretationnone givenQOCT offers potential advantages in terms of resolution but new challenges appear, such as low signal and signal artifacts.
“Finally, although QOCT offers potential advantages in terms of resolution, new challenges appear, such as low signal and signal artifacts.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
InterpretationcitationIf the maximally mixed polarization state is created by using one photon from a maximally entangled singlet state, then 2/3 of the time the other photon in the singlet state will have the orthogonal polarization of the cloned states, and 1/3 of the time the same polarization, effectively implementing an optimal universal NOT gate.
“Suppose we created the maximally mixed polarization state by using one of the photons from a maximally entangled singlet state.Then 2/3 of the time, the other photon in the singlet state will have the orthogonal polarization of the cloned states, and 1/3 of the time the same polarization.This effectively implements an optimal universal NOT gate [118,119]-itself a non-unitary operation.”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [118] Zhao, 2008, Quantum hacking: experimental demonstration of time-shift attack against practical quantum-key-distribution systems, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
- cites [119] Lydersen, 2010, Hacking commercial quantum cryptography systems by tailored bright illumination, Nat. Photon. source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationQuantum entanglement is the fundamental resource in quantum communication, quantum metrology, and quantum computing.
“At the heart of quantum information is the notion of quantum entanglement [10]-the fundamental resource in quantum communication [11], quantum metrology [12], and quantum computing [13].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [10] Hamilton, 2000, Phase shifts in multilayer dielectric beam splitters, Am. J. Phys. source
- cites [11] Paul, 1986, Interference between independent photons, Rev. Mod. Phys. source
- cites [12] Ou, 1989, Fourth-order interference technique for determining the coherence time of a light beam, J. Opt. Soc. Am. B source
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationUniversal quantum computation can be achieved with linear optics, post-selection, single photon sources and detectors, and feed-forward, as proposed by the KLM protocol.
“Universal quantum computation can be achieved with linear optics, post-selection, single photon sources and detectors, and feed-forward, as was proposed by the KLM protocol [76].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [76] Kaltenbaek, 2006, Experimental interference of independent photons, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds. It may state two separate claims as one.
Premisenone givenTo achieve optimal HOM interference, attenuated lasers are phase randomized, achieving a maximum HOM visibility of 1/2.
“In order to achieve an optimal HOM interference, the attenuated lasers are phase randomized, achieving a maximum HOM visibility of 1/2.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
Premisenone givenThe CZ and CNOT gates are main components for universal quantum computation.
“Two such gates are the control-Z (CZ) and control-NOT (CNOT) gates, which are main components for universal quantum computation.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
Interpretationnone givenTwo-photon interference is one of the primary tools used in quantum information processing.
“In addition to being one of the most peculiar phenomenon in quantum optics, two-photon interference is one of the primary tools used in quantum information processing.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
InterpretationreasoningThe last two Bell states |Φ± cannot be distinguished from each other with a simple pair of photon detectors, giving a success rate of 50%.
“We cannot distinguish the last two states, |Φ ± , from each other with a simple pair of photon detectors; hence, the success rate of 50%.”
Quote in the paperSubstantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationEntanglement is a key physical principle at the heart of quantum communications.
“Another key physical principle that is at the heart of quantum communications is entanglement [10].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [10] Hamilton, 2000, Phase shifts in multilayer dielectric beam splitters, Am. J. Phys. source
Probably not a substantial claim. The paper may give no reason why it holds. It may state two separate claims as one.
Premisenone givenA beam splitter can be represented by a unitary transformation, thus conserving energy and preserving orthogonality between input states.
“Formally, it can be represented by a unitary transformation, thus conserving energy and preserving orthogonality between input states.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
Interpretationnone givenThe HOM effect is not limited to photons; it has implementations in non-photonic systems such as plasmons, phonons, atoms and electrons.
“Of course, the HOM effect is not limited to photons, and thus we close the review with implementations in non-photonic systems, such as plasmons, phonons, atoms and electrons.”
Quote in the paperNot a substantial claimProbably not a substantial claim. It may state two separate claims as one.
Interpretationnone givenTwo-photon interference and Bell state analysis are central concepts in MDI-QKD.
“The two-photon interference and Bell state analysis are central concepts in MDI-QKD.”
Quote in the paperSubstantial claimIt may state two separate claims as one.
PremisereasoningIn the passive RRDPS scheme, Bob generates a reference pulse train and sends Alice's and his state to a beam splitter, taking advantage of the phase stability of the two-photon interference effect.
“Instead of measuring the interference of a train of pulses at Bob's stage, Bob generates a reference pulse train, and sends Alice's and his state to a beam splitter.By using such a configuration, Bob takes advantage of the phase stability of the twophoton interference effect.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationBy arranging four beam splitters to interfere the original state with another entangled ancillary pair of modes first, and then sending each of the two pairs of output modes through a simple Bell state analyzer, one can distinguish one of the two previously indistinguishable states and raise the success rate to 75%.
“As outlined in [77], an example can be to arrange four beam splitters so that we interfere the original state with another entangled ancillary pair of modes first, and then each of the two pairs of output modes goes through a simple Bell state analyzer.In this way, we can distinguish one of the two states that we could not distinguish before, raising the success rate to 75%.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [77] Mosley, 2008, Heralded generation of ultrafast single photons in pure quantum states, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
Interpretationnone givenA heralded single photon source achieving unity HOM visibility would lead to a higher secret key rate per transmitted photon.
“A heralded single photon source achieving a unity HOM visibility would lead to a higher secret key rate per transmitted photon.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationNew techniques are being investigated to exploit the full potential of QOCT.
“Thus, new techniques are being investigated in order to exploit the full potential of QOCT [29][30][31][32].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [29] Slussarenko, 2017, Unconditional violation of the shot-noise limit in photonic quantum metrology, Nat. Photon. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [30] D’Ambrosio, 2019, Tunable two-photon quantum interference of structured light, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [31] Hiekkamäki, 2020, Single-path two-photon interference effects between spatial modes source
It may state two separate claims as one.
PremisecitationTwo-photon interference has inherent dispersion cancellation, which does not occur in one-photon interference or classical light interference.
“Another particularity of the two-photon interference is its inherent dispersion cancellation, which does not occur in the case of the one-photon interference, or the interference of classical light.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [22] Einstein, 1935, Can quantum-mechanical description of physical reality be considered complete?, Phys. Rev. source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper may give no reason why it holds. It may state two separate claims as one.
InterpretationreasoningTwo-photon interference gives a distinct advantage to outperform classical computations, securely communicate information, simulate highly complex physical systems and increase the sensitivity of precise measurements.
“It is precisely this separation from classical to quantum physics that gives two-photon interference a distinct advantage to outperform classical computations, securely communicate information, simulate highly complex physical systems and increase the sensitivity of precise measurements.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationThe RRDPS protocol removes the requirement for signal disturbance monitoring by bounding the amount of information leaked to the eavesdropper, with the bound depending entirely on Alice's generation stage.
“The RRDPS protocol removes the requirement for signal disturbance monitoring by bounding the amount of information leaked to the eavesdropper, where the bound depends entirely on Alice's generation stage.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [102] Gisin, 2002, Quantum cryptography, Rev. Mod. Phys. source
It may state two separate claims as one.
PremisereasoningFull device independent QKD yields very low secret key rates and is highly impractical due to stringent requirements such as near unity detection efficiencies.
“However, this scheme yields very low secret key rates, and is highly impractical due to several stringent requirements such as near unity detection efficiencies.”
Quote in the paperNot a substantial claimProbably not a substantial claim. It may be too vague to check against evidence. The paper’s conclusions may not depend on it.
InterpretationreasoningThe HOM effect might play an important role in the engineering and analysis of entangled states.
“Quantum entanglement inherently deals with the interference of two-photon states, thus hinting to the fact that the HOM effect might play an important role in the engineering and analysis of entangled states.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationMany quantum communication schemes, such as entanglement swapping, quantum teleportation, and dense-coding, are based on the concept of entanglement.
“Beyond quantum cryptography, many quantum communication schemes-such as entanglement swapping [81], quantum teleportation [82], and dense-coding [83]-are also based on the concept of entanglement.”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [81] Wei, 2014, Deterministic and robust generation of single photons from a single quantum dot with 99.5% indistinguishability using adiabatic rapid passage, Nano Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [82] Senellart, 2017, High-performance semiconductor quantum-dot single-photon sources, Nat. Nanotechnol. source
- cites [83] Felinto, 2006, Conditional control of the quantum states of remote atomic memories for quantum networking, Nat. Phys. source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
PremisecitationThe two-way architecture for quantum repeaters works by having quantum memories evenly distributed along a communication channel, each memory hosting two atoms that emit photons forwards and backwards, with a Bell state analyzer midway between two memories measuring the two photons in the Bell basis.
“the so-called “two-way architecture” works by having quantum memories evenly distributed along a communication channel, each memory hosting two atoms that emit photons as described above, one forwards and one backwards along the channel.Mid-way between two memories M 1 M 2 sits a Bell state analyzer that measures the two photons coming from M 1 and M 2 in the Bell basis.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [89] Sipahigil, 2012, Quantum interference of single photons from remote nitrogen-vacancy centers in diamond, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
InterpretationcitationThe entangled state of two atoms created by this procedure will display non-local correlations, verifiable by violating Bell's inequalities.
“We have thus created an entangled state of two atoms, which will display non-local correlations as one can verify for example by violating Bell's inequalities [87].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [87] Chen, 2008, Memory-built-in quantum teleportation with photonic and atomic qubits, Nat. Phys. source
It may state two separate claims as one.
PremisereasoningThe issue of random detection time difference in entangling photons with different frequencies can be solved either by postselecting on measurements within a very narrow time window, or by recording the time difference and feed-forwarding a phase correction so that every single photon pair will have the same phase.
“However, one can solve this issue either by postselecting on only the measurements that fall within a very narrow time window (but this reduces the total number of successful measurements), or by recording the time difference and feed-forward a phase correction so that every single photon pair will have the same phase.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationBunching and anti-bunching are typical bosonic and fermionic behaviours, respectively.
“Interestingly, bunching and anti-bunching are typical bosonic and fermionic behaviours, respectively.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [14] Kim, 2014, Two-photon interference with continuous-wave multi-mode coherent light, Opt. Express source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
PremisecitationThe frequency difference ∆ω between photons from different-frequency pairs generates a phase exp(i∆ω∆t) between the components, which will render the state mixed if unaccounted for because the detection time difference ∆t is random.
“The frequency difference ∆ω generates a phase of exp(i∆ω∆t) between the components, which will render the state mixed if unaccounted for because the detection time difference ∆t is random.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [112] Hofmann, 2012, Heralded entanglement between widely separated atoms, Science source
It may state two separate claims as one.
PremisecitationThe MDI scheme has been demonstrated over long distances through optical fibres, showing feasibility and potential for unconditional security.
“Moreover, the MDI scheme has also been demonstrated over long distances through optical fibres [99,100], showing the feasibility of the protocol and its potential for unconditional security.”
Quote in the paperNot a substantial claim0 of 2 sources checkedProbably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
Interpretationnone givenBell state measurements are the gold standard for experimentally measuring maximally entangled states.
“Furthermore, Bell state measurements are the gold standard for experimentally measuring maximally entangled states.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
Interpretationnone givenIn all boson sampling tasks, multi-photon as well as multimodal interferences play a crucial role.
“in all boson sampling tasks, multi-photon as well as multimodal interferences, i.e. generalizations of the original HOM idea, play a crucial role.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationA probability surface or coincidence landscape is useful to probe indistinguishability or to predict the complex device's quantum behaviour.
“which is useful to probe indistinguishability or to predict the complex device's quantum behaviour [163].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [163] Reck, 1994, Experimental realization of any discrete unitary operator, Phys. Rev. Lett. source
It may state two separate claims as one.
PremisereasoningFor the two-dimensional case, a Bell state measurement can be implemented with a single beamsplitter followed by a detector in each output port, which is equivalent to a destructive SWAP test in the sense that the states get measured and are not available afterwards.
“For the two-dimensional case, we can implement a Bell state measurement with a single beamsplitter followed by a detector in each output port, which is equivalent to a destructive SWAP test in the sense that the states get measured and are not available afterwards.”
Quote in the paperSubstantial claimIt may state two separate claims as one.
PremisecitationIn the 4He BEC experiment, the cross-correlation measurements showed a clear dip with visibility 0.65±0.07, above the classical limit of 0.5.
“the results show a clear dip in the cross-correlation measurements with a visibility of 0.65±0.07,which is above the classical limit of 0.5”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [193] Tichy, 2013, Limits to multipartite entanglement generation with bosons and fermions, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationIn plasmonic systems, usually deleterious losses might be turned into an advantageous feature when the nanostructures are carefully tuned.
“it was shown that the usually deleterious losses associated with plasmonic systems might be turned into a advantageous feature when the nanostructures are carefully tuned.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [187] Crespi, 2013, Anderson localization of entangled photons in an integrated quantum walk, Nat. Photon. source
Probably not a substantial claim. The paper’s conclusions may not depend on it.
InterpretationreasoningBecause the initial findings used a continuous stream of electrons, the interference might not exclusively be interpreted as a result from the overlap between two single-electron wave packets.
“because these initial findings used a continuous stream of electrons, the interference might not exclusively be interpreted as a result from the overlap between two single-electron wave packets.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationDue to anti-bunching, a reduction in the noise properties of the output ports was observed, providing an indirect verification of two-electron antibunching.
“Due to anti-bunching, a reduction in the noise properties of the output ports was observed; thus, an indirect verification of two-electron antibunching was achieved.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [196] Broome, 2013, Photonic boson sampling in a tunable circuit, Science source
- Rests on an assumption: Fermions obey Fermi statistics, which leads to anti-bunching at a beam splitter.
Probably not a substantial claim. The paper’s conclusions may not depend on it. It may state two separate claims as one.
Premisenone givenThe HOM effect is colloquially referred to as a test for the distinguishability between two photons: if we witness a coincidence, the two photons had different states.
“The Hong-Ou-Mandel effect is colloquially referred to as a test for the distinguishability between two photons: if we witness a coincidence, the two photons had different states.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
InterpretationreasoningThe CZ gate heavily relies on the HOM effect, with the output depending on whether the control and target photons bunched or not.
“Overall, we see that the CZ gate heavily relies on the HOM effect, the output depending on whether the control and target photons bunched or not.”
Quote in the paperSubstantial claimProbably not a substantial claim.
InterpretationreasoningThe phonon experiment opens the path to phonon quantum information experiments relying on phononic HOM interference.
“the experiment opens the path to phonon quantum information experiments, such as boson sampling or entanglement generation in larger ion crystals, relying on a phononic HOM interference.”
Quote in the paperSubstantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationSuch bi-partite quantum walks give rise to interesting quantum correlation patterns.
“that gives rise to interesting quantum correlation patterns [157,158]”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [157] Weimann, 2016, Implementation of quantum and classical discrete fractional fourier transforms, Nat. Commun. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [158] Humphreys, 2013, Linear optical quantum computing in a single spatial mode, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
PremisecitationThe observed plasmonic HOM dip had a visibility of 0.43±0.02, below the classical limit of 0.5.
“Although the observed dip had only a visibility of 0.43±0.02(see Fig. 8b) and thus below the classical limit of 0.5”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [180] Lahini, 2012, Quantum walk of two interacting bosons, Phys. Rev. A source
It may state two separate claims as one.
InterpretationcitationBy making the photons pairwise distinguishable, e.g. by delaying independently two photons, one can map a probability surface with non-trivial features, which can be seen as the three-dimensional extension to the 2-dimensional HOM interference dip.
“By making the photons pairwise distinguishable, e.g. by delaying independently two photons, one can map a probability surface with non-trivial features (see Fig. 7b).This surface can be seen as the three-dimensional extension to the 2-dimensional HOM interference dip [141].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [141] Navez, 2003, Cloning a real d-dimensional quantum state on the edge of the no-signaling condition, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationThe complex features of three-partite interference experiments were also discussed in terms of quantum metrology and phase sensing to enhance precision.
“Importantly, the complex features of three-partite interference experiments were also discussed in terms of quantum metrology and phase sensing to enhance precision [145].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [145] Ricci, 2004, Teleportation scheme implementing the universal optical quantum cloning machine and the universal not gate, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
PremisecitationAt the plasmonic beam splitter, anti-coalescence or non-linear absorption can be observed.
“At the plasmonics beam splitter, anti-coalescence or non-linear absorption can be observed [187].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [187] Crespi, 2013, Anderson localization of entangled photons in an integrated quantum walk, Nat. Photon. source
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationSuch bi-partite quantum walks can probe the statistics in quantum walks.
“or can probe the statistics in quantum walks [161].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [161] Garcia-Escartin, 2013, Swap test and Hong–Ou–Mandel effect are equivalent, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
PremisereasoningFor two maximally distinguishable (orthogonal) states, the overlap is 0 and the pass probability is 1/2, while for maximally indistinguishable states the overlap is 1 and the probability to pass the test is also 1.
“For two maximally distinguishable (orthogonal) states, the overlap is 0 and P = 1/2, while for maximally indistinguishable states the overlap is 1 and the probability to pass the test is also 1.”
Quote in the paperSubstantial claimIt may state two separate claims as one.
InterpretationreasoningTwo-plasmon HOM interference is well-established and can be considered one of the building blocks of future quantum plasmonic circuits.
“Since two plasmon HOM interference is now well-established, it can be considered one of the building blocks of future quantum plasmonic circuits”
Quote in the paperSubstantial claimIt may state two separate claims as one.
PremisecitationThe triad phase is the sum of the three relative phases between pairwise inputs and only affects the outcome if the photons are partially distinguishable.
“This so-called triad phase is the sum of the three relative phases between pairwise inputs (see Fig. 7c) and only effects the outcome if the photons are partially distinguishable.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [144] De Martini, 2002, Experimental realization of the quantum universal not gate, Nature source
Probably not a substantial claim. The paper may give no reason why it holds.
Premisenone givenIn higher dimensions, one needs the equivalent circuit for projecting onto the symmetric/antisymmetric subspaces.
“In higher dimensions, one needs the equivalent circuit for projecting onto the symmetric/antisymmetric subspaces.”
Quote in the paperNot a substantial claimProbably not a substantial claim.
Premisenone givenThe SWAP test is a quantum computing primitive operation that tests for the inequality between two quantum states.
“Similarly, the SWAP test is a quantum computing primitive operation that tests for the inequality between two quantum states.”
Quote in the paperSubstantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationBell-ports have been discussed theoretically for many years in connection to multipartite and high-dimensional quantum information.
“Bell-ports have been discussed theoretically since many years in connection to multipartite and high-dimensional quantum information [137,139,140].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [137] Jamiolkowski, 1972, Linear transformations which preserve trace and positive semidefiniteness of operators, Rep. Math. Phys. source
- cites [139] Zhao, 2014, Entangling different-color photons via time-resolved measurement and active feed forward, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [140] Peres, 2003, How the no-cloning theorem got its name, Fortschr. Phys. source
Checked before — its earlier verdict is held back until a new check runs.
It may state two separate claims as one.
PremisereasoningIn the SWAP test, if the outcome is |'1', the two input states are different; if the outcome is |'0', they may or may not be equal.
“In terms of the measurement outcome, if |'1' is measured, we can confirm that the two input states are different; however, if the outcome is the state |'0' , they may or may not be equal.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationVariations of the NS gate have been reported: one proposal using only two beam splitters but with a slightly lower success probability of (3 - √2)/7; other schemes with two ancillary photons with success probabilities 1/5 and 1/4.
“Variations of the NS gate have been reported: one proposal shows the possibility to implement it using only two BS but with slightly lower success probability of (3 -√ 2)/7 [123]; other schemes with again two ancillary photons with success probabilities 1/5 [124] and 1/4 [125].”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites [123] Liu, 2013, Experimental measurement-device-independent quantum key distribution, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [124] Tang, 2014, Experimental demonstration of polarization encoding measurement-device-independent quantum key distribution, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [125] Tang, 2014, Measurement-device-independent quantum key distribution over 200 km, Phys. Rev. Lett. source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it. It may state two separate claims as one.
PremisecitationWaveguides in photonics chips allow for higher portability, higher cost efficiency, and higher robustness.
“Waveguides in photonics chips allow for higher portability, higher cost efficiency, and higher robustness [133,134].”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites [133] Yin, 2018, Improved security bound for the round-robin-differential-phase-shift quantum key distribution, Nat. Commun. source
Checked before — its earlier verdict is held back until a new check runs.
- cites [134] Bouchard, 2018, Round-robin differential-phase-shift quantum key distribution with twisted photons, Phys. Rev. A source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisereasoningBoson sampling challenges the extended Church-Turing thesis.
“In addition, it is also suggested that this challenges a fundamental principle of computer science, namely the extended Church-Turing thesis.”
Quote in the paperNot a substantial claim0 of 2 sources checkedProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationIf more than two photons are interfered, a probability surface or coincidence landscape can be investigated.
“if more than two photons are interfered, a probability surface or coincidence landscape can be investigated [162]”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [162] Zeilinger, 1993, Einstein–Podolsky–Rosen correlations in higher dimensions
Probably not a substantial claim. The paper’s conclusions may not depend on it.
PremisereasoningBoson sampling is considered a promising candidate to show quantum supremacy.
“and as such it is considered to be a promising candidate to show quantum supremacy.”
Quote in the paperNot a substantial claim0 of 2 sources checkedProbably not a substantial claim. The paper’s conclusions may not depend on it.
PremisecitationWhen two particles are sent into a multiport, the transmission can be described as a complex bi-partite quantum walk.
“When two particles for example are sent into a multiport, e.g.multimode waveguide [153,154], multimode fiber [155] or integrated waveguide structures [156], the transmission can be described as a complex bi-partite quantum walk”
Quote in the paperNot a substantial claim0 of 4 sources checked- cites [153] Okamoto, 2011, Realization of a Knill–Laflamme–Milburn controlled-not photonic quantum circuit combining effective optical nonlinearities, Proc. Natl Acad. Sci. source
- cites [154] Harrow, 2009, Quantum algorithm for linear systems of equations, Phys. Rev. Lett. source
- cites [155] Cai, 2013, Experimental quantum computing to solve systems of linear equations, Phys. Rev. Lett. source
- cites [156] Fisher, 2014, Quantum computing on encrypted data, Nat. Commun. source
Checked before — its earlier verdict is held back until a new check runs.
Probably not a substantial claim. The paper may give no reason why it holds. It may state two separate claims as one.
Premisenone givenThe eigenstates of the SWAP operator are the Bell states: three Bell states correspond to eigenvalue +1 (the symmetric subspace), and one corresponds to eigenvalue -1 (the singlet state, i.e. the antisymmetric subspace).
“The eigenstates of the SWAP operator are the Bell states: three Bell states correspond to the eigenvalue +1 (the symmetric subspace), and one corresponds to the eigenvalue -1 (the singlet state, i.e. the antisymmetric subspace).”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationThe triad phase leads to a change in detection probabilities when all three photons are detected in separate output ports and does not affect bi-photon transmission probabilities.
“It leads to a change in the detection probabilities when all three photons are detected in separate output ports and does not affect the bi-photon transmission probabilities.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [144] De Martini, 2002, Experimental realization of the quantum universal not gate, Nature source
It may state two separate claims as one.
PremisecitationLevitons have been observed and brought to two-fermionic quantum interference only recently.
“they have been observed and even brought to twofermionic quantum interference only recently [201].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites [201] Bentivegna, 2015, Experimental scattershot boson sampling, Sci. Adv. source
Probably not a substantial claim. The paper may give no reason why it holds.
Premisenone givenIn quantum computation, the interaction between two photons is often required to create building blocks of certain quantum gates, e.g. CNOT and CZ gates.
“In quantum computation, the interaction between two photons is often required to create the building blocks of certain quantum gates, for example CNOT and CZ gates.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper may give no reason why it holds.
Premisenone givenTwo-photon interference enables the measurement of maximally entangled states through Bell state measurements.
“two-photon interference enables the measurement of maximally entangled states through Bell states measurements, or equivalently, the projection onto the Bell basis.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper may give no reason why it holds.
Interpretationnone givenTwo-photon interference has no classical counterpart.
“Two-photon interference is fundamentally interesting because it has no classical counterpart”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper may give no reason why it holds. It may state two separate claims as one.
Interpretationnone givenIn quantum communication, two-photon interference can be used to circumvent the problem of untrusted measurement devices and build novel protocols.
“In quantum communication, it can be used to circumvent the problem of untrusted measurement devices, and build novel protocols.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper may give no reason why it holds.
Interpretationnone givenIn quantum state analysis, two-photon interference gives the possibility to distinguish between modes, since only indistinguishable states will bunch.
“In quantum state analysis, it gives the possibility to distinguish between modes, since only indistinguishable states will bunch.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
InterpretationreasoningTwo-photon interference has many applications ranging from precision measurement and state determination to quantum computations and quantum communication.
“with many applications ranging from precision measurement and state determination to quantum computations and quantum communication.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper may give no reason why it holds. It may state two separate claims as one.
Premisenone givenIn metrology, two-photon interference allows for femtosecond and even attosecond time-resolution, state determination, and generating non-classical light for resolution enhancement with linear optics.
“In metrology, two photon interference allows for femtosecond and even attosecond time-resolution, state determination (quantum state analysis), and generating non-classical light for resolution enhancement with linear optics.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper may give no reason why it holds. It may state two separate claims as one.
InterpretationreasoningTwo-photon interference acts as the linear optical solution to this challenge and provides a scalable technique to build photonic quantum computers.
“Two-photon interference acts as the linear optical solution to this challenge, and thus provides a scalable technique to build photonic quantum computers.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it. It may state two separate claims as one.
Interpretationnone givenTwo-particle interferences is the basis for most optical quantum information science and a powerful tool for metrology and other fields.
“Two particle interferences is not only the basis for most of optical quantum information science and a powerful tool for metrology and other fields”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds. It may state two separate claims as one.
Premisenone givenBell state measurements are central to teleportation and entanglement swapping.
“Bell state measurements are central to the concepts of teleportation and entanglement swapping.”
Quote in the paperNot a substantial claim
The paper relies on this without support.
Fermions obey Fermi statistics, which leads to anti-bunching at a beam splitter.
“The major difference between indistinguishable bosons and fermions is that the latter obey Fermi statistics, which leads to anti-bunching at a beam splitter.”
The paper relies on this without support.
SPPs, being bosonic quasiparticles, are expected to bunch in a HOM-type experiment.
“Because SPPs are described as quasiparticles with a bosonic nature, they were also expected to bunch in a HOM-type experiment.”
The paper relies on this without support.
Phonons follow Bose-Einstein statistics and are expected to bunch in a HOM-like arrangement.
“Phonons also follow Bose-Einstein statistics, and as such they are expected to bunch in a HOM-like arrangement.”
The paper relies on this without support.
Even massive particles should be able to exhibit two-particle interferences following quantum mechanics.
“following quantum mechanics, even massive particles should be able to exhibit two-particle interferences.”
Self-check
Percentages, sums and reported differences re-computed from the paper’s own numbers.
Each contradiction between two passages listed here was confirmed by an independent check.
The state-joining expansion swaps its two cross terms
MinorExpanding the tensor product gives αδ for a horizontally polarized photon in mode I and a vertically polarized photon in mode II, and βγ for the reverse. The displayed expansion assigns those coefficients the other way around.
“|φ I ⊗ |ψ II = (α |1 I,H + β |1 I,V ) ⊗ (γ |1 II,H + δ |1 II,V )”
“= αγ |1 H , 1 H + βγ |1 H , 1 V +αδ |1 V , 1 H + βδ |1 V , 1 V ,”
The two-photon N00N state is attributed to the wrong equation
MinorThe paper says the N = 2 N00N state is the state in Eq. (5), but Eq. (5) defines polarization Bell states with one photon in each input path. The two-photon path N00N state produced by the beam splitter is instead displayed in Eq. (4).
“For the case of N = 2 [36,37], we recognize the state from Eq. ( 5) where two indistinguishable photons are made incident onto both input ports of a 50:50 BS, resulting in HOM interference.”
“|Ψ ± ab = 1 √ 2 (|H a |V b ± |V a |H b ) (5”
Citations
Cites
Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?
Einstein, A., Podolsky, B., & Rosen, N. (1935) · Physical Review · doi:10.1103/physrev.47.777 · Cited by 16,654
Teleporting an unknown quantum state via dual classical and Einstein-Podolsky-Rosen channels
Bennett, C. H., Brassard, G., Crépeau, C., Jozsa, R., Peres, A., & Wootters, W. K. (1993) · Physical Review Letters · doi:10.1103/physrevlett.70.1895 · Cited by 13,703 · cited 1×
“Beyond quantum cryptography, many quantum communication schemes—such as entanglement swapping [106], quantum teleportation [107], and dense-coding [108]—are also based on the concept of entanglement.”
BackgroundOn the Einstein Podolsky Rosen paradox
Bell, J. S. (1964) · Physics Physique Fizika · doi:10.1103/physicsphysiquefizika.1.195 · Cited by 12,252
Quantum cryptography based on Bell’s theorem
Ekert, A. K. (1991) · Physical Review Letters · doi:10.1103/physrevlett.67.661 · Cited by 10,777
Gisin, N., Ribordy, G., Tittel, W., & Zbinden, H. (2002) · Reviews of Modern Physics · doi:10.1103/revmodphys.74.145 · Cited by 8,515
A scheme for efficient quantum computation with linear optics
Knill, E., Laflamme, R., & Milburn, G. J. (2001) · Nature · doi:10.1038/35051009 · Cited by 5,880
Communication via one- and two-particle operators on Einstein-Podolsky-Rosen states
Bennett, C. H., & Wiesner, S. J. (1992) · Physical Review Letters · doi:10.1103/physrevlett.69.2881 · Cited by 5,470
A single quantum cannot be cloned
Wootters, W. K., & Zurek, W. H. (1982) · Nature · doi:10.1038/299802a0 · Cited by 5,406 · cited 2×
“Considering the well-known fact that quantum mechanics does not allow the possibility to clone an unknown state [104, 140], the ability to perform quantum cloning may seem counterintuitive.”
BackgroundMeasurement of subpicosecond time intervals between two photons by interference
Hong, C. K., Ou, Z. Y., & Mandel, L. (1987) · Physical Review Letters · doi:10.1103/physrevlett.59.2044 · Cited by 4,369
Giovannetti, V., Lloyd, S., & Maccone, L. (2011) · Nature Photonics · doi:10.1038/nphoton.2011.35 · Cited by 3,894
Quantum Repeaters: The Role of Imperfect Local Operations in Quantum Communication
Briegel, H.-J., Dür, W., Cirac, J. I., & Zoller, P. (1998) · Physical Review Letters · doi:10.1103/physrevlett.81.5932 · Cited by 3,481
Quantum Algorithm for Linear Systems of Equations
Harrow, A. W., Hassidim, A., & Lloyd, S. (2009) · Physical Review Letters · doi:10.1103/physrevlett.103.150502 · Cited by 3,325
Simple Proof of Security of the BB84 Quantum Key Distribution Protocol
Shor, P. W., & Preskill, J. (2000) · Physical Review Letters · doi:10.1103/physrevlett.85.441 · Cited by 3,047
Linear optical quantum computing with photonic qubits
Kok, P., Munro, W. J., Nemoto, K., Ralph, T. C., Dowling, J. P., & Milburn, G. J. (2007) · Reviews of Modern Physics · doi:10.1103/revmodphys.79.135 · Cited by 2,904
Completely positive linear maps on complex matrices
Choi, M.-D. (1975) · Linear Algebra and its Applications · doi:10.1016/0024-3795(75)90075-0 · Cited by 2,659 · cited 1×
“Furthermore, in light of the Choi–Jamiołkowski isomorphism which allows us to associate a bipartite state to a quantum channel [136, 137], generating the desired quantum states also has consequences on our ability to implement full quantum channels through the technique of gate teleportation.”
BackgroundO'Brien, J. L., Furusawa, A., & Vučković, J. (2009) · Nature Photonics · doi:10.1038/nphoton.2009.229 · Cited by 2,388
Measurement-Device-Independent Quantum Key Distribution
Lo, H., Curty, M., & Qi, B. (2012) · Physical Review Letters · doi:10.1103/physrevlett.108.130503 · Cited by 2,313
Experimental realization of any discrete unitary operator
Reck, M., Zeilinger, A., Bernstein, H. J., & Bertani, P. (1994) · Physical Review Letters · doi:10.1103/physrevlett.73.58 · Cited by 2,155
Decoy state quantum key distribution
Lo, H.-K., Ma, X., & Chen, K. (2005) · Physical Review Letters · doi:10.1103/physrevlett.94.230504 · Cited by 2,138
‘‘Event-ready-detectors’’ Bell experiment via entanglement swapping
Żukowski, M., Zeilinger, A., Horne, M. A., & Ekert, A. K. (1993) · Physical Review Letters · doi:10.1103/physrevlett.71.4287 · Cited by 2,045
Advances in quantum cryptography
Pirandola, S., Andersen, U. L., Banchi, L., Berta, M., Bunandar, D., Colbeck, R., Englund, D., Gehring, T., Lupo, C., Ottaviani, C., et al. (2020) · Advances in Optics and Photonics · doi:10.1364/aop.361502 · Cited by 2,033
Quantum repeaters based on atomic ensembles and linear optics
Sangouard, N., Simon, C., de Riedmatten, H., & Gisin, N. (2011) · Reviews of Modern Physics · doi:10.1103/revmodphys.83.33 · Cited by 1,888
Integrated photonic quantum technologies
Wang, J., Sciarrino, F., Laing, A., & Thompson, M. G. (2020) · Nature Photonics · doi:10.1038/s41566-019-0532-1 · Cited by 1,576
Self-citationTame, M. S., McEnery, K. R., Özdemir, Ş. K., Lee, J., Maier, S. A., & Kim, M. S. (2013) · Nature Physics · doi:10.1038/nphys2615 · Cited by 1,573
Device-independent security of quantum cryptography against collective attacks
Acín, A., Brunner, N., Gisin, N., Massar, S., Pironio, S., & Scarani, V. (2007) · Physical Review Letters · doi:10.1103/physrevlett.98.230501 · Cited by 1,537
Linear transformations which preserve trace and positive semidefiniteness of operators
Jamiołkowski, A. (1972) · Reports on Mathematical Physics · doi:10.1016/0034-4877(72)90011-0 · Cited by 1,512
Quantum Interferometric Optical Lithography: Exploiting Entanglement to Beat the Diffraction Limit
Boto, A. N., Kok, P., Abrams, D. S., Braunstein, S. L., Williams, C. P., & Dowling, J. P. (2000) · Physical Review Letters · doi:10.1103/physrevlett.85.2733 · Cited by 1,494
Rubinsztein-Dunlop, H. H., Forbes, A., Berry, M., Dennis, M. R., Andrews, D. L., Mansuripur, M., Denz, C., Alpmann, C., Banzer, P., Bauer, T. A., et al. (2016) · Journal of Optics · doi:10.1088/2040-8978/19/1/013001 · Cited by 1,349
Self-citationHigh-performance semiconductor quantum-dot single-photon sources
Senellart, P., Solomon, G., & White, A. (2017) · Nature Nanotechnology · doi:10.1038/nnano.2017.218 · Cited by 1,237
Hacking commercial quantum cryptography systems by tailored bright illumination
Lydersen, L., Wiechers, C., Wittmann, C., Elser, D., Skaar, J., & Makarov, V. (2010) · Nature Photonics · doi:10.1038/nphoton.2010.214 · Cited by 1,005
Electron counting statistics and coherent states of electric current
Levitov, L. S., Lee, H., & Lesovik, G. B. (1996) · Journal of Mathematical Physics · doi:10.1063/1.531672 · Cited by 949
Quantum Walks of Correlated Photons
Peruzzo, A., Lobino, M., Matthews, J. C. F., Matsuda, N., Politi, A., Poulios, K., Zhou, X.-Q., Lahini, Y., Ismail, N., Wörhoff, K., et al. (2010) · Science · doi:10.1126/science.1193515 · Cited by 929 · cited 2×
“[157] Peruzzo, A.”
Shih, Y. H., & Alley, C. O. (1988) · Physical Review Letters · doi:10.1103/physrevlett.61.2921 · Cited by 917
Quantum optical metrology – the lowdown on high-N00N states
Dowling, J. P. (2008) · Contemporary Physics · doi:10.1080/00107510802091298 · Cited by 894
The computational complexity of linear optics
Aaronson, S., & Arkhipov, A. (2011) · Proceedings of the forty-third annual ACM symposium on Theory of computing · doi:10.1145/1993636.1993682 · Cited by 874
Beating the channel capacity limit for linear photonic superdense coding
Barreiro, J. T., Wei, T.-C., & Kwiat, P. G. (2008) · Nature Physics · doi:10.1038/nphys919 · Cited by 870
Boson Sampling on a Photonic Chip
Spring, J. B., Metcalf, B. J., Humphreys, P. C., Kolthammer, W. S., Jin, X.-M., Barbieri, M., Datta, A., Thomas-Peter, N., Langford, N. K., Kundys, D., et al. (2013) · Science · doi:10.1126/science.1231692 · Cited by 837
Measurement-Device-Independent Quantum Key Distribution Over a 404 km Optical Fiber
Yin, H.-L., Chen, T.-Y., Yu, Z.-W., Liu, H., You, L.-X., Zhou, Y.-H., Chen, S.-J., Mao, Y., Huang, M.-Q., Zhang, W.-J., et al. (2016) · Physical Review Letters · doi:10.1103/physrevlett.117.190501 · Cited by 836
Super-resolving phase measurements with a multiphoton entangled state
Mitchell, M. W., Lundeen, J. S., & Steinberg, A. M. (2004) · Nature · doi:10.1038/nature02493 · Cited by 830
Beating the Standard Quantum Limit with Four-Entangled Photons
Nagata, T., Okamoto, R., O'Brien, J. L., Sasaki, K., & Takeuchi, S. (2007) · Science · doi:10.1126/science.1138007 · Cited by 735
Tillmann, M., Dakić, B., Heilmann, R., Nolte, S., Szameit, A., & Walther, P. (2013) · Nature Photonics · doi:10.1038/nphoton.2013.102 · Cited by 709
Integrated multimode interferometers with arbitrary designs for photonic boson sampling
Crespi, A., Osellame, R., Ramponi, R., Brod, D. J., Galvão, E. F., Spagnolo, N., Vitelli, C., Maiorino, E., Mataloni, P., & Sciarrino, F. (2013) · Nature Photonics · doi:10.1038/nphoton.2013.112 · Cited by 662
Self-citationTwo-Photon Diffraction and Quantum Lithography
D’Angelo, M., Chekhova, M. V., & Shih, Y. H. (2001) · Physical Review Letters · doi:10.1103/physrevlett.87.013602 · Cited by 661
Quantum Teleportation of a Polarization State with a Complete Bell State Measurement
Kim, Y.-H., Kulik, S. P., & Shih, Y. (2001) · Physical Review Letters · doi:10.1103/physrevlett.86.1370 · Cited by 660
Side-Channel-Free Quantum Key Distribution
Braunstein, S. L., & Pirandola, S. (2012) · Physical Review Letters · doi:10.1103/physrevlett.108.130502 · Cited by 655
Photonic Boson Sampling in a Tunable Circuit
Broome, M. A., Fedrizzi, A., Rahimi-Keshari, S., Dove, J., Aaronson, S., Ralph, T. C., & White, A. G. (2013) · Science · doi:10.1126/science.1231440 · Cited by 634
Heralded generation of ultrafast single photons in pure quantum states
Mosley, P. J., Lundeen, J. S., Smith, B. J., Wasylczyk, P., U’Ren, A. B., Silberhorn, C., & Walmsley, I. A. (2008) · Physical Review Letters · doi:10.1103/physrevlett.100.133601 · Cited by 593
High-NOON States by Mixing Quantum and Classical Light
Afek, I., Ambar, O., & Silberberg, Y. (2010) · Science · doi:10.1126/science.1188172 · Cited by 588
Two-Particle Bosonic-Fermionic Quantum Walk via Integrated Photonics
Sansoni, L., Sciarrino, F., Vallone, G., Mataloni, P., Crespi, A., Ramponi, R., & Osellame, R. (2012) · Physical Review Letters · doi:10.1103/physrevlett.108.010502 · Cited by 578
Self-citationDe Broglie wavelength of a non-local four-photon state
Walther, P., Pan, J.-W., Aspelmeyer, M., Ursin, R., Gasparoni, S., & Zeilinger, A. (2004) · Nature · doi:10.1038/nature02552 · Cited by 555
An On-Demand Coherent Single-Electron Source
Fève, G., Mahé, A., Berroir, J., Kontos, T., Plaçais, B., Glattli, D. C., Cavanna, A., Etienne, B., & Jin, Y. (2007) · Science · doi:10.1126/science.1141243 · Cited by 543
Electron counting statistics and coherent states of electric currentPreprint
Levitov, L. S., Lee, H., & Lesovik, G. B. (1996) · Cited by 530
Zhao, Y., Fung, C.-H. F., Qi, B., Chen, C., & Lo, H.-K. (2008) · Physical Review A · doi:10.1103/physreva.78.042333 · Cited by 511
Fractional statistics in anyon collisions
Bartolomei, H., Kumar, M., Bisognin, R., Marguerite, A., Berroir, J.-M., Bocquillon, E., Plaçais, B., Cavanna, A., Dong, Q., Gennser, U., et al. (2020) · Science · doi:10.1126/science.aaz5601 · Cited by 504
Submicrometer axial resolution optical coherence tomography
Považay, B., Bizheva, K. K., Unterhuber, A., Hermann, B., Sattmann, H., FERCHER, A. F., Drexler, W., Apolonski, A. A., Wadsworth, W. J., Knight, J. C., et al. (2002) · Optics Letters · doi:10.1364/ol.27.001800 · Cited by 482
High-rate measurement-device-independent quantum cryptography
Pirandola, S., Ottaviani, C., Spedalieri, G., Weedbrook, C., Braunstein, S. L., Lloyd, S., Gehring, T., Jacobsen, C. S., & Andersen, U. L. (2015) · Nature Photonics · doi:10.1038/nphoton.2015.83 · Cited by 476
Anderson localization of entangled photons in an integrated quantum walk
Crespi, A., Osellame, R., Ramponi, R., Giovannetti, V., Fazio, R., Sansoni, L., De Nicola, F., Sciarrino, F., & Mataloni, P. (2013) · Nature Photonics · doi:10.1038/nphoton.2013.26 · Cited by 474
Self-citationExperimental demonstration of a BDCZ quantum repeater node
Yuan, Z.-S., Chen, Y.-A., Zhao, B., Chen, S., Schmiedmayer, J., & Pan, J.-W. (2008) · Nature · doi:10.1038/nature07241 · Cited by 473
Indistinguishable Photons from Separated Silicon-Vacancy Centers in Diamond
Sipahigil, A., Jahnke, K. D., Rogers, L. J., Teraji, T., Isoya, J., Zibrov, A. S., Jelezko, F., & Lukin, M. D. (2014) · Physical Review Letters · doi:10.1103/physrevlett.113.113602 · Cited by 473
Strongly correlated quantum walks in optical lattices
Preiss, P. M., Ma, R., Tai, M. E., Lukin, A., Rispoli, M., Zupancic, P., Lahini, Y., Islam, R., & Greiner, M. (2015) · Science · doi:10.1126/science.1260364 · Cited by 454
Heralded entanglement between widely separated atoms
Hofmann, J., Krug, M., Ortegel, N., Gérard, L., Weber, M., Rosenfeld, W., & Weinfurter, H. (2012) · Science · doi:10.1126/science.1221856 · Cited by 442
Full-field implementation of a perfect eavesdropper on a quantum cryptography system
Gerhardt, I., Liu, Q., Lamas-Linares, A., Skaar, J., Kurtsiefer, C., & Makarov, V. (2011) · Nature Communications · doi:10.1038/ncomms1348 · Cited by 436
High-efficiency multiphoton boson sampling
Wang, H., He, Y., Li, Y.-H., Su, Z.-E., Li, B., Huang, H.-L., Ding, X., Chen, M.-C., Liu, C., Qin, J., et al. (2017) · Nature Photonics · doi:10.1038/nphoton.2017.63 · Cited by 430
Experimental measurement-device-independent quantum key distribution
Liu, Y., Chen, T.-Y., Wang, L.-J., Liang, H., Shentu, G.-L., Wang, J., Cui, K., Yin, H.-L., Liu, N.-L., Li, L., et al. (2013) · Physical Review Letters · doi:10.1103/physrevlett.111.130502 · Cited by 413
Specht, H. P., Nölleke, C., Reiserer, A., Uphoff, M., Figueroa, E., Ritter, S., & Rempe, G. (2011) · Nature · doi:10.1038/nature09997 · Cited by 411
Quantum teleportation in high dimensions
Luo, Y.-H., Zhong, H.-S., Erhard, M., Wang, X.-L., Peng, L.-C., Krenn, M., Jiang, X., Li, L., Liu, N.-L., Lu, C.-Y., et al. (2019) · Physical Review Letters · doi:10.1103/physrevlett.123.070505 · Cited by 406
Coherence and Indistinguishability of Single Electrons Emitted by Independent Sources
Bocquillon, E., Freulon, V., Berroir, J., Degiovanni, P., Plaçais, B., Cavanna, A., Jin, Y., & Fève, G. (2013) · Science · doi:10.1126/science.1232572 · Cited by 391
Mach-Zehnder Interferometry at the Heisenberg Limit with Coherent and Squeezed-Vacuum Light
Pezzè, L., & Smerzi, A. (2008) · Physical Review Letters · doi:10.1103/physrevlett.100.073601 · Cited by 367
Minimal-excitation states for electron quantum optics using levitons
Dubois, J., Jullien, T., Portier, F., Roche, P., Cavanna, A., Jin, Y., Wegscheider, W., Roulleau, P., & Glattli, D. C. (2013) · Nature · doi:10.1038/nature12713 · Cited by 367
ON THE EINSTEIN PODOLSKY ROSEN PARADOX
Bell, J. S. (2001) · WORLD SCIENTIFIC eBooks · doi:10.1142/9789812386540_0002 · Cited by 359
Two-photon interference of the emission from electrically tunable remote quantum dots
Patel, R. B., Bennett, A. J., Farrer, I. A., Nicoll, C. A., Ritchie, D. A., & Shields, A. J. (2010) · Nature Photonics · doi:10.1038/nphoton.2010.161 · Cited by 343
Tang, Z., Liao, Z., Xu, F., Qi, B., Qian, L., & Lo, H.-K. (2014) · Physical Review Letters · doi:10.1103/physrevlett.112.190503 · Cited by 334
Demonstration of Dispersion-Canceled Quantum-Optical Coherence Tomography
Nasr, M. B., Saleh, B. E. A., Sergienko, A. V., & Teich, M. C. (2003) · Physical Review Letters · doi:10.1103/physrevlett.91.083601 · Cited by 333
Two-photon interference in a Mach-Zehnder interferometer
Rarity, J., Tapster, P., Jakeman, E., Larchuk, T., Campos, R., Teich, M., & Saleh, B. (1990) · Physical Review Letters · doi:10.1103/physrevlett.65.1348 · Cited by 325
Quantum interference between two single photons emitted by independently trapped atoms
Beugnon, J., Jones, M. P. A., Dingjan, J., Darquié, B., Messin, G., Browaeys, A., & Grangier, P. (2006) · Nature · doi:10.1038/nature04628 · Cited by 324
Boson Sampling from a Gaussian State
Lund, A. P., Laing, A., Rahimi-Keshari, S., Rudolph, T., O’Brien, J. L., & Ralph, T. C. (2014) · Physical Review Letters · doi:10.1103/physrevlett.113.100502 · Cited by 316
Practical quantum key distribution protocol without monitoring signal disturbance
Sasaki, T., Yamamoto, Y., & Koashi, M. (2014) · Nature · doi:10.1038/nature13303 · Cited by 315
Experimental validation of photonic boson sampling
Spagnolo, N., Vitelli, C., Bentivegna, M., Brod, D. J., Crespi, A., Flamini, F., Giacomini, S., Milani, G., Ramponi, R., Mataloni, P., et al. (2014) · Nature Photonics · doi:10.1038/nphoton.2014.135 · Cited by 312
Self-citationMaximum efficiency of a linear-optical Bell-state analyzer
Calsamiglia, J., & Lütkenhaus, N. (2001) · Applied Physics B · doi:10.1007/s003400000484 · Cited by 307
Kwiat, P. G., & Weinfurter, H. (1998) · Physical Review A · doi:10.1103/physreva.58.r2623 · Cited by 287
Quantum-optical coherence tomography with dispersion cancellation
Abouraddy, A. F., Nasr, M. B., Saleh, B. E. A., Sergienko, A. V., & Teich, M. C. (2002) · Physical Review A · doi:10.1103/physreva.65.053817 · Cited by 275
Time-Reversal and Super-Resolving Phase Measurements
Resch, K. J., Pregnell, K. L., Prevedel, R., Gilchrist, A., Pryde, G. J., O’Brien, J. L., & White, A. G. (2007) · Physical Review Letters · doi:10.1103/physrevlett.98.223601 · Cited by 269
Quantum interference of photon pairs from two remote trapped atomic ions
Maunz, P., Moehring, D. L., Olmschenk, S., Younge, K. C., Matsukevich, D. N., & Monroe, C. (2007) · Nature Physics · doi:10.1038/nphys644 · Cited by 268
Two-photon quantum interference from separate nitrogen vacancy centers in diamond
Bernien, H., Childress, L., Robledo, L., Markham, M., Twitchen, D., & Hanson, R. (2012) · Physical Review Letters · doi:10.1103/physrevlett.108.043604 · Cited by 262
Measurement-device-independent quantum key distribution over 200 km
Tang, Y.-L., Yin, H.-L., Chen, S.-J., Liu, Y., Zhang, W.-J., Jiang, X., Zhang, L., Wang, J., You, L.-X., Guan, J.-Y., et al. (2014) · Physical Review Letters · doi:10.1103/physrevlett.113.190501 · Cited by 251
Quantum interference in electron collision
Liu, R. C., Odom, B., Yamamoto, Y., & Tarucha, S. (1998) · Nature · doi:10.1038/34611 · Cited by 249
Interference of single photons from two separate semiconductor quantum dots
Flagg, E., Muller, A., Polyakov, S., Ling, A., Migdall, A., & Solomon, G. (2010) · Physical Review Letters · doi:10.1103/physrevlett.104.137401 · Cited by 243
Experimental scattershot boson sampling
Bentivegna, M., Spagnolo, N., Vitelli, C., Flamini, F., Viggianiello, N., Latmiral, L., Mataloni, P., Brod, D. J., Galvão, E. F., Crespi, A., et al. (2015) · Science Advances · doi:10.1126/sciadv.1400255 · Cited by 239
Self-citationUnconditional violation of the shot-noise limit in photonic quantum metrology
Slussarenko, S., Weston, M. M., Chrzanowski, H. M., Shalm, L. K., Verma, V. B., Nam, S. W., & Pryde, G. J. (2017) · Nature Photonics · doi:10.1038/s41566-017-0011-5 · Cited by 239
Minimal Excitation States of Electrons in One-Dimensional Wires
Keeling, J., Klich, I., & Levitov, L. S. (2006) · Physical Review Letters · doi:10.1103/physrevlett.97.116403 · Cited by 238
Realizable higher-dimensional two-particle entanglements via multiport beam splitters
Z-dotukowski, M., Zeilinger, A., & Horne, M. A. (1997) · Physical Review A · doi:10.1103/physreva.55.2564 · Cited by 234
Two-particle quantum interference in tunnel-coupled optical tweezers
Kaufman, A. M., Lester, B., Reynolds, C., Wall, M. L., Foss‐Feig, M., Hazzard, K. R. A., Rey, A. M., & Regal, C. A. (2014) · Science · doi:10.1126/science.1250057 · Cited by 232
Can Two-Photon Interference be Considered the Interference of Two Photons?
Pittman, T. B., Strekalov, D. V., Migdall, A., Rubin, M. H., Sergienko, A. V., & Shih, Y. H. (1996) · Physical Review Letters · doi:10.1103/physrevlett.77.1917 · Cited by 228
Ferreira da Silva, T., Vitoreti, D., Xavier, G. B., do Amaral, G. C., Temporão, G. P., & von der Weid, J. P. (2013) · Physical Review A · doi:10.1103/physreva.88.052303 · Cited by 227
Quantum tomography of an electron
Jullien, T., Roulleau, P., Roche, B., Cavanna, A., Jin, Y., & Glattli, D. C. (2014) · Nature · doi:10.1038/nature13821 · Cited by 222
Arbitrarily complete bell-state measurement using only linear optical elements
Grice, W. P. (2011) · Physical Review A · doi:10.1103/physreva.84.042331 · Cited by 218
Optimal quantum cloning of orbital angular momentum photon qubits through Hong–Ou–Mandel coalescence
Nagali, E., Sansoni, L., Sciarrino, F., De Martini, F., Marrucci, L., Piccirillo, B., Karimi, E., & Santamato, E. (2009) · Nature Photonics · doi:10.1038/nphoton.2009.214 · Cited by 218
Self-citationEdamatsu, K., Shimizu, R., & Itoh, T. (2002) · Physical Review Letters · doi:10.1103/physrevlett.89.213601 · Cited by 216
Attosecond-resolution Hong-Ou-Mandel interferometry
Lyons, A., Knee, G. C., Bolduc, E., Roger, T., Leach, J., Gauger, E. M., & Faccio, D. (2018) · Science Advances · doi:10.1126/sciadv.aap9416 · Cited by 211
Phase-remapping attack in practical quantum-key-distribution systems
Fung, C.-H. F., Qi, B., Tamaki, K., & Lo, H.-K. (2007) · Physical Review A · doi:10.1103/physreva.75.032314 · Cited by 209
Quantum interference of single photons from remote nitrogen-vacancy centers in diamond
Sipahigil, A., Goldman, M. L., Togan, E., Chu, Y., Markham, M., Twitchen, D. J., Zibrov, A. S., Kubanek, A., & Lukin, M. D. (2012) · Physical Review Letters · doi:10.1103/physrevlett.108.143601 · Cited by 205
Memory-built-in quantum teleportation with photonic and atomic qubits
Chen, Y.-A., Chen, S., Yuan, Z.-S., Zhao, B., Chuu, C.-S., Schmiedmayer, J., & Pan, J.-W. (2008) · Nature Physics · doi:10.1038/nphys832 · Cited by 205
Simple scheme for efficient linear optics quantum gates
Ralph, T. C., White, A. G., Munro, W. J., & Milburn, G. J. (2001) · Physical Review A · doi:10.1103/physreva.65.012314 · Cited by 205
Steinberg, A. M., Kwiat, P. G., & Chiao, R. Y. (1992) · Physical Review A · doi:10.1103/physreva.45.6659 · Cited by 202
Quantum theory of the lossless beam splitter
Fearn, H., & Loudon, R. (1987) · Optics Communications · doi:10.1016/0030-4018(87)90275-6 · Cited by 197
Politi, A., Matthews, J., Thompson, M. G., & O'Brien, J. L. (2009) · IEEE Journal of Selected Topics in Quantum Electronics · doi:10.1109/jstqe.2009.2026060 · Cited by 196
Atomic Hong–Ou–Mandel experiment
Lopes, R., Imanaliev, A., Aspect, A., Cheneau, M., Boiron, D., & Westbrook, C. I. (2015) · Nature · doi:10.1038/nature14331 · Cited by 195
Electron Quantum Optics: Partitioning Electrons One by One
Bocquillon, E., Parmentier, F. D., Grenier, C., Berroir, J., Degiovanni, P., Glattli, D. C., Plaçais, B., Cavanna, A., Jin, Y., & Fève, G. (2012) · Physical Review Letters · doi:10.1103/physrevlett.108.196803 · Cited by 195
Experimental interference of independent photons
Kaltenbaek, R., Blauensteiner, B., Żukowski, M., Aspelmeyer, M., & Zeilinger, A. (2006) · Physical Review Letters · doi:10.1103/physrevlett.96.240502 · Cited by 192
Two-plasmon quantum interference
Fakonas, J. S., Lee, H., Kelaita, Y., & Atwater, H. A. (2014) · Nature Photonics · doi:10.1038/nphoton.2014.40 · Cited by 188
Quantum interference in plasmonic circuits
Heeres, R. W., Kouwenhoven, L. P., & Zwiller, V. (2013) · Nature Nanotechnology · doi:10.1038/nnano.2013.150 · Cited by 185
Frequency-domain Hong–Ou–Mandel interference
Kobayashi, T., Ikuta, R., Yasui, S., Miki, S., Yamashita, T., Terai, H., Yamamoto, T., Koashi, M., & Imoto, N. (2016) · Nature Photonics · doi:10.1038/nphoton.2016.74 · Cited by 185
Swap test and Hong–Ou–Mandel effect are equivalent
Garcia-Escartin, J. C., & Chamorro-Posada, P. (2013) · Physical Review A · doi:10.1103/physreva.87.052330 · Cited by 182
Experimental Quantum Computing to Solve Systems of Linear Equations
Cai, X.-D., Weedbrook, C., Su, Z.-E., Chen, M.-C., Gu, M., Zhu, M.-J., Li, L., Liu, N.-L., Lu, C.-Y., & Pan, J.-W. (2013) · Physical Review Letters · doi:10.1103/physrevlett.110.230501 · Cited by 173
Three-photon bosonic coalescence in an integrated tritter
Spagnolo, N., Vitelli, C., Aparo, L., Mataloni, P., Sciarrino, F., Crespi, A., Ramponi, R., & Osellame, R. (2013) · Nature Communications · doi:10.1038/ncomms2616 · Cited by 170
Self-citationWei, Y.-J., He, Y.-M., Chen, M.-C., Hu, Y.-N., He, Y., Wu, D., Schneider, C., Kamp, M., Höfling, S., Lu, C.-Y., et al. (2014) · Nano Letters · doi:10.1021/nl503081n · Cited by 169
Two-photon quantum walk in a multimode fiber
Defienne, H., Barbieri, M., Walmsley, I. A., Smith, B. J., & Gigan, S. (2016) · Science Advances · doi:10.1126/sciadv.1501054 · Cited by 168
A quantum description of the beam splitter
Prasad, S., Scully, M. O., & Martienssen, W. (1987) · Optics Communications · doi:10.1016/0030-4018(87)90015-0 · Cited by 167
Fundamental Aspects of Quantum Theory
Frigerio, A., & Gorini, V. (1986) · NATO ASI series. Series B : Physics · doi:10.1007/978-1-4684-5221-1 · Cited by 166
Distinguishability and Many-Particle Interference
Menssen, A. J., Jones, A. E., Metcalf, B. J., Tichy, M. C., Barz, S., Kolthammer, W. S., & Walmsley, I. A. (2017) · Physical Review Letters · doi:10.1103/physrevlett.118.153603 · Cited by 162
Photonic implementation of boson sampling: a review
Brod, D. J., Galvão, E. F., Crespi, A., Osellame, R., Spagnolo, N., & Sciarrino, F. (2019) · Advanced Photonics · doi:10.1117/1.ap.1.3.034001 · Cited by 159
Self-citationQuantum interference of tunably indistinguishable photons from remote organic molecules
Lettow, R., Rezus, Y. L. A., Renn, A., Zumofen, G., Ikonen, E., Götzinger, S., & Sandoghdar, V. (2010) · Physical Review Letters · doi:10.1103/physrevlett.104.123605 · Cited by 157
Quantum computing on encrypted data
Fisher, K. A. G., Broadbent, A., Shalm, L. K., Yan, Z., Lavoie, J., Prevedel, R., Jennewein, T., & Resch, K. J. (2014) · Nature Communications · doi:10.1038/ncomms4074 · Cited by 157
Experimental demonstration of a quantum key distribution without signal disturbance monitoring
Wang, S., Yin, Z.-Q., Chen, W., He, D.-Y., Song, X.-T., Li, H.-W., Zhang, L.-J., Zhou, Z., Guo, G.-C., & Han, Z.-F. (2015) · Nature Photonics · doi:10.1038/nphoton.2015.209 · Cited by 156
Experimental realization of the quantum universal not gate
De Martini, F., Bužek, V., Sciarrino, F., & Sias, C. (2002) · Nature · doi:10.1038/nature01093 · Cited by 153
Self-citationRelation between input and output states for a beam splitter
Ou, Z. Y., Hong, C. K., & Mandel, L. (1987) · Optics Communications · doi:10.1016/0030-4018(87)90271-9 · Cited by 152
Spatially structured photons that travel in free space slower than the speed of light
Giovannini, D., Romero, J., Potoček, V., Ferenczi, G., Speirits, F., Barnett, S. M., Faccio, D., & Padgett, M. J. (2015) · Science · doi:10.1126/science.aaa3035 · Cited by 150
Engineering two-photon high-dimensional states through quantum interference
Zhang, Y., Roux, F. S., Konrad, T., Agnew, M., Leach, J., & Forbes, A. (2016) · Science Advances · doi:10.1126/sciadv.1501165 · Cited by 149
Self-citationQuantum Walks of Correlated Photon Pairs in Two-Dimensional Waveguide Arrays
Poulios, K., Keil, R., Fry, D., Meinecke, J. D. A., Matthews, J. C. F., Politi, A., Lobino, M., Gräfe, M., Heinrich, M., Nolte, S., et al. (2014) · Physical Review Letters · doi:10.1103/physrevlett.112.143604 · Cited by 148 · cited 2×
“[158] Poulios, K.”
MethodInterference between independent photons
Paul, H. (1986) · Reviews of Modern Physics · doi:10.1103/revmodphys.58.209 · Cited by 147
Linear optical quantum computing in a single spatial mode
Humphreys, P. C., Metcalf, B. J., Spring, J. B., Moore, M., Jin, X.-M., Barbieri, M., Kolthammer, W. S., & Walmsley, I. A. (2013) · Physical Review Letters · doi:10.1103/physrevlett.111.150501 · Cited by 145
Multiphoton quantum interference in a multiport integrated photonic device
Metcalf, B. J., Thomas-Peter, N., Spring, J. B., Kundys, D., Broome, M. A., Humphreys, P. C., Jin, X.-M., Barbieri, M., Steven Kolthammer, W., Gates, J. C., et al. (2013) · Nature Communications · doi:10.1038/ncomms2349 · Cited by 143
Hong-Ou-Mandel experiment for temporal investigation of single-electron fractionalization
Freulon, V., Marguerite, A., Berroir, J., Plaçais, B., Cavanna, A., Jin, Y., & Fève, G. (2015) · Nature Communications · doi:10.1038/ncomms7854 · Cited by 138
Two-photon quantum walks in an elliptical direct-write waveguide array
Owens, J. O., Broome, M. A., Biggerstaff, D. N., Goggin, M. E., Fedrizzi, A., Linjordet, T., Ams, M., Marshall, G. D., Twamley, J., Withford, M. J., et al. (2011) · New Journal of Physics · doi:10.1088/1367-2630/13/7/075003 · Cited by 135
High-dimensional quantum cloning and applications to quantum hacking
Bouchard, F., Fickler, R., Boyd, R. W., & Karimi, E. (2017) · Science Advances · doi:10.1126/sciadv.1601915 · Cited by 135
Self-citationSingle-electron quantum tomography in quantum Hall edge channels
Grenier, C., HERVÉ, R., Bocquillon, E., Parmentier, F. D., Plaçais, B., Berroir, J., Fève, G., & Degiovanni, P. (2011) · New Journal of Physics · doi:10.1088/1367-2630/13/9/093007 · Cited by 131
Generalized Multiphoton Quantum Interference
Tillmann, M., Tan, S.-H., Stoeckl, S. E., Sanders, B. C., de Guise, H., Heilmann, R., Nolte, S., Szameit, A., & Walther, P. (2015) · Physical Review X · doi:10.1103/physrevx.5.041015 · Cited by 127
Zero-Transmission Law for Multiport Beam Splitters
Tichy, M. C., Tiersch, M., de Melo, F., Mintert, F., & Buchleitner, A. (2010) · Physical Review Letters · doi:10.1103/physrevlett.104.220405 · Cited by 126
Quantum interferometry with three-dimensional geometry
Spagnolo, N., Aparo, L., Vitelli, C., Crespi, A., Ramponi, R., Osellame, R., Mataloni, P., & Sciarrino, F. (2012) · Scientific Reports · doi:10.1038/srep00862 · Cited by 115
Self-citationRobust concurrent remote entanglement between two superconducting qubits
Narla, A., Shankar, S., Hatridge, M., Leghtas, Z., Sliwa, K. M., Zalys-Geller, E., Mundhada, S. O., Pfaff, W., Frunzio, L., Schoelkopf, R. J., et al. (2016) · Physical Review X · doi:10.1103/physrevx.6.031036 · Cited by 115
Revisiting Quantum Optics with Surface Plasmons and Plasmonic Resonators
Marquier, F., Sauvan, C., & Greffet, J. (2017) · ACS Photonics · doi:10.1021/acsphotonics.7b00475 · Cited by 115
Implementation of quantum and classical discrete fractional fourier transforms
Weimann, S., Perez-Leija, A., Lebugle, M., Keil, R., Tichy, M., Gräfe, M., Heilmann, R., Nolte, S., Moya-Cessa, H., Weihs, G., et al. (2016) · Nature Communications · doi:10.1038/ncomms11027 · Cited by 114
Efficient Generation of Large Number-Path Entanglement Using Only Linear Optics and Feed-Forward
Cable, H. V., & Dowling, J. P. (2007) · Physical Review Letters · doi:10.1103/physrevlett.99.163604 · Cited by 112
Observation of Quantum Interference in the Plasmonic Hong-Ou-Mandel Effect
Martino, G. D., Sonnefraud, Y., Tame, M., Kéna‐Cohen, S., Dieleman, F., Özdemir, Ş. K., Kim, M. S., & Maier, S. A. (2014) · Physical Review Applied · doi:10.1103/physrevapplied.1.034004 · Cited by 110
Anti-coalescence of bosons on a lossy beam splitter
Vest, B., Dheur, M.-C., Devaux, É., Baron, A., Rousseau, E., Hugonin, J., Greffet, J., Messin, G., & Marquier, F. (2017) · Science · doi:10.1126/science.aam9353 · Cited by 106
Partial indistinguishability theory for multiphoton experiments in multiport devices
Shchesnovich, V. S. (2015) · Physical Review A · doi:10.1103/physreva.91.013844 · Cited by 104
Quantum interference between transverse spatial waveguide modes
Mohanty, A., Zhang, M., Dutt, A., Ramelow, S., Nussenzveig, P., & Lipson, M. (2017) · Nature Communications · doi:10.1038/ncomms14010 · Cited by 103
Hong-Ou-Mandel interferometry on a biphoton beat note
Chen, Y., Fink, M., Steinlechner, F., Torres, J. P., & Ursin, R. (2019) · npj Quantum Information · doi:10.1038/s41534-019-0161-z · Cited by 101
Indistinguishable Photons from Independent Semiconductor Nanostructures
Sanaka, K., Pawlis, A., Ladd, T. D., Lischka, K., & Yamamoto, Y. (2009) · Physical Review Letters · doi:10.1103/physrevlett.103.053601 · Cited by 99
Quantum walk of two interacting bosons
Lahini, Y., Verbin, M., Huber, S. D., Bromberg, Y., Pugatch, R., & Silberberg, Y. (2012) · Physical Review A · doi:10.1103/physreva.86.011603 · Cited by 99
Karimi, E., Giovannini, D., Bolduc, E., Bent, N., Miatto, F. M., Padgett, M. J., & Boyd, R. W. (2014) · Physical Review A · doi:10.1103/physreva.89.013829 · Cited by 99
Self-citationInterference of identical particles from entanglement to boson-sampling
Tichy, M. C. (2014) · Journal of Physics B Atomic Molecular and Optical Physics · doi:10.1088/0953-4075/47/10/103001 · Cited by 98
Experimental quantum key distribution without monitoring signal disturbance
Takesue, H., Sasaki, T., Tamaki, K., & Koashi, M. (2015) · Nature Photonics · doi:10.1038/nphoton.2015.173 · Cited by 97
Hong-Ou-Mandel interference of two phonons in trapped ions
Toyoda, K., Hiji, R., Noguchi, A., & Urabe, S. (2015) · Nature · doi:10.1038/nature15735 · Cited by 97
Experimental passive round-robin differential phase-shift quantum key distribution
Guan, J.-Y., Cao, Z., Liu, Y., Shen-Tu, G.-L., Pelc, J. S., Fejer, M. M., Peng, C.-Z., Ma, X., Zhang, Q., & Pan, J.-W. (2015) · Physical Review Letters · doi:10.1103/physrevlett.114.180502 · Cited by 96
Quantum Interference between Light Sources Separated by 150 Million Kilometers
Deng, Y.-H., Wang, H., Ding, X., Duan, Z.-C., Qin, J., Chen, M.-C., He, Y., He, Y., Li, J.-P., Li, Y.-H., et al. (2019) · Physical Review Letters · doi:10.1103/physrevlett.123.080401 · Cited by 93
Okamoto, R., O’Brien, J. L., Hofmann, H. F., & Takeuchi, S. (2011) · Proceedings of the National Academy of Sciences · doi:10.1073/pnas.1018839108 · Cited by 92
Quantum gates using linear optics and postselection
Knill, E. (2002) · Physical Review A · doi:10.1103/physreva.66.052306 · Cited by 92
Fourth-order interference in parametric downconversion
Rarity, J. G., & Tapster, P. R. (1989) · Journal of the Optical Society of America B · doi:10.1364/josab.6.001221 · Cited by 91
Conditional control of the quantum states of remote atomic memories for quantum networking
Felinto, D., Chou, C. W., Laurat, J., Schomburg, E. W., de Riedmatten, H., & Kimble, H. J. (2006) · Nature Physics · doi:10.1038/nphys450 · Cited by 90
Ricci, M., Sciarrino, F., Sias, C., & De Martini, F. (2004) · Physical Review Letters · doi:10.1103/physrevlett.92.047901 · Cited by 90
Self-citationBeating the standard quantum limit: phase super-sensitivity of N-photon interferometers
Okamoto, R., Hofmann, H. F., Nagata, T., O'Brien, J. L., Sasaki, K., & Takeuchi, S. (2008) · New Journal of Physics · doi:10.1088/1367-2630/10/7/073033 · Cited by 90
Experimental access to higher-dimensional entangled quantum systems using integrated optics
Schaeff, C., Polster, R., Huber, M., Ramelow, S., & Zeilinger, A. (2015) · Optica · doi:10.1364/optica.2.000523 · Cited by 89
Direct Observation of the Second-Order Coherence of Parametrically Generated Light
Abram, I. I., Raj, R. K., Oudar, J. L., & Dolique, G. (1986) · Physical Review Letters · doi:10.1103/physrevlett.57.2516 · Cited by 89
Many-particle interference beyond many-boson and many-fermion statistics
Tichy, M. C., Tiersch, M., Mintert, F., & Buchleitner, A. (2012) · New Journal of Physics · doi:10.1088/1367-2630/14/9/093015 · Cited by 86
Entanglement: quantum or classical?
Paneru, D., Cohen, E., Fickler, R., Boyd, R. W., & Karimi, E. (2020) · Reports on Progress in Physics · doi:10.1088/1361-6633/ab85b9 · Cited by 86
Self-citationExperimental optimal cloning of four-dimensional quantum states of photons
Nagali, E., Giovannini, D., Marrucci, L., Slussarenko, S., Santamato, E., & Sciarrino, F. (2010) · Physical Review Letters · doi:10.1103/physrevlett.105.073602 · Cited by 85
Self-citationInterference of two photons of different color
Raymer, M. G., van Enk, S. J., McKinstrie, C. J., & McGuinness, H. J. (2010) · Optics Communications · doi:10.1016/j.optcom.2009.10.057 · Cited by 84
Current Correlations from a Mesoscopic Anyon Collider
Rosenow, B., Levkivskyi, I. P., & Halperin, B. I. (2016) · Physical Review Letters · doi:10.1103/physrevlett.116.156802 · Cited by 83
Quantum optical coherence tomography of a biological sample
Nasr, M. B., Goode, D. P., Nguyen, N., Rong, G., Yang, L., Reinhard, B. M., Saleh, B. E. A., & Teich, M. C. (2009) · Optics Communications · doi:10.1016/j.optcom.2008.11.061 · Cited by 79
Nonmonotonic quantum-to-classical transition in multiparticle interference
Ra, Y.-S., Tichy, M. C., Lim, H., Kwon, O., Mintert, F., Buchleitner, A., & Kim, Y.-H. (2013) · Proceedings of the National Academy of Sciences · doi:10.1073/pnas.1206910110 · Cited by 78
Indistinguishable photons from a single molecule
Kiraz, A., Ehrl, M., Hellerer, T., Müstecaplıoğlu, Ö. E., Bräuchle, C., & Zumbusch, A. (2005) · Physical Review Letters · doi:10.1103/physrevlett.94.223602 · Cited by 77
Dispersion-Cancelled and Dispersion-Sensitive Quantum Optical Coherence Tomography
Nasr, M. B., Saleh, B. E. A., Sergienko, A. V., & Teich, M. C. (2004) · Optics Express · doi:10.1364/opex.12.001353 · Cited by 76
Levitons for electron quantum optics
Glattli, D. C., & Roulleau, P. (2016) · physica status solidi (b) · doi:10.1002/pssb.201600650 · Cited by 74
Observation of subluminal twisted light in vacuum
Bouchard, F., Harris, J., Mand, H., Boyd, R. W., & Karimi, E. (2016) · Optica · doi:10.1364/optica.3.000351 · Cited by 73
Self-citationElectron quantum optics as quantum signal processing
Roussel, B., Cabart, C., Fève, G., Thibierge, É., & Degiovanni, P. (2017) · physica status solidi (b) · doi:10.1002/pssb.201600621 · Cited by 73
Joining the quantum state of two photons into one
Vitelli, C., Spagnolo, N., Aparo, L., Sciarrino, F., Santamato, E., & Marrucci, L. (2013) · Nature Photonics · doi:10.1038/nphoton.2013.107 · Cited by 72
Self-citationDecoherence and relaxation of a single electron in a one-dimensional conductor
Marguerite, A., Cabart, C., Wahl, C., Roussel, B., Freulon, V., Ferraro, D., Grenier, C., Berroir, J., Plaçais, B., Jonckheere, T., et al. (2016) · Physical review. B./Physical review. B · doi:10.1103/physrevb.94.115311 · Cited by 72
Quantum tomography of electrical currents
Bisognin, R., Marguerite, A., Roussel, B., Kumar, M., Cabart, C., Chapdelaine, C., Ali Mohammad-djafari, A., Berroir, J., Bocquillon, E., Plaçais, B., et al. (2019) · Nature Communications · doi:10.1038/s41467-019-11369-5 · Cited by 71
Efficient Optical Quantum State Engineering
McCusker, K. T., & Kwiat, P. G. (2009) · Physical Review Letters · doi:10.1103/physrevlett.103.163602 · Cited by 70
Yuan, Z.-S., Chen, Y.-A., Chen, S., Zhao, B., Koch, M., Strassel, T., Zhao, Y., Zhu, G.-J., Schmiedmayer, J., & Pan, J.-W. (2007) · Physical Review Letters · doi:10.1103/physrevlett.98.180503 · Cited by 65
High-Visibility On-Chip Quantum Interference of Single Surface Plasmons
Cai, Y.-J., Li, M., Ren, X.-F., Zou, C.-L., Xiong, X., Lei, H.-L., Liu, B.-H., Guo, G.-P., & Guo, G.-C. (2014) · Physical Review Applied · doi:10.1103/physrevapplied.2.014004 · Cited by 63
Entangling different-color photons via time-resolved measurement and active feed forward
Zhao, T.-M., Zhang, H., Yang, J., Sang, Z.-R., Jiang, X., Bao, X.-H., & Pan, J.-W. (2014) · Physical Review Letters · doi:10.1103/physrevlett.112.103602 · Cited by 61
Proposal for demonstrating the Hong–Ou–Mandel effect with matter waves
Lewis-Swan, R. J., & Kheruntsyan, K. V. (2014) · Nature Communications · doi:10.1038/ncomms4752 · Cited by 61
Cloning a reald-dimensional quantum state on the edge of the no-signaling condition
Navez, P., & Cerf, N. J. (2003) · Physical Review A · doi:10.1103/physreva.68.032313 · Cited by 60
Phase-conjugate optical coherence tomography
Erkmen, B. I., & Shapiro, J. H. (2006) · Physical Review A · doi:10.1103/physreva.74.041601 · Cited by 60
Improved security bound for the round-robin-differential-phase-shift quantum key distribution
Yin, Z.-Q., Wang, S., Chen, W., Han, Y.-G., Wang, R., Guo, G.-C., & Han, Z.-F. (2018) · Nature Communications · doi:10.1038/s41467-017-02211-x · Cited by 59
Fourth-order interference technique for determining the coherence time of a light beam
Ou, Z. Y., Gage, E. C., Magill, B. E., & Mandel, L. (1989) · Journal of the Optical Society of America B · doi:10.1364/josab.6.000100 · Cited by 57
Four-photon indistinguishability transition
Tichy, M. C., Lim, H., Ra, Y.-S., Mintert, F., Kim, Y.-H., & Buchleitner, A. (2011) · Physical Review A · doi:10.1103/physreva.83.062111 · Cited by 57
Classical dispersion-cancellation interferometry
Resch, K. J., Puvanathasan, P., Lundeen, J. S., Mitchell, M. W., & Bizheva, K. (2007) · Optics Express · doi:10.1364/oe.15.008797 · Cited by 56
Non-classical interference in integrated 3D multiports
Meany, T., Delanty, M., Gross, S., Marshall, G. D., Steel, M. J., & Withford, M. J. (2012) · Optics Express · doi:10.1364/oe.20.026895 · Cited by 53
Coalescence and anti-coalescence of surface plasmons on a lossy beamsplitterPreprint
Vest, B., Dheur, M.-C., Devaux, É., Ebbesen, T. W., Baron, A., Rousseau, E., Hugonin, J., Greffet, J., Messin, G., & Marquier, F. (2016) · arXiv (Cornell University) · doi:10.48550/arxiv.1610.07479 · Cited by 49
Quantum Walks of a Phonon in Trapped Ions
Tamura, M., Mukaiyama, T., & Toyoda, K. (2020) · Physical Review Letters · doi:10.1103/physrevlett.124.200501 · Cited by 49
Quantum Entanglement: A Fundamental Concept Finding its Applications
Zeilinger, A. (1998) · Physica Scripta · doi:10.1238/physica.topical.076a00203 · Cited by 47
Three-photon Hong–Ou–Mandel interference at a multiport mixer
Campos, R. A. (2000) · Physical Review A · doi:10.1103/physreva.62.013809 · Cited by 47
Two-photon interference in optical fiber multiports
Weihs, G., Reck, M., Weinfurter, H., & Zeilinger, A. (1996) · Physical Review A · doi:10.1103/physreva.54.893 · Cited by 47
Experimental round-robin differential phase-shift quantum key distribution
Li, Y.-H., Cao, Y. W., Dai, H., Lin, J., Zhang, Z., Chen, W. R., Xu, Y., Guan, J.-Y., Liao, S., Yin, J., et al. (2016) · Physical Review A · doi:10.1103/physreva.93.030302 · Cited by 47
Bootstrapping Approach for Generating Maximally Path-Entangled Photon States
Kapale, K. T., & Dowling, J. P. (2007) · Physical Review Letters · doi:10.1103/physrevlett.99.053602 · Cited by 46
Knill, E. (2003) · Physical Review A · doi:10.1103/physreva.68.064303 · Cited by 46
Three-photon N00N states generated by photon subtraction from double photon pairs
Kim, H., Park, H. S., & Choi, S.-K. (2009) · Optics Express · doi:10.1364/oe.17.019720 · Cited by 44
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Barbieri, M. (2022) · PRX Quantum · doi:10.1103/prxquantum.3.010202 · Cited by 122
Quantum structured light in high dimensions
Nape, I. M., Sephton, B., Ornelas, P., Moodley, C., & Forbes, A. (2023) · APL Photonics · doi:10.1063/5.0138224 · Cited by 107
Two-Photon Interference from a Quantum Emitter in Hexagonal Boron Nitride
Fournier, C., Roux, S., Watanabe, K., Taniguchi, T., Buil, S., Barjon, J., Hermier, J., & Delteil, A. (2023) · Physical Review Applied · doi:10.1103/physrevapplied.19.l041003 · Cited by 73
High-Dimensional Two-Photon Interference Effects in Spatial Modes
Hiekkamäki, M., & Fickler, R. (2021) · Physical Review Letters · doi:10.1103/physrevlett.126.123601 · Cited by 70
Self-citationPolarization-entangled Bell state generation from an epsilon-near-zero metasurface
Jia, W., Saerens, G., Talts, Ü., Weigand, H., Chapman, R. J., Li, L., Grange, R., & Yang, Y. (2025) · Science Advances · doi:10.1126/sciadv.ads3576 · Cited by 56
Quantum interferometers: Principles and applications
Jin, R., Zeng, Z.-Q., You, C., & Yuan, C. (2024) · Progress in Quantum Electronics · doi:10.1016/j.pquantelec.2024.100519 · Cited by 46
Artificial Intelligence in Classical and Quantum Photonics
Vernuccio, F., Bresci, A., Cimini, V., Giuseppi, A., Cerullo, G., Polli, D., & Valensise, C. M. (2022) · Laser & Photonics Review · doi:10.1002/lpor.202100399 · Cited by 43
Triggered emission of indistinguishable photons from an organic dye molecule
Lombardi, P., Colautti, M., Duquennoy, R., Murtaza, G., Majumder, P., & Toninelli, C. (2021) · Applied Physics Letters · doi:10.1063/5.0048567 · Cited by 40
Telecom-Band Quantum Interference of Frequency-Converted Photons from Remote Detuned NV Centers
Stolk, A., van der Enden, K. L., Roehsner, M.-C., Teepe, A., Faes, S. O. J., Bradley, C. E., Cadot, S., van Rantwijk, J., Raa, I. T., Hagen, R., et al. (2022) · PRX Quantum · doi:10.1103/prxquantum.3.020359 · Cited by 38
Requirements for a processing-node quantum repeater on a real-world fiber grid
Avis, G., da Silva, F. F., Coopmans, T. J., Dahlberg, A., Jirovská, H., Maier, D., Rabbie, J., Torres‐Knoop, A., & Wehner, S. (2023) · npj Quantum Information · doi:10.1038/s41534-023-00765-x · Cited by 38
High speed imaging of spectral-temporal correlations in Hong-Ou-Mandel interference
Zhang, Y., England, D. G., NOMEROTSKI, A., & Sussman, B. (2021) · Optics Express · doi:10.1364/oe.432191 · Cited by 37
Self-citationDigital Discovery of 100 diverse Quantum Experiments with PyTheus
Ruiz-Gonzalez, C., Arlt, S., Petermann, J., Sayyad, S., Jaouni, T., Karimi, E., Tischler, N., Gu, X., & Krenn, M. (2023) · Quantum · doi:10.22331/q-2023-12-12-1204 · Cited by 37
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Ubbelohde, N., Freise, L., Pavlovska, E., Silvestrov, P. G., Recher, P., Kokainis, M., Barinovs, Ğ., Hohls, F., Weimann, T., Pierz, K., et al. (2023) · Nature Nanotechnology · doi:10.1038/s41565-023-01370-x · Cited by 35
Suprano, A., Zia, D., Pont, M., Giordani, T., Rodari, G., Valeri, M., Piccirillo, B., Carvacho, G., Spagnolo, N., Senellart, P., et al. (2023) · Advanced Photonics · doi:10.1117/1.ap.5.4.046008 · Cited by 32
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Jones, A. E., Kumar, S., D’Aurelio, S. E., Bayerbach, M. J., Menssen, A. J., & Barz, S. (2023) · Physical Review A · doi:10.1103/physreva.108.053701 · Cited by 30
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Zhang, J., & Kivshar, Y. S. (2024) · APL Quantum · doi:10.1063/5.0201107 · Cited by 30
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Yousef, K. M. A., D’Alessandro, M., Yeh, M., Sinclair, N. E., Lončar, M., & Capasso, F. (2025) · Science · doi:10.1126/science.adw8404 · Cited by 28
Triggiani, D., Psaroudis, G., & Tamma, V. (2023) · Physical Review Applied · doi:10.1103/physrevapplied.19.044068 · Cited by 27
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Duquennoy, R., Colautti, M., Emadi, R., Majumder, P., Lombardi, P., & Toninelli, C. (2022) · Optica · doi:10.1364/optica.452317 · Cited by 26
Liu, Z.-F., Chen, C., Xu, J.-M., Cheng, Z.-M., Ren, Z., Dong, B.-W., Lou, Y.-C., Yang, Y.-X., Xue, S.-T., Liu, Z.-H., et al. (2022) · Physical Review Letters · doi:10.1103/physrevlett.129.263602 · Cited by 26
Jordan, K. M., Abrahão, R. A., & Lundeen, J. S. (2022) · Physical Review A · doi:10.1103/physreva.106.063715 · Cited by 25
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Multiple Tin-Vacancy Centers in Diamond with Nearly Identical Photon Frequency and Linewidth
Narita, Y., Wang, P., Ikeda, K., Oba, K., Miyamoto, Y., Taniguchi, T., Onoda, S., Hatano, M., & Iwasaki, T. (2023) · Physical Review Applied · doi:10.1103/physrevapplied.19.024061 · Cited by 24
Ru, S., An, M., Yang, Y., Qu, R., Wang, F., Wang, Y., Zhang, P., & Li, F. (2021) · Physical Review A · doi:10.1103/physreva.103.052404 · Cited by 24
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Husel, L., Trapp, J., Scherzer, J., Wu, X., Wang, P., Fortner, J., Nutz, M., Hümmer, T., Polovnikov, B., Förg, M., et al. (2024) · Nature Communications · doi:10.1038/s41467-024-48119-1 · Cited by 23
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Goorney, S., Bley, J., Heusler, S., & Sherson, J. F. (2024) · European Journal of Physics · doi:10.1088/1361-6404/ad7e60 · Cited by 23
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Yu, Y., Seo, I. C., Luo, M., Lu, K., Son, B., Tan, J. K., & Nam, D. (2024) · Nanophotonics · doi:10.1515/nanoph-2024-0050 · Cited by 22
Triggiani, D., & Tamma, V. (2024) · Physical Review Letters · doi:10.1103/physrevlett.132.180802 · Cited by 21
Semi-Device-Independent Characterization of Multiphoton Indistinguishability
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Two-photon interferences of weak coherent lights
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High-speed imaging of spatiotemporal correlations in Hong-Ou-Mandel interference
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Self-citationZhan, X.-H., Zhong, Z.-Q., Wang, S., Yin, Z., Chen, W., He, D., Guo, G., & Han, Z. (2023) · Physical Review Applied · doi:10.1103/physrevapplied.20.034069 · Cited by 17
Massively parallel Hong-Ou-Mandel interference based on independent soliton microcombs
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Spectrally resolved two-photon interference in a modified Hong–Ou–Mandel interferometer
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Engineering Quantum Emitters in 2D Materials
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Fabre, N., Amanti, M. I., Baboux, F., Keller, A., Ducci, S., & Milman, P. (2022) · The European Physical Journal D · doi:10.1140/epjd/s10053-022-00525-0 · Cited by 11
Sgobba, F., Pallotti, D. K., Elefante, A., Russo, S. D., Dequal, D., de Cumis, M. S., & Amato, L. S. (2023) · Photonics · doi:10.3390/photonics10010072 · Cited by 11
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Proppe, A. H., Lee, K. L. K., Kaplan, A. E. K., Ginterseder, M., Krajewska, C. J., & Bawendi, M. G. (2023) · Physical Review Letters · doi:10.1103/physrevlett.131.053603 · Cited by 10
Labay-Mora, A., da Silva, F. F., & Wehner, S. (2024) · Quantum Science and Technology · doi:10.1088/2058-9565/ad57e9 · Cited by 10
Xu, A., Duan, L., Wang, L., & Zhang, Y. (2023) · Optics Express · doi:10.1364/oe.479535 · Cited by 10
Self-citationMultiparameter estimation for qubit states with collective measurements: a case study
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Entanglement-induced collective many-body interference
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Universal Multiport Interferometers for Post‐Selected Multi‐Photon Gates
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Quantum-enhanced microscopic imaging technology [Invited]
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Entanglement engineering of optomechanical systems by reinforcement learning
Ye, L., Arenz, C., Lukens, J. M., & Lai, Y. (2025) · APL Machine Learning · doi:10.1063/5.0233470 · Cited by 9
Space-time propagation of photon pulses in dielectric media, illustrations with beam splitters
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Probing ultra-fast dephasing via entangled photon pairs
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Li, Y., Yu, Y., Lai, K., Han, Y., Gao, F., Zhang, B., & Shvets, G. B. (2022) · Applied Physics Letters · doi:10.1063/5.0083989 · Cited by 8
Li, G., Cheng, W.-C., Wang, Q., & Liu, J. (2023) · Quantum Information Processing · doi:10.1007/s11128-023-04205-9 · Cited by 8
Advantages of the frequency-conversion technique in quantum interference
Yang, C., Niu, S., Zhou, Z., Li, Y., Li, Y., Ge, Z., Gao, M., Han, Z.-Q.-Z., Chen, R., Guo, G., et al. (2022) · Physical Review A · doi:10.1103/physreva.105.063715 · Cited by 8
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Chen, S., Peng, C., Fan, Y., Qiu, X., & Tsai, D. P. (2025) · Light Advanced Manufacturing · doi:10.37188/lam.2025.059 · Cited by 7
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Generation of the complete Bell basis via Hong-Ou-Mandel interference of vector modes
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Self-citationSlepyan, G. Y., Mogilevtsev, D. S., Levie, I., & Boag, A. (2022) · Physical Review Applied · doi:10.1103/physrevapplied.18.014024 · Cited by 7
Liu, Z., Shiu, J., Cheng, C.-Y., & Chen, Y. (2023) · Physical Review A · doi:10.1103/physreva.108.013702 · Cited by 7
Kashi, A. K., Caspani, L., & Kues, M. (2023) · Physical Review Letters · doi:10.1103/physrevlett.131.233601 · Cited by 7
Multi-parameter estimation of the state of two interfering photonic qubits
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Broadband Biphoton Generation and Polarization Splitting in a Monolithic AlGaAs Chip
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Quantum Interference between Nonidentical Single Particles
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Inter-pixel cross-talk as background to two-photon interference effects in SPAD arrays
Kulkov, S., Potuckova, T., Bernasconi, E., Bruschini, C. E., Milanese, T., Edoardo Charbon, A., Shawkat, M. S. A., NOMEROTSKI, A., & Švihra, P. (2024) · Journal of Instrumentation · doi:10.1088/1748-0221/19/12/p12015 · Cited by 6
Characterization of two-particle interference by complementarity
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Li, B., Chen, C., Xiang, X., Quan, R., Dong, R., Zhang, S., Hao, X., & Jin, R. (2023) · Physical Review A · doi:10.1103/physreva.108.023713 · Cited by 6
Attosecond-Level Delay Sensing via Temporal Quantum Erasing
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Quantum kernel evaluation via Hong–Ou–Mandel interference
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Dispersion broadening of the two-photon quantum interference width due to temporal filtering
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Momentum-entangled two-photon interference for quantum-limited transverse-displacement estimation
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Dual views of plasmonics: from near-field optics to electron nanoscopy
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Semiparametric estimation of the Hong-Ou-Mandel profile
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Li, Y., Sun, Z., Li, P., Li, Z., Wang, J., Zhou, L. H., & Ma, H. (2023) · Quantum Information Processing · doi:10.1007/s11128-023-03886-6 · Cited by 6
Singular spectrum analysis of two-photon interference from distinct quantum emitters
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Interference of single photons with ultralong coherence time
Wang, M., Li, Y., Liu, H., Ni, H., Niu, Z., Wei, X. F., Yang, R., & Hu, C. (2024) · Applied Physics Letters · doi:10.1063/5.0217815 · Cited by 5
Pan, F., Bordoloi, P., Chen, C., & Dionne, J. A. (2025) · Nanophotonics · doi:10.1515/nanoph-2025-0196 · Cited by 5
Quantum spectroscopy with biphotons: Lyapunov-based input-output dynamics
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Hong-Ou-Mandel interference with a diode-pumped 1-GHz Ti:sapphire laser
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Quantum entanglement between signal and frequency-up-converted idler photons
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Ogunyemi, O. J., Rani, C., Varnavski, O. P., Wajahath, R., Norscia, M., Malaikal, B., Qiu, Y., Sun, S., Gu, Y., Mukamel, S., et al. (2024) · The Journal of Physical Chemistry C · doi:10.1021/acs.jpcc.4c05907 · Cited by 5
Metadata
- Authors
- Bouchard, F., Sit, A., Zhang, Y., Fickler, R., Miatto, F. M., Yao, Y., Sciarrino, F., & Karimi, E.
- Affiliations
- University of Ottawa (CA)
- National Research Council Canada (CA)
- Télécom Paris (FR)
- Sapienza University of Rome (IT)
- Corresponding author
- Karimi, Ebrahim
- ORCID
- Venue
- Reports on Progress in Physics
- Publisher
- IOP Publishing
- Published
- 2020-12-24
- Volume
- 84
- Issue
- 1
- Pages
- 012402
- ISSN
- 0034-4885 (ISSN-L)
- 1361-6633
- OpenAlex
- W3034980548
- Semantic Scholar
- 93d14a8357b5c60331f7ab0d5939307953fa1e08
- Cited by
- 232
- References
- 257
- Citations by year
- 2026: 48 · 2025: 50 · 2024: 40 · 2023: 51 · 2022: 31 · 2021: 12
- FWCI
- 9.61
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Licence
- Locations
- Reports on Progress in Physics (publishedVersion)
- PubMed (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- NPARC (submittedVersion)
- Figshare (submittedVersion, cc-by)
- arXiv (Cornell University)
- Funders
- Ontario Early Researcher Award
- Canada Research Chairs
- Canada First Research Excellence Fund
- Topics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Information and Cryptography
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Mechanics and Applications
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum optics and atomic interactions
- Keywords
- two-photon interference, Hong-Ou-Mandel interference, two-particle interference, quantum optics, massive particles, electrons, atoms, plasmons, quantum computing, quantum communication, quantum simulation, precision measurement
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