Experimental proposal for symmetric minimal two-qubit state tomography
Open accessAbstract
We propose an experiment that realizes a symmetric informationally complete (SIC) probability-operator measurement (POM) in the four-dimensional Hilbert space of a qubit pair. The qubit pair is carried by a single photon as a polarization qubit and a path qubit. The implementation of the SIC POM is accomplished with the means of linear optics. The experimental scheme exploits an approach to SIC POMs that uses a two-step process: a measurement with full-rank outcomes, followed by a projective measurement on a basis that is chosen in accordance with the result of the first measurement. The basis of the first measurement and the four bases of the second measurements are pairwise unbiased---a hint at a possibly profound link between SIC POMs and mutually unbiased bases.
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Written from the paper’s full text.
TL;DR
The paper proposes a linear-optics experiment to realize a symmetric informationally complete (SIC) probability-operator measurement (POM) for a two-qubit system encoded in a single photon’s polarization and path. It uses a two-step measurement scheme whose second bases are mutually unbiased with the first, suggesting a structural link between SIC POMs and mutually unbiased bases.
Key findings
The proposal implements the four-dimensional SIC POM as two successive measurements with \(d=4\) outcomes each, yielding \(d^2=16\) overall outcomes \(P_{n,m}=A_n^\dagger B_m^{(n)}A_n\). The first measurement is a POM diagonal in the computational basis with Kraus operators \(A_k\), and the second is a projective measurement in one of four mutually unbiased bases \(B_k\), chosen according to the first outcome. The paper reports that the SIC POM for the qubit pair corresponds to this construction and that the fiducial vectors in dimension 4 have a structural relation to the MUB vectors. Specific optical parameters are given, including \(N=\sqrt{5+\sqrt5}\), \(\chi=\sqrt{2+\sqrt5}\), beam-splitter reflection coefficients \(r_1=1/N\), \(r_2=1/\sqrt{N^2-1}\), and PPBS amplitude coefficient \(y=1/\sqrt{N^2-2}\).
Methods
The work is a theoretical experimental proposal, not an experiment; it designs an optical implementation using passive linear elements: half-wave plates, beam splitters, phase shifters, partially polarizing beam splitters, polarizing beam splitters, and photodetectors. The two qubits are encoded in a single photon as a polarization qubit (vertical/horizontal) and a path qubit (left/right). The first measurement is realized by beam splitters and PPBSs configured to implement the Kraus operators \(A_k\); the second measurement applies a unitary \(U_k\) that transforms basis \(B_k\) into the computational basis, followed by PBSs and photodetectors. The paper analyzes the SIC POM construction in \(d=4\), identifies the \(A\)s as Kraus operators, and shows the operations transform the computational basis into the MUB.
Limitations
The paper states that practical implementation of the qubit scheme in Fig. 1 requires stabilization of the interferometer loop defined by four beam splitters, and that for the two-qubit proposal the unitaries \(U_3\) and \(U_4\) require PPBSs together with a Mach-Zehnder interferometer. It also states that there is no systematic procedure for implementing SIC POMs in higher dimensions in a simple experimental setup, and that generalizing this scheme to higher dimensions is left as an open question. Evident from the text: this is a proposal only, with no experimental data, error analysis, or demonstrated implementation reported.
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Claims the paper makes
7 of 8 cited sources checked · 7 supported · 0 flagged
- Premisecitation§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
All experiments and proposals for experiments implementing SIC POMs up to date have been limited to the two-level system (qubit), with the exception of one where a SIC POM for a three-level system was approximated.
“In contrast to the major theoretical progress, up to date, all experiments and even proposals for experiments implementing SIC POMs have been limited to the very basic quantum system, the two-level system (qubit) [10, 11], with the exception of [12] where a SIC POM for a three-level system was approximated.”
Quote in the paperSubstantial claim2 of 3 sources checked- cites [10] source
- cites [11] W.M. Pimenta, B. Marques, M.A. Carvalho, M.R. Barros, J.G. Fonseca, J. Ferraz, M. Terra Cunha, and S. P´ adua, Opt. Express 18 , 24423 (2010). source
- cites [12] Z.E.D. Medendorp, F.A. Torres-Ruiz, L.K. Shalm, G.N.M. Tabia, C.A. Fuchs, and A.M. Steinberg, Phys. Rev. A 83 , 051801(R) (2011). source
- Premisecitation§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The qubit pair is carried by a single photon as a polarization qubit and a path qubit.
“The qubit pair is carried by a single photon as a polarization qubit and a path qubit.”
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 3 · plain
“Our proposal is based on the methods of [15] where the two qubits, a polarization qubit and a path qubit, are encoded in a single photon.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites [15] B.-G. Englert, C. Kurtsiefer, and H. Weinfurter, Phys. Rev. A 63 , 032303 (2001). source
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 3 · plain
- Premisecitation§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 2
The SIC POM in dimension 4 is composed of 16 subnormalized projectors onto 16 fiducial kets.
“This SIC POM is composed of 16 subnormalized projectors onto 16 (fiducial) kets.”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites [16] I. Bengtsson, J. Phys.: Conf. Ser. 254 , 012007 (2010). source
- Premisecitation§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The experimental scheme uses a two-step process that breaks the SIC POM into two successive measurements, each with d outcomes: a measurement with full-rank outcomes, followed by a projective measurement on a basis chosen in accordance with the result of the first measurement.
“The experimental scheme exploits a new approach to SIC POMs that uses a two-step process: a measurement with full-rank outcomes, followed by a projective measurement on a basis that is chosen in accordance with the result of the first measurement.”
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 1 · hedged
“In this approach, we 'break' the SIC POM into two successive measurements, each with d outcomes, with the intention that each measurement would be relatively easy to implement.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites [13] source
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 1 · hedged
- Premisecitation§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The proposal exploits a new theoretical approach for constructing SIC POMs.
“The proposal exploits a new theoretical approach for constructing SIC POMs [13].”
Quote in the paperSubstantial claim1 of 1 sources checked- cites [13] source
- Findingown data§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 4
The SIC POM for the qubit pair corresponds to a POM diagonal in the computational basis, followed by projections onto bases which are mutually unbiased.
“We found that the SIC POM for the qubit pair corresponds to a POM diagonal in the computational basis, followed by projections onto bases which are mutually unbiased.”
Quote in the paperSubstantial claim - Findingown data§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The two successive measurements that make up the SIC POM in dimension 4 have a strikingly simple form.
“Unexpectedly, we find that the two successive measurements that make up the SIC POM in dimension 4, not only have a strikingly simple form, but also hint at a close relation between the structure of mutually unbiased bases (MUB) and that of the SIC POM”
Quote in the paperSubstantial claim - Findingreasoning§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 4
The unitary transformations U1 and U2 can be decomposed into a tensor product of two unitary transformations, one for the path qubit and one for the polarization qubit.
“We see that the unitary transformation U 1 and U 2 can be decomposed into a tensor product of two uni-”
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
“tary transformations, one for the path qubit and one for the polarization qubit.”
Quote in the paperNot a substantial claim - Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
- Findingnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 2
Each of the matrices of fiducial vectors can be written as a diagonal matrix times a unitary matrix.
“Each of these matrices could be written as a diagonal matrix times a unitary matrix.”
Quote in the paperSubstantial claim - Findingnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 2
The operations of Eq. (3) transform the computational basis into the MUB.
“Actually, the operations of Eq. (3) transform the computational basis into the MUB,”
Quote in the paperSubstantial claim - Findingnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The basis of the first measurement and the four bases of the second measurements are pairwise unbiased.
“The basis of the first measurement and the four bases of the second measurements are pairwise unbiased - a hint at a possibly profound link between SIC POMs and mutually unbiased bases.”
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
“We found that the SIC POM for the qubit pair corresponds to a POM diagonal in the computational basis, followed by projections onto bases which are mutually unbiased.”
Quote in the paperSubstantial claim - Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
- Interpretationown data§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The two successive measurements that make up the SIC POM in dimension 4 hint at a close relation between the structure of mutually unbiased bases (MUB) and that of the SIC POM.
“Unexpectedly, we find that the two successive measurements that make up the SIC POM in dimension 4, not only have a strikingly simple form, but also hint at a close relation between the structure of mutually unbiased bases (MUB) and that of the SIC POM”
Quote in the paperNot a substantial claim - Interpretationnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
There is no systematic procedure for implementing SIC POMs in higher dimensions in a simple experimental set-up.
“This is, in part, due to the fact that there is no systematic procedure for implementing SIC POMs in higher dimensions, in a simple experimental set-up.”
Quote in the paperSubstantial claim - Interpretationreasoning§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 3
The structure of fiducial vectors in Eq. (1) allows implementation of the SIC POM by two successive measurements: a measurement whose Kraus operators are given in Eq. (2), and depending on the measurement outcome, a measurement in one of the MUB of Eq. (4).
“The structure of fiducial vectors in Eq. (1) (which form the SIC POM in dimension 4) allows us to implement the SIC POM by two successive measurements: A measurement whose Kraus operators are given in Eq. (2), and depending on the measurement outcome, a measurement in one of the MUB of Eq. (4).”
Quote in the paperSubstantial claim - Interpretationreasoning§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The proposed experiment realizes a symmetric informationally complete (SIC) probability-operator measurement (POM) in the four-dimensional Hilbert space of a qubit pair.
“We propose an experiment that realizes a symmetric informationally complete (SIC) probabilityoperator measurement (POM) in the four-dimensional Hilbert space of a qubit pair.”
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
“To conclude, we are proposing a feasible experimental scheme that implements the SIC POM for a twoqubit system.”
Quote in the paperSubstantial claim - Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
- Interpretationreasoning§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 3
The settings of the optical elements ensure that the measurement of Eq. (2) is realized.
“These settings ensure that the measurement of Eq. (2) is realized.”
Quote in the paperSubstantial claim - Interpretationreasoning§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The experiment is feasible with current technology.
“The experiment is clearly feasible with current technology.”
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · boosted
“Our scheme uses linear optical elements and photodetectors, and is, therefore, well within the reach of existing technology.”
Quote in the paperSubstantial claim - Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · boosted
- Interpretationnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 1
The implementation of the SIC POM is accomplished with the means of linear optics.
“The implementation of the SIC POM is accomplished with the means of linear optics.”
- Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
“Our scheme uses linear optical elements and photodetectors, and is, therefore, well within the reach of existing technology.”
Quote in the paperSubstantial claim - Also stated in: § Experimental proposal for symmetric minimal two-qubit state tomography · p. 4 · plain
- Classified as probably not a substantial claim. 4
- May combine two claims. 3
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Premisecitation§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 2In dimension 4, there is only one known SIC POM, and all other known SIC POMs are unitarily equivalent to it.
“In dimension 4, there is only one known SIC POM, and all the other known SIC POMs are unitarily equivalent to it [6].”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites [6] source
May combine two claims.
Findingnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 3The bases B1 and B2 are composed of product states, while the bases B3 and B4 consist of maximally entangled states.
“The bases B 1 and B 2 are composed of product states, while the bases B 3 and B 4 consist of maximally entangled states.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Findingnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 2The set of bases corresponding to each unitary matrix, together with the computational basis, form the complete set of MUB in dimension 4.
“The set of bases, corresponding to each unitary matrix, together with the computational basis, form the complete set of MUB in dimension 4.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based). May combine two claims.
Interpretationnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 4The unitary transformations U3 and U4 are not of that kind and could be realized by using PPBSs together with a Mach-Zehnder interferometer.
“The unitary transformation U 3 and U 4 are not of that kind and could be realized, for example, by using PPBSs together with a Mach-Zehnder interferometer.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone given§ Experimental proposal for symmetric minimal two-qubit state tomography · p. 4This unique construction is owed to a structural relation between the fiducial vectors and the MUB vectors in dimension 4.
“We observed that this unique construction is owed to a structural relation between the fiducial vectors and the MUB vectors in dimension 4.”
Quote in the paperNot a substantial claim
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 same unitaries are assigned opposite basis transformations
MinorThe paper says the operations of Eq. (3) transform the computational basis into the mutually unbiased bases. The measurement instructions instead apply those same operations to transform those bases into the computational basis; that step would generally require the inverse unitaries.
“Actually, the operations of Eq. (3) transform the computational basis into the MUB,”
“we first apply a unitary operation U k of Eq. (3) that transforms the basis B k into the computational basis and then measure in the computational basis”
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Self-citation
Flagged first, then by citations
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Cited by
Sorted by citations
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Self-citation
- Authors
- Kalev, A., Shang, J., & Englert, B.-G.
- Affiliations
- Centre for Quantum Technologies (SG)
- Venue
- Physical Review A
- Publisher
- American Physical Society (APS)
- Published
- 2012-05-17
- Volume
- 85
- Issue
- 5
- ISSN
- 0556-2791 (ISSN-L)
- 1050-2947
- 1094-1622
- OpenAlex
- W2011594711
- Semantic Scholar
- f0dcabbc3d127c191b342202848a0ea5879098eb
- Cited by
- 13
- References
- 17
- Citations by year
- 2020: 1 · 2018: 2 · 2017: 2 · 2015: 2 · 2014: 1 · 2013: 4 · 2012: 1
- FWCI
- 2.52
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Physical Review A (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- National University of Singapore (submittedVersion)
- arXiv (Cornell University)
- Topics
- Physical Sciences › Computer Science › Artificial Intelligence › 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
- symmetric informationally complete measurements, qubit pairs, polarization qubits, linear optics, mutually unbiased bases, quantum state tomography
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