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

Cambridge University Press eBooks

States and Observables

Jan van Neerven

Published Jun 22, 2022• 0 citations
Publisher
DOI
10.1017/9781009232487.017

Related papers

State-Changing Observation and the Decomposition of Retrieval Loss: An Instrument-Based Formulation of Loopback Observation Theory

Masahito Takagi

This preprint extends the finite probabilistic model of Loopback Observation Theory (LOT) from nondisturbing record formation to state-changing observation, as a sequel to the FinStat-style model of probabilistic observation and retrieval hypotheses. A finite pre-observation state space, a finite record space, a finite post-observation state space, and a prior distribution are used to define a state-changing instrument, from which three prior-relative retrieval losses are constructed: from the record alone, from the post-observation state alone, and from both together. The paper does not claim to model the internal structure of the boundary M0, nor does it develop higher observer structures. The nondisturbing model of the preceding paper is recovered as a degenerate case in which the post-observation state coincides with the pre-observation state, and a post-state reset case, in which the post-observation state is independent of the pre-observation state, is identified as the opposite extreme. The joint retrieval loss is decomposed into the initial uncertainty about the pre-observation state, the information carried separately by the record and by the post-observation state, and a co-information interaction term. Under the sign convention adopted here, a positive interaction term indicates redundancy-like overlap, while a negative one indicates synergy-like behavior, in which the record and the post-observation state jointly retrieve more than the sum of their separate contributions. Output-separable instruments, for which the two outputs are conditionally independent given the pre-observation state, are shown to have a nonnegative interaction term and therefore cannot produce synergistic loopback closure. The mathematical components used here are standard: conditional entropy, mutual information, conditional mutual information, and co-information. The contribution of this paper is to organize these structures within the LOT triad of record formation, post-state realization, and retrieval, classifying state-changing instruments by whether pre-state information resides in the record, in the post-observation state, or in the coupling between them. AI-assisted: large language model tools (ChatGPT, Claude) were used for drafting, translation, and cross-checking; all claims and final content are the author's responsibility.

•Jun 28, 2026•0 citations

States and observables

Theoretical and mathematical physics•Sep 22, 2008•0 citations

States and Observables

Bernd Thaller

Springer eBooks•Jan 1, 2000•0 citations

Linear Quantum State Observers

Maison Clouâtré, Mark J. Balas, Vinod P. Gehlot +1 more

This paper considers the use of linear state observers to infer the unknown state (density matrix) of a closed quantum system using generalized quantum measurement—positive operator-valued measures (POVMs). An efficient test for observability is described in terms of two quantum observability matrices. The main contribution of this work is the development of a canonical quantum state observer, which may be utilized to estimate the state of any closed quantum system using POVM measurements. The observer ensures the state estimation error tends to the unobservable space of the system, which is exactly zero when the system is observable. The space of Hermitian matrices is shown to be invariant with respect to the dynamics of the canonical observer, which allows one to project the observer's state onto the space of valid quantum density operators while retaining convergence to the true state.

IEEE Transactions on Quantum Engineering•Jan 1, 2022•9 citations

STATES AND OBSERVABLES

WORLD SCIENTIFIC eBooks•Jul 1, 1996•0 citations

Quantum Theory, Consciousness, and Being

Daegene Song

In [NeuroQuantology 6, 46 (2008): arXiv:0706.4180], a certain natural phenomenon of self-observing consciousness was shown to be incompatible with the standard axioms of quantum theory. In order to consider a possibility of removing this inconsistency, which arises due to the separation between an observing party and a state vector being observed stated in the quantum theory axioms, we provide a conjecture where ‘being’, or existence, is identified with the experience of observing the state vector. That is, the observer is not observing the state vector in terms of the relative difference between reference frames, instead, the experience of observing the state vector should define the observer, or being. It is shown that the Heisenberg picture provides a natural description of this conjecture. 1

•Mar 5, 2007•0 citations
This preprint extends the finite probabilistic model of Loopback Observation Theory (LOT) from nondisturbing record formation to state-changing observation, as a sequel to the FinStat-style model of probabilistic observation and retrieval hypotheses. A finite pre-observation state space, a finite record space, a finite post-observation state space, and a prior distribution are used to define a state-changing instrument, from which three prior-relative retrieval losses are constructed: from the record alone, from the post-observation state alone, and from both together. The paper does not claim to model the internal structure of the boundary M0, nor does it develop higher observer structures. The nondisturbing model of the preceding paper is recovered as a degenerate case in which the post-observation state coincides with the pre-observation state, and a post-state reset case, in which the post-observation state is independent of the pre-observation state, is identified as the opposite extreme. The joint retrieval loss is decomposed into the initial uncertainty about the pre-observation state, the information carried separately by the record and by the post-observation state, and a co-information interaction term. Under the sign convention adopted here, a positive interaction term indicates redundancy-like overlap, while a negative one indicates synergy-like behavior, in which the record and the post-observation state jointly retrieve more than the sum of their separate contributions. Output-separable instruments, for which the two outputs are conditionally independent given the pre-observation state, are shown to have a nonnegative interaction term and therefore cannot produce synergistic loopback closure. The mathematical components used here are standard: conditional entropy, mutual information, conditional mutual information, and co-information. The contribution of this paper is to organize these structures within the LOT triad of record formation, post-state realization, and retrieval, classifying state-changing instruments by whether pre-state information resides in the record, in the post-observation state, or in the coupling between them. AI-assisted: large language model tools (ChatGPT, Claude) were used for drafting, translation, and cross-checking; all claims and final content are the author's responsibility.
This paper considers the use of linear state observers to infer the unknown state (density matrix) of a closed quantum system using generalized quantum measurement—positive operator-valued measures (POVMs). An efficient test for observability is described in terms of two quantum observability matrices. The main contribution of this work is the development of a canonical quantum state observer, which may be utilized to estimate the state of any closed quantum system using POVM measurements. The observer ensures the state estimation error tends to the unobservable space of the system, which is exactly zero when the system is observable. The space of Hermitian matrices is shown to be invariant with respect to the dynamics of the canonical observer, which allows one to project the observer's state onto the space of valid quantum density operators while retaining convergence to the true state.
In [NeuroQuantology 6, 46 (2008): arXiv:0706.4180], a certain natural phenomenon of self-observing consciousness was shown to be incompatible with the standard axioms of quantum theory. In order to consider a possibility of removing this inconsistency, which arises due to the separation between an observing party and a state vector being observed stated in the quantum theory axioms, we provide a conjecture where ‘being’, or existence, is identified with the experience of observing the state vector. That is, the observer is not observing the state vector in terms of the relative difference between reference frames, instead, the experience of observing the state vector should define the observer, or being. It is shown that the Heisenberg picture provides a natural description of this conjecture. 1