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

Optical coherence redistribution and complementarity closure in exact non-Markovian photonic feedback channels

Matthias Jakob

Published Jun 5, 2026• 0 citations
Publisher

Abstract

Non-Markovian optical channels can redistribute interferometric visibility,which-path information, and entanglement in ways that are not captured byconcurrence dynamics alone. Motivated by cavity-QED, waveguide-feedback,and related photonic reservoir architectures, we study an exactly solvabletwo-qubit mini-reservoir model and interpret its reduced dynamics as an effectivelocal photonic feedback channel. For the reduced two-qubit state, predictabilityPk, visibility Vk, and concurrence C obey the mixed-state relationP2k (t)+V 2k (t)+C2(t) = Bk(t) ≤ 1, where Bk(t) is the locally accessible complementaritybudget. Within the Hilbert–Schmidt formulation of completecomplementarity, we show that the corresponding deficit is closed exactly byMk(t) ≡ 1 − Bk(t) = 2Cnlhs(t) − C2(t). The remainder therefore identifiesthe part of the nonlocal optical coherence sector that is not already encodedin concurrence. Exact trajectories for Bell, nonmaximally entangled parity,superposition-of-Bell, and Werner initial states reveal memory-inducedcollapse-and-revival structure in the accessible budget, in the visibility sectorwhen local coherence is present, and in the remainder itself. Comparisonswith one-sided discord and with the purity deficit show that Mk(t)is a distinct reduced-state diagnostic rather than a relabeling of entanglement,discord, or mixedness. Because all quantities are reconstructed fromthe same reduced two-qubit state, the framework is naturally compatible with interferometric and tomographic readout in memory-bearing quantumopticalplatforms.

DOI
10.5281/zenodo.20553203

Related papers

Complementarity balance in a solvable non-Markovian two-qubit model

Matthias Jakob

We present a conservative reformulation of the complementarity analysis containedin the underlying manuscript materials. The claim is restricted to the part that isdirectly supported by the available derivations: an exact reduced-state balance for localpredictability, local visibility, and entanglement in an exactly solvable mini-reservoir modelfor non-Markovian two-qubit dynamics. For each local qubit, the reduced budget is definedas Bk(t) = P2k (t) + V 2k (t) + C2(t) and is completed by a remainder Mk(t) = 1 − Bk(t).Within the Hilbert–Schmidt bookkeeping adopted from the source material, this remainderis written as the nonlocal contribution beyond concurrence, Mk(t) = 2Cnlhs(t)− C2(t). Theresult is model bound and should not be read as a universal conservation law for arbitrarycombinations of coherence, discord, and entanglement measures. Instead, it isolates a precisecomplementarity identity inside a controlled Markov-embedded open-system setting.

•Jun 5, 2026•0 citations

Structure and Flow Observables in Complementarity Dynamics of Open Two-Qubit Systems

Matthias Jakob

Abstract We develop a complementarity-based description of open two-qubit dynamics built aroundthe budget Bk(t) = P2k(t)+V 2k(t)+C2(t) and the associated deficit Dk(t) = 1−Bk(t). The mainoutcome is not a new universal witness of non-Markovianity, but a more useful split betweenstructure observables and flow observables. Using explicit prototype amplitude-damping anddephasing channels, together with asymmetric couplings and mixed initial states, we showthat deficit-based distances such as ∆D = maxt|Dk(t) − SL(t)| mainly encode state- andchannel-dependent geometry, whereas positive-variation functionals such as NC and N−Drespond more directly to memory-driven recovery. In addition, for an exactly solvable Bell-statedephasing sector we prove that the revival windows of C and −DA coincide and obtain closedexpressions for BA and DA. The paper reframes complementarity dynamics as a two-levelproblem: geometry of resource partition on one side and temporal backflow on the other. Theframework is tied to a same-dataset BLP-like benchmark and to two analytical propositionsthat anchor the relation between concurrence revival and deficit flow in solvable sectors and ongeneral revival intervals

•May 19, 2026•0 citations

Non-Markovian thermalization of entangled qubits

I. Glendinning, Matthias Jakob, Michael Noelle

We study the decoherence properties of an entangled bipartite qubit system, represented by two two-level atoms that are individually coupled to non-Markovian reservoirs. This coupling ensures that the dynamical equations of the atoms can be treated independently. The non-Markovian reservoirs are described by a model which leads to an exact non-Markovian master equation of the Nakajima-Zwanzig form [J. Salo, S. M. Barnett, and S. Stenholm, Optics Commun. 259, 772 (2006)]. We consider the evolution of the entanglement of a two-atom state that is initially completely entangled, quantified by its concurrence. Collapses and revivals in the concurrence, induced by the memory effects of the reservoir, govern the dynamics of the entangled quantum system. These collapses and revivals in the concurrence are a strong manifestation of the non-Markovian reservoir.

arXiv:quant-ph/0604030•Apr 5, 2006•0 citations

Minimal qutrit diagnostics of coherence sharing: distinguishing coherence amount from coherence structure

Matthias Jakob

We identify the qutrit as the minimal Hilbert-space dimension in which coherence amountand coherence sharing become operationally distinguishable. The starting point is theexact purity decomposition into population predictability, Hilbert–Schmidt coherence, andmixedness. Although this closure is a state-space identity, in dimension three it selects aEuclidean coherence coordinate that can be compared nontrivially with normalized ℓ1coherence. Their mismatch defines a positive deficit Δℓ1 that vanishes if and only if thethree pairwise coherence moduli are equal. The deficit therefore diagnosescoherence-sharing anisotropy rather than total coherence magnitude alone. We show thatΔℓ1 separates two physically distinct mechanisms of coherence reduction: populationanisotropy in symmetric channels and branch asymmetry in balanced qutrits. In a purifiedqutrit–meter model the same Euclidean language acquires a dynamical interpretationbecause reduced mixedness equals normalized linear-entropy entanglement across thesystem–meter cut. We clarify the resource-theoretic status of the diagnostic by showingthat it is not a coherence monotone, but a witness of unequal sharing among pairwisechannels. Finally, we give a reduced-state reconstruction protocol based on populationsand three embedded SU(2) Ramsey blocks, supported by finite-sample simulations. Thesame quantity has a direct three-path interferometric implementation in terms of pairwisefringe visibilities and calibrated path intensities, where it measures anisotropicmutual-coherence sharing rather than a universal violation of classical coherence theory.

•Jun 5, 2026•0 citations

Optical coherence redistribution and complementarity closure in exact non-Markovian photonic feedback channels

Matthias Jakob

Optics Communications•Jul 7, 2026•1 citation

Optical coherence redistribution and complementarity closure in exact non-Markovian photonic feedback channels

Matthias Jakob

•Jan 1, 2026•0 citations
Non-Markovian optical channels can redistribute interferometric visibility,which-path information, and entanglement in ways that are not captured byconcurrence dynamics alone. Motivated by cavity-QED, waveguide-feedback,and related photonic reservoir architectures, we study an exactly solvabletwo-qubit mini-reservoir model and interpret its reduced dynamics as an effectivelocal photonic feedback channel. For the reduced two-qubit state, predictabilityPk, visibility Vk, and concurrence C obey the mixed-state relationP2k (t)+V 2k (t)+C2(t) = Bk(t) ≤ 1, where Bk(t) is the locally accessible complementaritybudget. Within the Hilbert–Schmidt formulation of completecomplementarity, we show that the corresponding deficit is closed exactly byMk(t) ≡ 1 − Bk(t) = 2Cnlhs(t) − C2(t). The remainder therefore identifiesthe part of the nonlocal optical coherence sector that is not already encodedin concurrence. Exact trajectories for Bell, nonmaximally entangled parity,superposition-of-Bell, and Werner initial states reveal memory-inducedcollapse-and-revival structure in the accessible budget, in the visibility sectorwhen local coherence is present, and in the remainder itself. Comparisonswith one-sided discord and with the purity deficit show that Mk(t)is a distinct reduced-state diagnostic rather than a relabeling of entanglement,discord, or mixedness. Because all quantities are reconstructed fromthe same reduced two-qubit state, the framework is naturally compatible with interferometric and tomographic readout in memory-bearing quantumopticalplatforms.
We present a conservative reformulation of the complementarity analysis containedin the underlying manuscript materials. The claim is restricted to the part that isdirectly supported by the available derivations: an exact reduced-state balance for localpredictability, local visibility, and entanglement in an exactly solvable mini-reservoir modelfor non-Markovian two-qubit dynamics. For each local qubit, the reduced budget is definedas Bk(t) = P2k (t) + V 2k (t) + C2(t) and is completed by a remainder Mk(t) = 1 − Bk(t).Within the Hilbert–Schmidt bookkeeping adopted from the source material, this remainderis written as the nonlocal contribution beyond concurrence, Mk(t) = 2Cnlhs(t)− C2(t). Theresult is model bound and should not be read as a universal conservation law for arbitrarycombinations of coherence, discord, and entanglement measures. Instead, it isolates a precisecomplementarity identity inside a controlled Markov-embedded open-system setting.
Abstract We develop a complementarity-based description of open two-qubit dynamics built aroundthe budget Bk(t) = P2k(t)+V 2k(t)+C2(t) and the associated deficit Dk(t) = 1−Bk(t). The mainoutcome is not a new universal witness of non-Markovianity, but a more useful split betweenstructure observables and flow observables. Using explicit prototype amplitude-damping anddephasing channels, together with asymmetric couplings and mixed initial states, we showthat deficit-based distances such as ∆D = maxt|Dk(t) − SL(t)| mainly encode state- andchannel-dependent geometry, whereas positive-variation functionals such as NC and N−Drespond more directly to memory-driven recovery. In addition, for an exactly solvable Bell-statedephasing sector we prove that the revival windows of C and −DA coincide and obtain closedexpressions for BA and DA. The paper reframes complementarity dynamics as a two-levelproblem: geometry of resource partition on one side and temporal backflow on the other. Theframework is tied to a same-dataset BLP-like benchmark and to two analytical propositionsthat anchor the relation between concurrence revival and deficit flow in solvable sectors and ongeneral revival intervals
We study the decoherence properties of an entangled bipartite qubit system, represented by two two-level atoms that are individually coupled to non-Markovian reservoirs. This coupling ensures that the dynamical equations of the atoms can be treated independently. The non-Markovian reservoirs are described by a model which leads to an exact non-Markovian master equation of the Nakajima-Zwanzig form [J. Salo, S. M. Barnett, and S. Stenholm, Optics Commun. 259, 772 (2006)]. We consider the evolution of the entanglement of a two-atom state that is initially completely entangled, quantified by its concurrence. Collapses and revivals in the concurrence, induced by the memory effects of the reservoir, govern the dynamics of the entangled quantum system. These collapses and revivals in the concurrence are a strong manifestation of the non-Markovian reservoir.
We identify the qutrit as the minimal Hilbert-space dimension in which coherence amountand coherence sharing become operationally distinguishable. The starting point is theexact purity decomposition into population predictability, Hilbert–Schmidt coherence, andmixedness. Although this closure is a state-space identity, in dimension three it selects aEuclidean coherence coordinate that can be compared nontrivially with normalized ℓ1coherence. Their mismatch defines a positive deficit Δℓ1 that vanishes if and only if thethree pairwise coherence moduli are equal. The deficit therefore diagnosescoherence-sharing anisotropy rather than total coherence magnitude alone. We show thatΔℓ1 separates two physically distinct mechanisms of coherence reduction: populationanisotropy in symmetric channels and branch asymmetry in balanced qutrits. In a purifiedqutrit–meter model the same Euclidean language acquires a dynamical interpretationbecause reduced mixedness equals normalized linear-entropy entanglement across thesystem–meter cut. We clarify the resource-theoretic status of the diagnostic by showingthat it is not a coherence monotone, but a witness of unequal sharing among pairwisechannels. Finally, we give a reduced-state reconstruction protocol based on populationsand three embedded SU(2) Ramsey blocks, supported by finite-sample simulations. Thesame quantity has a direct three-path interferometric implementation in terms of pairwisefringe visibilities and calibrated path intensities, where it measures anisotropicmutual-coherence sharing rather than a universal violation of classical coherence theory.