Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Springer eBooks

Measurement Theory with Instruments Treated Partially Quantum Mechanically

Franklin E. Schroeck

Published Jan 1, 1981• 2 citations
Publisher
DOI
10.1007/978-1-4613-3258-9_34

Related papers

Quantum measurement beyond projection: POVMs, instruments, dilation theorems, ancilla-assisted partial measurement, and operational trade-offs

Sachin .

The projection postulate and spectral representation of observables remain central in quantum theory but describe only an idealized measurement limit. Realistic measurements may be inefficient, unsharp, weak, indirect, adaptive, destructive, or informationally incomplete. Positive-operator-valued measures (POVMs) provide the probability rule for processes, whereas quantum instruments specify state transformation. This review traces the hierarchy from von Neumann projective measurement to generalized measurement, emphasizing distinctions among effects, instruments, channels, and implementations. Naimark dilation realizes arbitrary POVMs through unitary coupling to an ancillary meter and projective readout. Stinespring dilation represents completely positive trace-preserving dynamics by unitary evolution on an enlarged system followed by partial trace. A qubit–ancilla interaction yields a partial-measurement instrument, its POVM effects, and its information–disturbance trade-off. It compares projective, generalized, and ancilla-mediated schemes; examines compatibility, instrument incompatibility, and disturbance; and surveys applications to state discrimination, tomography, control, and error correction. Recent developments in dynamic-circuit measurements and noisy-POVM compatibility are integrated with questions concerning measurement back-action and outcome definiteness. The review stresses that a POVM does not uniquely determine state update, dilation theorems establish realizability rather than unique mechanisms, and operational measurement theory does not settle definite outcomes, arguing quantum instruments provide a complete description of measurement.

International Journal of Physics and Applications•Jul 1, 2025•0 citations

Quantum measurement theory

Howard M. Wiseman, Gerard J Milburn

Cambridge University Press eBooks•Nov 12, 2009•2 citations

Quantum Theory of Measurement: A Non-Quantum Mechanical Approach

Gen-Ichiro Nagasaka

Boston studies in the philosophy of science•Jan 1, 1984•0 citations

Black Hole Information Loss and Quantum Measurement Collapse as the Same Admissibility Transition in Modal Triplet Theory

Peter Nero

This paper develops a rigorous Modal Triplet Theory language for projected information, effective dynamics, and restricted recovery. An autonomous projected map exists exactly when the upper evolution preserves projection fibers; it is invertible exactly when the fiber equivalence is preserved in both time directions. Fiber splitting, effective merger, and restricted recovery are therefore distinct mechanisms. Quantum measurement is treated as an ordinary physical instrument followed by retention or loss of a record. Black-hole exterior restriction is a separate physical channel whose identification with an MTT admissibility boundary remains a model assumption. Island and entanglement-wedge results are represented by recovery on a code subspace or observable algebra, not by a partial right inverse between different state spaces. No common origin for Born and Hawking weights is claimed without an explicit measure and both pushforwards. The surviving MTT result is a rigorous language for projected information and recovery, together with a falsifiable source contract; it is not yet a solution of either the measurement problem or the black-hole information problem.

•Jan 15, 2026•0 citations

Postprocessing of quantum instruments

Leevi Leppäjärvi, Michal Sedlák

Studying sequential measurements is of the utmost importance to both the foundational aspects of quantum theory and the practical implementations of quantum technologies, with both of these applications being abstractly described by the concatenation of quantum instruments into a sequence of a certain length. In general, the choice of instrument at any given step in the sequence can be conditionally chosen based on the classical results of all preceding instruments. For two instruments in a sequence we consider the conditional second instrument as an effective way of postprocessing the first instrument into a new one. This is similar to how a measurement described by a positive operator-valued measure (POVM) can be postprocessed into another by way of classical randomization of its outcomes using a stochastic matrix. In this work we study the postprocessing relation of instruments and the partial order it induces on their equivalence classes. We characterize the greatest and the least element of this order, give examples of postprocessings between different types of instruments, and draw connections between postprocessings of some of these instruments and their induced POVMs.

arXiv:2010.15816•Physical Review A•Feb 25, 2021•13 citations

Quantum Measurement Theory

János A. Bergou, Mark S. Hillery

Graduate texts in physics•Jan 1, 2013•6 citations
The projection postulate and spectral representation of observables remain central in quantum theory but describe only an idealized measurement limit. Realistic measurements may be inefficient, unsharp, weak, indirect, adaptive, destructive, or informationally incomplete. Positive-operator-valued measures (POVMs) provide the probability rule for processes, whereas quantum instruments specify state transformation. This review traces the hierarchy from von Neumann projective measurement to generalized measurement, emphasizing distinctions among effects, instruments, channels, and implementations. Naimark dilation realizes arbitrary POVMs through unitary coupling to an ancillary meter and projective readout. Stinespring dilation represents completely positive trace-preserving dynamics by unitary evolution on an enlarged system followed by partial trace. A qubit–ancilla interaction yields a partial-measurement instrument, its POVM effects, and its information–disturbance trade-off. It compares projective, generalized, and ancilla-mediated schemes; examines compatibility, instrument incompatibility, and disturbance; and surveys applications to state discrimination, tomography, control, and error correction. Recent developments in dynamic-circuit measurements and noisy-POVM compatibility are integrated with questions concerning measurement back-action and outcome definiteness. The review stresses that a POVM does not uniquely determine state update, dilation theorems establish realizability rather than unique mechanisms, and operational measurement theory does not settle definite outcomes, arguing quantum instruments provide a complete description of measurement.
This paper develops a rigorous Modal Triplet Theory language for projected information, effective dynamics, and restricted recovery. An autonomous projected map exists exactly when the upper evolution preserves projection fibers; it is invertible exactly when the fiber equivalence is preserved in both time directions. Fiber splitting, effective merger, and restricted recovery are therefore distinct mechanisms. Quantum measurement is treated as an ordinary physical instrument followed by retention or loss of a record. Black-hole exterior restriction is a separate physical channel whose identification with an MTT admissibility boundary remains a model assumption. Island and entanglement-wedge results are represented by recovery on a code subspace or observable algebra, not by a partial right inverse between different state spaces. No common origin for Born and Hawking weights is claimed without an explicit measure and both pushforwards. The surviving MTT result is a rigorous language for projected information and recovery, together with a falsifiable source contract; it is not yet a solution of either the measurement problem or the black-hole information problem.
Studying sequential measurements is of the utmost importance to both the foundational aspects of quantum theory and the practical implementations of quantum technologies, with both of these applications being abstractly described by the concatenation of quantum instruments into a sequence of a certain length. In general, the choice of instrument at any given step in the sequence can be conditionally chosen based on the classical results of all preceding instruments. For two instruments in a sequence we consider the conditional second instrument as an effective way of postprocessing the first instrument into a new one. This is similar to how a measurement described by a positive operator-valued measure (POVM) can be postprocessed into another by way of classical randomization of its outcomes using a stochastic matrix. In this work we study the postprocessing relation of instruments and the partial order it induces on their equivalence classes. We characterize the greatest and the least element of this order, give examples of postprocessings between different types of instruments, and draw connections between postprocessings of some of these instruments and their induced POVMs.