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arXiv:2611.01749

An Observable-Algebra Approach to Quantum Coherence in Anyonic Systems

Cheng-Qian Xu, D. L. Zhou

quant-phmath-phSubmitted Nov 1, 2026• Announced Nov 3, 2026
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Abstract

Physical restrictions on operations can make quantum coherence inaccessible. Quantifying off-diagonal density matrix elements in a chosen basis alone does not reveal which information is hidden by each restriction. To distinguish their effects, we describe physical restrictions through subalgebras of accessible observables. The associated trace-preserving conditional expectations unify two reconstruction principles: each gives both the maximum-entropy state compatible with the accessible data and the closest state in the corresponding subalgebra in relative entropy. We apply this framework to anyonic systems to separate the contributions from local-charge superselection and non-Abelian fusion rules. We prove that the charge-line severing map is the conditional expectation onto the local-product subalgebra. It is completely positive and quantum-trace-preserving, and uniquely reconstructs a state in this space from all local-product expectation values. The hierarchy of measurement restrictions then separates total bipartite coherence into three nonnegative contributions: coherence between local charges, inaccessible fusion information, and conventional coherence. The first two decompose the anyonic charge entanglement and distinguish the effects of local-charge superselection from the remaining fusion information. Finally, we relate basis-independent measures of anyonic coherence to entanglement. For pure anyonic states with vacuum total charge, the optimized total and correlated coherence equal the total and conventional relative-entropy entanglement, respectively.

AI Summary

The paper asks how to distinguish information hidden by local-charge superselection from information hidden by non-Abelian fusion, rather than identifying coherence solely with off-diagonal density-matrix elements. It describes accessible measurements by finite-dimensional observable subalgebras. Their trace-preserving conditional expectations give both the unique maximum-entropy state compatible with accessible data and the unique relative-entropy minimizer within the subalgebra. Information loss equals the entropy increase, and nested subalgebras yield additive, nonnegative losses. These statements are established using expectation-value preservation and relative-entropy identities, including singular states and the anyonic quantum trace. For bipartite anyons, charge-line severing is identified with conditional expectation onto the local-product algebra, establishing complete positivity and quantum-trace preservation. A hierarchy of local-charge-preserving, local-product, and local-diagonal algebras gives $C=C_{\rm sec}+C_{\rm fus}+C_{\rm conv}$, with $S_{\rm ACE}=C_{\rm sec}+C_{\rm fus}$. Fusion information vanishes for Abelian anyons but can persist in globally diagonal states: two Fibonacci anyons fusing to vacuum have $C_{\rm fus}=2\log_2 d_\tau$ despite zero fusion-basis coherence. For vacuum-total-charge pure states, sectorwise Schmidt bases minimize total and correlated coherence, recovering total and conventional relative-entropy entanglement, respectively. The charge contributions are $H(p)$ and $2\sum_a p_a\log_2d_a$. The framework assumes accessible observables form unital subalgebras; local-product reconstruction does not additionally impose known global charge. The optimized entanglement equalities are restricted to vacuum pure states. A discussion expresses topological entanglement entropy through optimized microscopic regional coherences, but this optimization does not remove spurious conditional-mutual-information contributions.

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Physical restrictions on operations can make quantum coherence inaccessible. Quantifying off-diagonal density matrix elements in a chosen basis alone does not reveal which information is hidden by each restriction. To distinguish their effects, we describe physical restrictions through subalgebras of accessible observables. The associated trace-preserving conditional expectations unify two reconstruction principles: each gives both the maximum-entropy state compatible with the accessible data and the closest state in the corresponding subalgebra in relative entropy. We apply this framework to anyonic systems to separate the contributions from local-charge superselection and non-Abelian fusion rules. We prove that the charge-line severing map is the conditional expectation onto the local-product subalgebra. It is completely positive and quantum-trace-preserving, and uniquely reconstructs a state in this space from all local-product expectation values. The hierarchy of measurement restrictions then separates total bipartite coherence into three nonnegative contributions: coherence between local charges, inaccessible fusion information, and conventional coherence. The first two decompose the anyonic charge entanglement and distinguish the effects of local-charge superselection from the remaining fusion information. Finally, we relate basis-independent measures of anyonic coherence to entanglement. For pure anyonic states with vacuum total charge, the optimized total and correlated coherence equal the total and conventional relative-entropy entanglement, respectively.
The paper asks how to distinguish information hidden by local-charge superselection from information hidden by non-Abelian fusion, rather than identifying coherence solely with off-diagonal density-matrix elements.
It describes accessible measurements by finite-dimensional observable subalgebras. Their trace-preserving conditional expectations give both the unique maximum-entropy state compatible with accessible data and the unique relative-entropy minimizer within the subalgebra. Information loss equals the entropy increase, and nested subalgebras yield additive, nonnegative losses. These statements are established using expectation-value preservation and relative-entropy identities, including singular states and the anyonic quantum trace.
For bipartite anyons, charge-line severing is identified with conditional expectation onto the local-product algebra, establishing complete positivity and quantum-trace preservation. A hierarchy of local-charge-preserving, local-product, and local-diagonal algebras gives C=Csec+Cfus+CconvC=C_{\rm sec}+C_{\rm fus}+C_{\rm conv}C=Csec​+Cfus​+Cconv​, with SACE=Csec+CfusS_{\rm ACE}=C_{\rm sec}+C_{\rm fus}SACE​=Csec​+Cfus​. Fusion information vanishes for Abelian anyons but can persist in globally diagonal states: two Fibonacci anyons fusing to vacuum have Cfus=2log⁡2dτC_{\rm fus}=2\log_2 d_\tauCfus​=2log2​dτ​ despite zero fusion-basis coherence.
For vacuum-total-charge pure states, sectorwise Schmidt bases minimize total and correlated coherence, recovering total and conventional relative-entropy entanglement, respectively. The charge contributions are H(p)H(p)H(p) and 2∑apalog⁡2da2\sum_a p_a\log_2d_a2∑a​pa​log2​da​.
The framework assumes accessible observables form unital subalgebras; local-product reconstruction does not additionally impose known global charge. The optimized entanglement equalities are restricted to vacuum pure states. A discussion expresses topological entanglement entropy through optimized microscopic regional coherences, but this optimization does not remove spurious conditional-mutual-information contributions.
An anyonic system not only has potential applications in the construction of topological quantum computers but also presents a unique property known as topological entanglement entropy (TEE) in quantum many-body systems. Recently, Bonderson et al. [Ann. Phys. (NY) 385, 399 (2017)] have formally defined the entropy of anyonic charge entanglement (ACE) in anyonic states that has been shown to be able to derive TEE. We give it operational meaning from the perspective of quantum information theory. Specifically, for an anyonic bipartite system, we define an operational measure of topological correlation based on the principle of maximum entropy, where the topological correlation is the information that cannot be accessed by local operations constrained by anyonic superselection rules (SSRs) and classical communication. For a given anyonic bipartite state with maximal rank, we prove that its topological correlation is equal to its entropy of ACE. This measure can be extended to measure nonlocal resources of other compound quantum systems in the presence of SSRs and can provide a more refined classification of correlations in a multipartite system with SSRs.
Anyonic systems are modeled by topologically protected Hilbert spaces which obey complex superselection rules restricting possible operations. These Hilbert spaces cannot be decomposed into tensor products of spatially localized subsystems, whereas the tensor product structure is a foundation of the standard entanglement theory. We formulate bipartite entanglement theory for pure anyonic states and analyze its properties as a nonlocal resource for quantum information processing. We introduce a new entanglement measure, asymptotic entanglement entropy (AEE), and show that it characterizes distillable entanglement and entanglement cost similarly to entanglement entropy in conventional systems. AEE depends not only on the Schmidt coefficients but also on the quantum dimensions of the anyons shared by the local subsystems. Moreover, it turns out that AEE coincides with the entanglement gain by anyonic excitations in certain topologically ordered phases.
Non-Abelian anyons, a promising platform for fault-tolerant topological quantum computation, adhere to the charge super-selection rule (cSSR), which imposes restrictions on physically allowed states and operations. However, the ramifications of cSSR and fusion rules in anyonic quantum information theory remain largely unexplored. In this study, we unveil that the information-theoretic characteristics of anyons diverge fundamentally from those of non-anyonic systems such as qudits, bosons, and fermions and display intricate structures. In bipartite anyonic systems, pure states may have different marginal spectra, and mixed states may contain pure marginal states. More striking is that in a pure entangled state, parties may lack equal access to entanglement. This entanglement asymmetry is manifested in quantum teleportation employing an entangled anyonic state shared between Alice and Bob, where Alice can perfectly teleport unknown quantum information to Bob, but Bob lacks this capability. These traits challenge conventional understanding, necessitating new approaches to characterize quantum information and correlations in anyons. We expect that these distinctive features will also be present in non-Abelian lattice gauge field theories. Our findings significantly advance the understanding of the information-theoretic aspects of anyons and may lead to realizations of quantum communication and cryptographic protocols where one party holds sway over the other.
We study measures of quantum information when the space spanned by the set of accessible observables is not closed under products, i.e., we consider systems where an observer may be able to measure the expectation values of two operators, ⟨O1⟩⟨{O}_{1}⟩⟨O1​⟩ and ⟨O2⟩⟨{O}_{2}⟩⟨O2​⟩, but may not have access to ⟨O1O2⟩⟨{O}_{1}{O}_{2}⟩⟨O1​O2​⟩. This problem is relevant for the study of localized quantum information in gravity since the set of approximately local operators in a region may not be closed under arbitrary products. While we cannot naturally associate a density matrix with a state in this setting, it is still possible to define a modular operator for a state, and distinguish between two states using a relative modular operator. These operators are defined on a ``little Hilbert space,'' which parametrizes small deformations of the system away from its original state, and they do not depend on the structure of the full Hilbert space of the theory. We extract a class of relative-entropy-like quantities from the spectrum of these operators that measure the distance between states, are monotonic under contractions of the set of available observables, and vanish only when the states are equal. Consequently, these distance measures can be used to define measures of bipartite and multipartite entanglement. We describe applications of our measures to ``coarse-grained'' and ``fine-grained'' subregion dualities in AdS/CFT\mathrm{AdS}/\mathrm{CFT}AdS/CFT and provide a few sample calculations to illustrate our formalism.
A reasonable quantum information theory for fermions must respect the parity superselection rule to comply with the special theory of relativity and the no-signaling principle. This rule restricts the possibility of any quantum state to have a superposition between even- and odd-parity fermionic states. thereby characterizing the set of physically allowed fermionic quantum states. Here we introduce the physically allowed quantum operations, in congruence with the parity superselection rule, that map the set of allowed fermionic states onto itself. We first introduce unitary and projective measurement operations of the fermionic states. We further extend the formalism to general quantum operations in the forms of Stinespring dilation, operator-sum representation, and axiomatic completely positive and trace-preserving maps. We explicitly show the equivalence between these three representations of fermionic quantum operations. We discuss the possible implications of our results in characterization of correlations in fermionic systems.
Quantum systems may contain underlying correlations which are inaccessible to computationally bounded observers. We capture this distinction through a framework that analyses bipartite states only using efficiently implementable quantum channels. This leads to a complexity-constrained max-divergence and a corresponding computational min-entropy. The latter quantity recovers the standard operational meaning of the conditional min-entropy: in the fully quantum case, it quantifies the largest overlap with a maximally entangled state attainable via efficient operations on the conditional subsystem. For classical-quantum states, it further reduces to the optimal guessing probability of a computationally bounded observer with access to side information. Lastly, in the absence of side information, the computational min-entropy simplifies to a computational notion of the operator norm. We then establish strong separations between the information-theoretic and complexity-constrained notions of min-entropy. For pure states, there exist highly entangled families of states with extremal min-entropy whose efficiently accessible entanglement in terms of computational min-entropy is exponentially suppressed. For mixed states, the separation is even sharper: the information-theoretic conditional min-entropy can be highly negative while the complexity-constrained quantity remains nearly maximal. Under the cryptographic Learning with Errors hardness assumption, we construct efficiently preparable states exhibiting both separations, even when their preparation circuits are fully known. Overall, our results demonstrate that computational constraints can fundamentally limit the quantum correlations that are observable in practice.