Teaching ideal quantum measurement, from dynamics to interpretation

We present a graduate course on ideal measurements, analyzed as dynamical processes of interaction between the tested system S and an apparatus A, described by quantum statistical mechanics. The apparatus A = M + B involves a macroscopic measuring device M and a bath B. The requirements for ideality...

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Main Authors: Allahverdyan, Armen E., Balian, Roger, Nieuwenhuizen, Theo M.
Format: Article
Language:English
Published: Académie des sciences 2024-05-01
Series:Comptes Rendus. Physique
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Online Access:https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.180/
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author Allahverdyan, Armen E.
Balian, Roger
Nieuwenhuizen, Theo M.
author_facet Allahverdyan, Armen E.
Balian, Roger
Nieuwenhuizen, Theo M.
author_sort Allahverdyan, Armen E.
collection DOAJ
description We present a graduate course on ideal measurements, analyzed as dynamical processes of interaction between the tested system S and an apparatus A, described by quantum statistical mechanics. The apparatus A = M + B involves a macroscopic measuring device M and a bath B. The requirements for ideality of the measurement allow us to specify the Hamiltonian of the isolated compound system S + M + B. The resulting dynamical equations may be solved for simple models. Conservation laws are shown to entail two independent relaxation mechanisms: truncation and registration. Approximations, justified by the large size of M and of B, are needed. The final density matrix $\hat{\mathcal{D}}$(tf) of S + A has an equilibrium form. It describes globally the outcome of a large set of runs of the measurement. The measurement problem, i.e., extracting physical properties of individual runs from $\hat{\mathcal{D}}$(tf), then arises due to the ambiguity of its splitting into parts associated with subsets of runs. To deal with this ambiguity, we postulate that each run ends up with a distinct pointer value Ai of the macroscopic M. This is compatible with the principles of quantum mechanics. Born’s rule then arises from the conservation law for the tested observable; it expresses the frequency of occurrence of the final indications Ai of M in terms of the initial state of S. Von Neumann’s reduction amounts to updating of information due to selection of Ai. We advocate the terms q-probabilities and q-correlations when analyzing measurements of non-commuting observables. These ideas may be adapted to different types of courses.
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spelling doaj-art-39d734564aa64385810f3e270d0bd4d72025-02-07T13:53:46ZengAcadémie des sciencesComptes Rendus. Physique1878-15352024-05-0125G125128710.5802/crphys.18010.5802/crphys.180Teaching ideal quantum measurement, from dynamics to interpretationAllahverdyan, Armen E.0Balian, Roger1Nieuwenhuizen, Theo M.2Yerevan Physics Institute, Alikhanian Brothers Street 2, Yerevan 375036, ArmeniaInstitut de Physique Théorique, CEA Saclay, 91191 Gif-sur-Yvette cedex, FranceInstitute for Theoretical Physics, Science Park 904, 1098 XH Amsterdam, The NetherlandsWe present a graduate course on ideal measurements, analyzed as dynamical processes of interaction between the tested system S and an apparatus A, described by quantum statistical mechanics. The apparatus A = M + B involves a macroscopic measuring device M and a bath B. The requirements for ideality of the measurement allow us to specify the Hamiltonian of the isolated compound system S + M + B. The resulting dynamical equations may be solved for simple models. Conservation laws are shown to entail two independent relaxation mechanisms: truncation and registration. Approximations, justified by the large size of M and of B, are needed. The final density matrix $\hat{\mathcal{D}}$(tf) of S + A has an equilibrium form. It describes globally the outcome of a large set of runs of the measurement. The measurement problem, i.e., extracting physical properties of individual runs from $\hat{\mathcal{D}}$(tf), then arises due to the ambiguity of its splitting into parts associated with subsets of runs. To deal with this ambiguity, we postulate that each run ends up with a distinct pointer value Ai of the macroscopic M. This is compatible with the principles of quantum mechanics. Born’s rule then arises from the conservation law for the tested observable; it expresses the frequency of occurrence of the final indications Ai of M in terms of the initial state of S. Von Neumann’s reduction amounts to updating of information due to selection of Ai. We advocate the terms q-probabilities and q-correlations when analyzing measurements of non-commuting observables. These ideas may be adapted to different types of courses.https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.180/ideal quantum measurements<i>q</i>-probabilitysystem-apparatus dynamicsmeasurement problemBorn rulevon Neumann reductionminimalist interpretationcontextuality
spellingShingle Allahverdyan, Armen E.
Balian, Roger
Nieuwenhuizen, Theo M.
Teaching ideal quantum measurement, from dynamics to interpretation
Comptes Rendus. Physique
ideal quantum measurements
<i>q</i>-probability
system-apparatus dynamics
measurement problem
Born rule
von Neumann reduction
minimalist interpretation
contextuality
title Teaching ideal quantum measurement, from dynamics to interpretation
title_full Teaching ideal quantum measurement, from dynamics to interpretation
title_fullStr Teaching ideal quantum measurement, from dynamics to interpretation
title_full_unstemmed Teaching ideal quantum measurement, from dynamics to interpretation
title_short Teaching ideal quantum measurement, from dynamics to interpretation
title_sort teaching ideal quantum measurement from dynamics to interpretation
topic ideal quantum measurements
<i>q</i>-probability
system-apparatus dynamics
measurement problem
Born rule
von Neumann reduction
minimalist interpretation
contextuality
url https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.180/
work_keys_str_mv AT allahverdyanarmene teachingidealquantummeasurementfromdynamicstointerpretation
AT balianroger teachingidealquantummeasurementfromdynamicstointerpretation
AT nieuwenhuizentheom teachingidealquantummeasurementfromdynamicstointerpretation