Quantifying Information Extraction using Generalized Quantum Measurements
Abstract: Observational entropy is interpreted as the uncertainty an observer making measurements associates with a system. So far, properties that make such an interpretation possible rely on the assumption of ideal projective measurements. We show that the same properties hold even when considering generalized measurements. Thus, the interpretation still holds: Observational entropy is a well-defined quantifier determining how influential a given series of measurements is in information extraction. This generalized framework allows for the study of the performance of indirect measurement schemes, which are those using a probe. Using this framework, we first analyze the limitations of a finite-dimensional probe. Then we study several scenarios of the von Neumann measurement scheme, in which the probe is a classical particle characterized by its position. Finally, we discuss observational entropy as a tool for quantum state inference. Further developed, this framework could find applications in quantum information processing. For example, it could help in determining the best read-out procedures from quantum memories and to provide adaptive measurement strategies alternative to quantum state tomography.
- R. Y. Rubinstein and D. P. Kroese, The cross-entropy method: a unified approach to combinatorial optimization, Monte-Carlo simulation and machine learning (Springer Science & Business Media, 2013).
- R. Clausius, The Mechanical Theory of Heat: With Its Applications to the Steam-engine and to the Physical Properties of Bodies (J. Van Voorst, 1867).
- J. Dunkel and S. Hilbert, Nat. Phys. 10, 67 (2014).
- E. T. Jaynes, Am. J. Phys. 33, 391 (1965).
- C. E. Shannon, The Bell system technical journal 27, 379 (1948).
- J. von Neumann, Nachrichten von der Gesellschaft der Wissenschaften zu Göttingen, Mathematisch-Physikalische Klasse 1927, 273 (1927a).
- H. M. Wiseman and J. A. Vaccaro, Phys. Rev. Lett. 91, 097902 (2003).
- M. B. Plenio and S. S. Virmani, “An introduction to entanglement theory,” in Quantum information and coherence (Springer, 2011) p. 173.
- L. Boltzmann, in The kinetic theory of gases: an anthology of classic papers with historical commentary (World Scientific, Hackensack, 2003) p. 262.
- S. Goldstein and J. L. Lebowitz, Physica D 193, 53 (2004).
- J. von Neumann, The European Physical Journal H 35, 201 (2010a), https://arxiv.org/abs/1003.2133 .
- A. Wehrl, Rev. Mod. Phys. 50, 221 (1978).
- J. Gemmer and R. Steinigeweg, Phys. Rev. E 89, 042113 (2014).
- N. Engelhardt and A. C. Wall, J. High Energy Phys. 2019, 160 (2019).
- J. D. Farmer, Zeitschrift für Naturforschung A 37, 1304 (1982).
- V. Latora and M. Baranger, Phys. Rev. Lett. 82, 520 (1999).
- R. Frigg, Brit. J. Phil. Sc. 55, 411 (2004).
- J. Jost, Dynamical systems: examples of complex behaviour (Springer Science & Business Media, 2006).
- Thermodynamic entropies encode information about the energy eigenstate (microstate) of the system due to an increase in energy. Whereas, information-theoretic entropies capture details about the state of the system due to its interaction with an external system.
- R. Uzdin and S. Rahav, PRX Quantum 2, 010336 (2021).
- F. Anzà and V. Vedral, Sci. Rep. 7, 44066 (2017).
- C. S. Lent, Phys. Rev. E 100, 012101 (2019).
- K. Yoshida, Phys. Rev. A 101, 032110 (2020).
- H.-J. Schmidt and J. Gemmer, Zeitschrift Naturforschung Teil A 75, 265 (2020).
- P. Strasberg and A. Winter, PRX Quantum 2, 030202 (2021).
- J. Thingna and P. Talkner, Phys. Rev. A 102, 012213 (2020).
- J. von Neumann, “Mathematical foundations of quantum mechanics,” (Princeton university press, 1955) p. 410.
- D. Biggerstaff, Experiments with generalized quantum measurements and entangled photon pairs, Master’s thesis, University of Waterloo (2009).
- Operators Π^i=\sum@\slimits@mK^im†K^imsubscript^Π𝑖\sum@subscript\slimits@𝑚superscriptsubscript^𝐾𝑖𝑚†subscript^𝐾𝑖𝑚{\hat{\Pi}}_{i}=\sum@\slimits@_{m}\hat{K}_{im}^{\dagger}\hat{K}_{im}over^ start_ARG roman_Π end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT = start_POSTSUBSCRIPT italic_m end_POSTSUBSCRIPT over^ start_ARG italic_K end_ARG start_POSTSUBSCRIPT italic_i italic_m end_POSTSUBSCRIPT start_POSTSUPERSCRIPT † end_POSTSUPERSCRIPT over^ start_ARG italic_K end_ARG start_POSTSUBSCRIPT italic_i italic_m end_POSTSUBSCRIPT are called POVM elements. Their collection {Π^i}subscript^Π𝑖\{{\hat{\Pi}}_{i}\}{ over^ start_ARG roman_Π end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT } a POVM (positive operator-valued measure) in the literature. Unlike the general measurement given by {𝒜i}subscript𝒜𝑖\{{\mathcal{A}}_{i}\}{ caligraphic_A start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT }, POVM by itself cannot determine the post-measurement state Kraus et al. (1983).
- Number of m𝑚mitalic_m for each i𝑖iitalic_i in decomposition (5\@@italiccorr) is not unique, and the number of m𝑚mitalic_m for each i𝑖iitalic_i can vary. Minimal number of m𝑚mitalic_m such that the decomposition holds is called the Kraus rank of 𝒜isubscript𝒜𝑖{\mathcal{A}}_{i}caligraphic_A start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT. Projective measurements are a special type of Kraus rank-1 measurements defined by 𝒜i(X^)≡P^iX^P^isubscript𝒜𝑖^𝑋subscript^𝑃𝑖^𝑋subscript^𝑃𝑖{\mathcal{A}}_{i}(\hat{X})\equiv\hat{P}_{i}\hat{X}\hat{P}_{i}caligraphic_A start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT ( over^ start_ARG italic_X end_ARG ) ≡ over^ start_ARG italic_P end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT over^ start_ARG italic_X end_ARG over^ start_ARG italic_P end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT.
- By 𝒞={P^i(∙)P^i}𝒞subscript^𝑃𝑖∙subscript^𝑃𝑖{\mathcal{C}}=\{\hat{P}_{i}(\bullet)\hat{P}_{i}\}caligraphic_C = { over^ start_ARG italic_P end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT ( ∙ ) over^ start_ARG italic_P end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT } we mean that 𝒞={𝒜i}𝒞subscript𝒜𝑖{\mathcal{C}}=\{{\mathcal{A}}_{i}\}caligraphic_C = { caligraphic_A start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT }, where 𝒜i(X^)=P^iX^P^isubscript𝒜𝑖^𝑋subscript^𝑃𝑖^𝑋subscript^𝑃𝑖{\mathcal{A}}_{i}(\hat{X})=\hat{P}_{i}\hat{X}\hat{P}_{i}caligraphic_A start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT ( over^ start_ARG italic_X end_ARG ) = over^ start_ARG italic_P end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT over^ start_ARG italic_X end_ARG over^ start_ARG italic_P end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT for an operator X^^𝑋\hat{X}over^ start_ARG italic_X end_ARG.
- J.-P. Pellonpää and M. Tukiainen, Rep. Math. Phys. 79, 261 (2017).
- This corresponds to the system coarse-graining 𝒞={trB[(I^⊗|m⟩⟨m|)U^(∙⊗σ^)U^†(I^⊗|m⟩⟨m|)]}{\mathcal{C}}=\{\mathrm{tr}_{B}[({\hat{I}}\otimes|m\rangle\langle m|){\hat{U}}% (\bullet\otimes{\hat{\sigma}}){\hat{U}}^{\dagger}({\hat{I}}\otimes|m\rangle% \langle m|)]\}caligraphic_C = { roman_tr start_POSTSUBSCRIPT italic_B end_POSTSUBSCRIPT [ ( over^ start_ARG italic_I end_ARG ⊗ | italic_m ⟩ ⟨ italic_m | ) over^ start_ARG italic_U end_ARG ( ∙ ⊗ over^ start_ARG italic_σ end_ARG ) over^ start_ARG italic_U end_ARG start_POSTSUPERSCRIPT † end_POSTSUPERSCRIPT ( over^ start_ARG italic_I end_ARG ⊗ | italic_m ⟩ ⟨ italic_m | ) ] }.
- M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information: 10th Anniversary Edition (Cambridge University Press, 2010).
- S. S. Straupe, Soviet Journal of Experimental and Theoretical Physics Letters 104, 510 (2016), arXiv:1610.02840 [quant-ph] .
- S. Vinjanampathy and J. Anders, Cont. Phys. 57, 545 (2016).
- J. von Neumann, Eur. Phys. J. H 35, 201 (2010b).
- J. von Neumann, Nachrichten von der Gesellschaft der Wissenschaften zu Göttingen, Mathematisch-Physikalische Klasse 1927, 273 (1927b).
- E. Sheridan, arXiv:2007.06673 (2020).
- I. C. Percival, J. Math. Phys. 2, 235 (1961).
- R. C. Tolman, The principles of statistical mechanics (Courier Corporation, 1979).
- O. Penrose, Rep. Prog. Phys. 42, 1937 (1979).
- M. Nauenberg, Am. J. Phys. 72, 313 (2004).
- M. Ohya and D. Petz, Quantum entropy and its use (Springer Science & Business Media, 2004).
- J. L. W. V. Jensen, Acta mathematica 30, 175 (1906).
- T. Needham, The American mathematical monthly 100, 768 (1993).
- L. N. Trefethen and J. Weideman, siam REVIEW 56, 385 (2014).
- M. G. Mayer, J. H. D. Jensen, and E. Wigner, “The Nobel Prize in Physics 1963,” (1963).
Paper Prompts
Sign up for free to create and run prompts on this paper using GPT-5.
Top Community Prompts
Collections
Sign up for free to add this paper to one or more collections.