The DOI matches its Crossref record; 16 of the 16 references it cites were found in a registry or an index; none of the 3 sources its claims cite is checked for support yet.
Teleporting an unknown quantum state via dual classical and Einstein-Podolsky-Rosen channels
Open accessAbstract
An unknown quantum state \ensuremath{\Vert}\ensuremath{\varphi}〉 can be disassembled into, then later reconstructed from, purely classical information and purely nonclassical Einstein-Podolsky-Rosen (EPR) correlations. To do so the sender, ``Alice,'' and the receiver, ``Bob,'' must prearrange the sharing of an EPR-correlated pair of particles. Alice makes a joint measurement on her EPR particle and the unknown quantum system, and sends Bob the classical result of this measurement. Knowing this, Bob can convert the state of his EPR particle into an exact replica of the unknown state \ensuremath{\Vert}\ensuremath{\varphi}〉 which Alice destroyed.
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20 Own interpretation · 17 No basis given · 3 Sources not found
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“An unknown quantum state ]P) can be disassembled into, then later reconstructed from, purely classical information and purely nonclassical Einstein-Podolsky-Rosen (EPR) correlations.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“Furthermore, after Alice s measurement, Bob's particle 3 will have been projected into one of the four pure states superposed in Eq. ( 5), according to the measurement outcome.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“Each of these possible resultant states for Bob's EPR particle is related in a simple way to the original state IP) which Alice sought to teleport.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“Thus an accurate teleportation can be achieved in all cases by having Alice tell Bob the classical outcome of her mea- surement, after which Bob applies the required rotation to transform the state of his particle into a replica of IP).”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“It follows that, regardless of the unknown state I/i), the four measurement outcomes are equally likely, each occurring with probability 1/4.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“In the three other cases, Bob must apply one of the unitary operators in Eq. ( 6), corresponding, respectively, to 180' rotations around the z, x, and y axes, in order to”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“Knowing this, Bob can convert the state of his EPR particle into an exact replica of the unknown state ]P) which Alice destroyed.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“Having received these two transmissions, Bob can construct an accurate replica of IP).”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“The teleportation of lg) from Alice to Bob has the side effect of producing two bits of random classical information, uncorrelated to lg), which are left behind at the end of the process.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“Then, after teleportation, particles 0 and 3 would be left in a singlet state, even though they had originally belonged to separate EPR pairs.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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In the paper
“In the case of the first (singlet) outcome, Bob's state is the same except for an irrelevant phase factor, so Bob need do nothing further to produce a replica of Alice's spin.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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In the paper
“Alice makes a joint measurement on her EPR particle and the unknown quantum system, and sends Bob the classical result of this measurement.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“Alice, on the other hand, is left with particles 1 and 2 in one of the states 4~2 ) or IC~~), without any trace of (+) ' (+) the original state I P) .”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“States which are less entangled reduce the fidelity of teleportation, and/or the range of states lg) that can be accurately tele- ported.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“P) will be reconstructed (in the spin-2 case) as a ran- dom mixture of the four states of Eq. ( 6).”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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“It is known that instantaneous information transfer is definitely impossible [3].”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
What the sources say
- Not matchedcites [3] 3. A. Einstein, in Albert Einstein, Philosopher Scientist, - edited by P. A. Schilpp (Library of Living Philosophers, Evanston, 1949) p. 85.
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“This”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
What the sources say
- Not matchedcites [5] 5. J. L. Park, Found. Phys. 1, 23 (1970).
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In the paper
“Finally, teleportation has the advantage of still being possible in situations where Alice and Bob, after sharing their EPR pairs, have wandered about independently and no longer know each others' locations.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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In the paper
“All of what we have said above can be generalized to systems having N & 2 orthogonal states.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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In the paper
“This diagram is of interest because it can be used to show that a full two bits of classical channel capacity are necessary for accurate tele- portation of a two-state particle (cf.caption).”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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In the paper
“Although it is currently unfeasible to store separated EPR particles for more than a brief time, if it becomes feasible to do so, quantum teleportation could be quite useful.”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
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In the paper
“Trying to draw similar”
§ Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels > Abstract
hedgeddirect- Asserted: passes — The authors put it forward as true.
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Probably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
The paper relies on this without support.
If Alice knows beforehand that the unknown state belongs to a given orthonormal set, she can make a measurement whose result will allow her to make an accurate copy.
“Only if Alice knows before- hand that ~qb) belongs to a given orthonormal set can she make a measurement whose result will allow her to make an accurate copy of [P).”
The paper relies on this without support.
If the possibilities for the unknown state include two or more nonorthogonal states, then no measurement will yield sufficient information to prepare a perfectly accurate copy.
“Conversely, if the possibilities for ~P) include two or more nonorthogonal states, then no measurement will yield sufhcient information to prepare a perfectly accurate copy.”
The paper relies on this without support.
In general, there is no way to learn the state vector of an unknown quantum system.
“Knowing the state vector ]P) itself would be sufficient information, but in general there is no way to learn it.”
Claims other papers make about this one
Each is checked against this paper’s own text: does it say what the citing paper says it does?
The cited source says what the claim attributes to it.
In the citing paper
“Quantum teleportation (Bennett et al., 1993) enables a faithful transfer of an unknown quantum state from one location to another, using entangled states as a quantum channel.”
From Multiphoton entanglement and interferometry (2012) · cites this paper as Bennett et al., 1993
The cited source says what the claim attributes to it.
In the citing paper
“The projection of two photons into a Bell state lies at the heart for many quantum information processing protocols, such as quantum dense coding (Bennett and Wiesner, 1992), quantum teleportation (Bennett et al., 1993), and entanglement swapping ( Żukowski et al., 1993).”
From Multiphoton entanglement and interferometry (2012) · cites this paper as Bennett et al., 1993
The cited source says what the claim attributes to it.
In the citing paper
“By exploiting entanglement one can efficiently encode classical messages (Bennett and Wiesner, 1992; section VI.A), transfer quantum information to a remote location (Bennett et al., 1993; section VI.B), entangle two remote particles that have no common past ( Żukowski et al., 1993; section VI.C), and purify a large ensemble in a less entangled states into a smaller ensemble with higher”
From Multiphoton entanglement and interferometry (2012) · cites this paper as Bennett et al., 1993
The cited source says what the claim attributes to it.
In the citing paper
“The fascinating possibility of quantum teleportation was discovered by Bennett, Brassard, Crépeau, Jozsa, Peres, and Wootters (1993).”
From Multiphoton entanglement and interferometry (2012) · cites this paper as Bennett, Brassard, Crépeau, Jozsa, Peres, and Wootters (1993)
The cited source says what the claim attributes to it.
In the citing paper
“This is the case when, as already remarked by Bennett et al. (1993), particle 1 itself is a member of an entangled pair, ultimately leading to entanglement swapping ( Żukowski et al., 1993;Bose et al., 1998).”
From Multiphoton entanglement and interferometry (2012) · cites this paper as Bennett et al. (1993)
The cited source says what the claim attributes to it.
In the citing paper
“Some of the promising quantum communication protocols to expand the possibility of classical data transmission in quantum-based systems include quantum key distribution (QKD) [126,127], quantum teleportation [128] and dense coding [129].”
From Quantum Machine Learning for 6G Communication Networks: State-of-the-Art and Vision for the Future (2019) · cites this paper as [129]
The check wasn’t confident either way, so it gives no verdict — never disputed.
In the citing paper
“To complete the G min gate set so that we can implement arbitrary quantum computations, it suffices to add HAD and preparation of the state | π/ 8 〉 = cos( π/ 8) | 0 〉 + sin( π/ 8) | 1 〉 . 26, 27”
From Quantum computing with realistically noisy devices (2005) · cites this paper as [26]
Experimental — accuracy not yet measuredThe check wasn’t confident either way, so it gives no verdict — never disputed.
In the citing paper
“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].”
From Two-photon interference: the Hong–Ou–Mandel effect (2021) · cites this paper as [107]
Experimental — accuracy not yet measuredIn the citing paper
“Other unique quantum phenomena like 'teleportation' [30] could also be investigated.”
From Two-bit gates are universal for quantum computation (1995) · cites this paper as [30]
In the citing paper
“Since quantum teleportation [14] rests entirely on Bell's Theorem, then this and all research based upon quantum teleportation requires reassessment.”
From EPR Correlations Using Quaternion Spin (2024) · cites this paper as [14]
In the citing paper
“Fortunately, the success probability of the nondeterministic CNOT can be boosted by harnessing quantum teleportation [12]-a process whereby the unknown state of a qubit can be transfered to another qubit.”
From Optical Quantum Computing (2007) · cites this paper as [12]
In the citing paper
“Bennett et al. [1] have suggested that it is possible to transfer the quantum state of a particle onto another particle - the process of quantum teleportation - provided one does not get any information about the state in the course of this transformation.”
From Experimental quantum teleportation (1997) · cites this paper as [1]
In the citing paper
“Quantum physics predicts [1] that once particles 1 and 2 are projected into | ψ -〉 12 , particle 3 is instantaneously projected into the initial state of particle 1.”
From Experimental quantum teleportation (1997) · cites this paper as [1]
In the citing paper
“Although the projection postulate in quantum mechanics seems to bring Alice's attempts to provide Bob with the state | ψ 〉 to a halt, it was realised by Bennett et al. [1] that precisely this projection postulate enables teleportation of | ψ 〉 from Alice to Bob.”
From Experimental quantum teleportation (1997) · cites this paper as [1]
In the citing paper
“It is now well known that the photons produced via the down-conversion process share nonclassical correlations [7].”
From Ultrabright source of polarization-entangled photons (1999) · cites this paper as [7]
In the citing paper
“Using teleportation, an arbitrary unknown qubit can be faithfully transmitted via a pair of maximally-entangled qubits ( e.g. two spin1 2 particles in a pure singlet state) previously shared between sender and receiver, and a 2-bit classical message from the sender to the receiver.”
From Purification of Noisy Entanglement and Faithful Teleportation via Noisy Channels (1996) · cites this paper as [1]
In the citing paper
“While | φ 3 〉 corresponds to a GHZ state of three qubits [7]”
From Persistent Entanglement in Arrays of Interacting Particles (2001) · cites this paper as [7]
In the citing paper
“Be it in quantum computation [1,2], teleportation [3] or quantum cryptography [4], entanglement is viewed as an important resource and, as such, must be quantified.”
From Measures and dynamics of entangled states (2005) · cites this paper as [3]
Citations
Cites
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- C. H. Bennett, 1984, Proceedings of IEEE International Conference on Computers, Systems, and Signal Processing, Bangalore, India
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Long-Distance High-Fidelity Teleportation Using Singlet States
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Driven spin chains as high-quality quantum routers
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Hierarchy of Multipartite Nonlocality and Device-Independent Effect Witnesses
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“Constraints derived under notions of GMNL that disallow entangled measurements will indeed be intimately linked to device-independent certificates of entangled measurements, a crucial tool for teleportation and entanglement swapping protocols in quantum networks [21].”
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“Quantum communication processes, which include quantum teleportation, provide procedures for sending and receiving quantum states of single photons [20].”
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Demonstration of Einstein–Podolsky–Rosen entanglement for an electron in a uniform magnetic field
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Nonclassical properties and Anderson localization of quantum states in coupled waveguides
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Entangling distant systems via universal nonadiabatic passage
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“Remote entangled systems are desired for quantum communication protocols, including quantum teleportation [10], quantum key distribution [11], quantum repeaters [12], quantum secret sharing [13], quantum secure direct communication [14], and quantum secure communication [15].”
Quantum Switch for Continuous Variable Teleportation
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States of the quantized electromagnetic field with highly concentrated phase distribution
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Implementing positive maps with multiple copies of an input state
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Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage
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Fault-Tolerant Coding for Entanglement-Assisted Communication
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“Because of superdense coding [22] and teleportation [23], the classical entanglement-assisted capacity of a channel is exactly double its quantum entanglement-assisted capacity.”
BackgroundEffect of Quantum Noise on the Controlled Remote Preparation via the Brown State
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Two-qubit mixed states and teleportation fidelity: purity, concurrence, and beyond
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N -Qubit W State of Spatially Separated Atoms via Fractional Adiabatic Passage
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Multi-hop teleportation ofN-qubit state via Bell states
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Deterministic multicopy entanglement concentration
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Work extraction and fully entangled fraction
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Photonic Four-qubit Entangled Decoherence-free States Assisted by Cavity-QED System
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Protecting quantum correlations of the XXZ model by topological boundary conditions
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Quantum entanglement in a mixed-spin trimer: Effects of a magnetic field and heterogeneous g factors
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Local invariants for a finite multipartite quantum system
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Visually quantifying single-qubit quantum memory
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“Clearly, quantum information tasks based on entangled resources (i.e., entanglement-based quantum key distribution [9–11], quantum communication [12–15], and quantum teleportation [16–18]) are not functional if there is an entanglement-breaking (EB) quantum memory in the network.”
BackgroundEfficient scheme for remote preparation of arbitrary n-qubit equatorial states
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Quantum decoherence with the Unruh single-particle state having right and left components
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Constructing five qutrit absolutely maximally entangled state via recurrence relation
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Two different efficient controlled quantum teleportation schemes via four-qubit cluster state
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Towards a Deeper Understanding of the Einstein–Podolsky–Rosen Problem
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On teleportation in a system of identical particles
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The Information-Complete Quantum Theory
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Hybrid photonic loss resilient entanglement swapping
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Quantum entanglement and geometry of determinantal varieties
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Cryptanalysis and Improvement of a Quantum Network System of QSS-QDC Using χ-Type Entangled States
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Exploring a Quantum Theory with Graph Rewriting and Computer Algebra
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“Creating large-scale entanglement [3–5] as one of the main tasks of quantum control, is a necessary step toward quantum information processing [6–8], quantum teleportation [9], and one-way quantum computation [10].”
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Parameterized Quantum Circuits for Learning Cooperative Quantum Teleportation
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Tight quantum teleportation without a shared reference frame
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Global quantum correlations in tripartite nonorthogonal states and monogamy properties
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Enhanced Quantum Teleportation between Noninertial Moved Parties by Weak Measurements
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An efficient multiparty quantum secret sharing scheme using a single qudit
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A Remote State Preparation Scheme Initiated and Fixed by a Mentor
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“In particular, in 1993, employing Einstein–Podolsky– Rosen pairs as quantum channel, Bennett et al [19] put forwar-ded a novel concept named as quantum teleportation (QT).”
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On teleportation of a completely unknown state of relativistic photon
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Teleportation of squeezed states in the absence and presence of dissipation
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Multi-hop quantum teleportation with GHZ-class states and Bell states in quantum networks
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Practical Protocol for Telecloning Quantum States
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Generation of NOON states via Raman transitions in a bimodal cavity
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Entanglement and correlation for identical particles in quantum computing
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Unified monogamy relation of entanglement measures
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A useful strong lower bound on two-qubit concurrence
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Metadata
- Authors
- Bennett, C. H., Brassard, G., Crépeau, C., Jozsa, R., Peres, A., & Wootters, W. K.
- Affiliations
- Technion – Israel Institute of Technology (IL)
- Venue
- Physical Review Letters
- Publisher
- American Physical Society (APS)
- Published
- 1993-03-29
- Volume
- 70
- Issue
- 13
- Pages
- 1895-1899
- ISSN
- 0031-9007 (ISSN-L)
- OpenAlex
- W1978553093
- Cited by
- 13,703
- References
- 15
- Citations by year
- 2026: 437 · 2025: 724 · 2024: 696 · 2023: 708 · 2022: 628 · 2021: 640 · 2020: 571 · 2019: 598 · 2018: 477 · 2017: 497 · 2016: 545 · 2015: 500 · 2014: 492 · 2013: 526 · 2012: 492
- FWCI
- 42.66
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Physical Review Letters (publishedVersion)
- PubMed (publishedVersion)
- 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 › Computer Science › Artificial Intelligence › Quantum Computing Algorithms and Architecture
- Keywords
- quantum teleportation, unknown quantum states, Einstein-Podolsky-Rosen correlations, EPR pairs, classical information, joint measurement, quantum state tomography, quantum entanglement
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