{"total":21,"items":[{"citing_arxiv_id":"2606.26477","ref_index":22,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Algebraic structures of the Lindblad equation","primary_cat":"quant-ph","submitted_at":"2026-06-25T00:28:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Lindblad dynamics admits a universal closed algebra of Hermitian operators with model dependence isolated in a single set of coefficients.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.26162","ref_index":29,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Dissipative Quantum Multiplicative Weights with Sampling Feedback: A Classically Hard Primitive Realized via Engineered Open-System Dynamics","primary_cat":"quant-ph","submitted_at":"2026-06-24T04:52:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"DQMW-Sample realizes a classically hard online learning primitive via dissipative quantum dynamics with sublinear regret and proven hardness for classical simulation including PH collapse.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.23652","ref_index":2,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Robust Structure Learning of $k$-local Lindbladians","primary_cat":"quant-ph","submitted_at":"2026-06-22T17:38:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Protocol learns k-local Lindbladians to ε accuracy with Õ(n^{2k}/ε²) samples and projects to valid generators; improves to log n under sparsity assumptions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.19947","ref_index":35,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"QMaxCal: Path-Space Regularization for Open Quantum Control via Girsanov's Theorem","primary_cat":"quant-ph","submitted_at":"2026-06-18T08:44:18+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Derives KL_W and R_DV regularizers from Girsanov's theorem that reduce infidelity by up to 50% and improve robustness to noise mismatch on single- and multi-qubit benchmarks including an IBM Kingston calibration.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.15383","ref_index":3,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Quantum optimal control of steady orbits","primary_cat":"quant-ph","submitted_at":"2026-06-13T16:25:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A new quantum optimal control formalism for stroboscopic steady states and limit cycles in dissipative systems, implemented in Spinach with GRAPE-like scaling and distinct from Floquet-Lindblad approaches.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.09950","ref_index":20,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Integrating Out, Twice:The Open-System Case That Neural-Network Ensemble Theory Is Missing","primary_cat":"cs.LG","submitted_at":"2026-06-08T08:57:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Neural-network ensembles match closed Gaussian systems but lack the open-system non-Hermitian generator and continuous spectrum required by nuclear optical models, yielding a structural negative on applicability.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.26925","ref_index":20,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Adaptive Reinforcement Learning for Robust Open Quantum System Control: A Multi-Task Framework with Temporal Optimization","primary_cat":"quant-ph","submitted_at":"2026-05-26T12:20:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A multi-task SAC RL model discovers control pulses, evolution time, and segment numbers for 51 open quantum Hamiltonians, achieving high fidelity state transfer with better robustness to noise than GRAPE.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.26644","ref_index":29,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Evolution of Hypoequilibrium States in Steepest Entropy Ascent Models for Nonequilibrium Quantum Thermodynamics","primary_cat":"quant-ph","submitted_at":"2026-05-26T07:27:09+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Formal proof that M-th order hypoequilibrium states constitute an invariant manifold under SEAQT evolution, with connection to RCCE for reduced-order modeling of nonequilibrium quantum systems.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.23852","ref_index":15,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Convexity and non-Markovianity of Weyl Maps","primary_cat":"quant-ph","submitted_at":"2026-05-22T17:07:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Weyl dynamical maps are fully classified via phase-space subgroups; convex mixing of eternally non-Markovian dephasing maps yields Markovian semigroups, and irreducible eternally non-Markovian examples exist for qutrits.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.23358","ref_index":39,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"A Compilation Framework for Quantum Simulation of Non-unitary Dynamics","primary_cat":"quant-ph","submitted_at":"2026-05-22T08:22:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A new compilation framework treats quantum channels as first-class objects via ChannelIR and LindFront, achieving up to 99% gate count reduction on Lindbladian benchmarks versus unoptimized and Stinespring baselines.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.05162","ref_index":21,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Dynamical correlations in a dissipative XXZ spin chain","primary_cat":"cond-mat.str-el","submitted_at":"2026-05-06T17:32:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Dynamical correlations in a dissipative XXZ spin chain preserve early-time transport universality classes (ballistic, KPZ, diffusive) with magnon ballistic features at finite magnetization, but acquire exponential damping at long times under Lindblad evolution.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"The coherent dynamics is governed by the XXZ Hamiltonian H= J 4 L/2−1X l=−L/2 σx l σx l+1 +σ y l σy l+1 + ∆σ z l σz l+1 \u0001 ,(1) where σα l (α = x, y, z) are Pauli matrices at site l, J > 0 is the exchange energy, and ∆ is the dimensionless anisotropy parameter. The coupling to a Markovian environment is described by the Lindblad master equa- 3 SciPost Physics Submission tion [21,22] dρ(t) dt =−iL[ρ(t)] =−i[H, ρ(t)] +D[ρ(t)],(2) which provides the most general Markovian, completely positive, and trace-preserving map for the density matrix ρ(t) [23]. The coherent part generates unitary evolution, while D[ρ] encodes the action of the bath. We focus on spin loss and pumping applied uniformly at every site, a dissipation channel realizable in quantum simulation platforms based on ultracold atoms in optical"},{"citing_arxiv_id":"2605.04096","ref_index":12,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Quantum Dynamics: A Dilation-Based Approach","primary_cat":"math-ph","submitted_at":"2026-04-30T15:26:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"This thesis reviews and organizes dilation-based representations of quantum channel curves as an alternative to standard reduced dynamics in finite dimensions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.22010","ref_index":47,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Expansion of time-convolutionless non-Markovian quantum master equations: A case study using the Fano-Anderson model","primary_cat":"quant-ph","submitted_at":"2026-04-23T18:58:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"For the Fano-Anderson model with Lorentzian spectral density, the TCL expansion converges within a radius set by the detuning-to-width ratio, and its second and fourth orders represent non-Markovianity differently as measured by Bures distance evolution.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"and to the noise integral I(4)(t) = Z ∞ 0 dω2J(ω)n(ω) Re \u0012Z t 0 dτ G(2)(τ)e iωτ Z t 0 dτ e−i(ω−ω0)τ \u0013 .(44) Altogether, they lead to the emission and absorption rates of the master equation given by: γ−(t) =γ(t) +γI(t) + ˙I(t) (45) ≈γ (2)(t) +γ (4)(t) +γ (2) + (t) +γ (4) + (t),(46) γ+(t)≈ ˙I(2)(t)| {z } γ(2) + (t) + ˙I(4)(t) +γ (2)(t)I(2)(t)| {z } γ(4) + (t) .(47) To find the Green function the differential equation (24) has to be solved in fourth order: d dt G(4)(t) +iω 0G(4)(t) + Z t 0 dτK(t−τ)G (2)(τ) = 0, (48) which yields ˙˜G(4)(t) =− Z t 0 dτK(τ−t)e iω0(t−τ) ˜G(2)(τ).(49) 6 IV. VALIDITY AND LIMITATIONS OF THE TCL EXPANSION In this section we compare the TCL expansion for a Lorentzian spectral density up to fourth order with the"},{"citing_arxiv_id":"2604.19973","ref_index":32,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Dissipative microcanonical ensemble preparation from KMS-detailed balance","primary_cat":"quant-ph","submitted_at":"2026-04-21T20:30:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Extends KMS-detailed balance constructions from open quantum systems to prepare microcanonical ensembles and other stationary states with criteria for efficient implementation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.18440","ref_index":102,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Coherent terahertz field tomographic imaging in warm Rydberg vapors","primary_cat":"physics.atom-ph","submitted_at":"2026-04-20T15:59:21+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Coherent THz-to-optical conversion in warm Rb vapor via adjustable optical probe interference enables tomographic reconstruction of THz field amplitude and phase.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.10255","ref_index":15,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Model-Free Quantum Stabilization via Finite-Difference Lyapunov Control","primary_cat":"quant-ph","submitted_at":"2026-04-11T15:36:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A model-free quantum stabilization framework uses sign-based Lyapunov descent, adaptive gains, and finite-difference LaSalle analogue to guarantee asymptotic stability in drift-free cases and practical ISS with unknown drift and noise.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"ing quantum filtering and continuous measurement models [1, 6, 7, 8]. Such approaches provide powerful tools for real-time control under uncertainty, yet still require specification or estimation of the drift and noise operators. Related stability ana lyses for open quantum systems have also been developed using operator-theoretic and s emigroup-based methods [15, 16, 17]. More recently, learning-based approaches have been explored fo r measurement-based quantum feedback control, including reinforcement learning and de ep reinforcement learning schemes that construct control policies directly from measureme nt data [18]. These meth- ods demonstrate impressive empirical performance, such as acce lerated convergence and"},{"citing_arxiv_id":"2603.00189","ref_index":7,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Thermodynamics Beyond State Functions from Quantum Relaxation","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-02-27T02:06:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In quantum thermalization with detailed balance, internal energy becomes E(S, dot S), extending thermodynamics to include dynamical rates.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2602.13922","ref_index":60,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Decoherence, Perturbations and Symmetry in Lindblad Dynamics -- Implications for Diffractive Dissociation","primary_cat":"quant-ph","submitted_at":"2026-02-14T23:23:29+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Single-diffractive cross sections in pp and pbar p collisions are described by a three-parameter fit in a dephasing Lindblad framework yielding a consistent decoherence factor φ ≈ 0.89 that favors CPT-invariant dephasing over CP-invariant.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.11242","ref_index":33,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Dissipation-Induced Steady States in Topological Superconductors: Mechanisms and Design Principles","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-08-15T06:15:20+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Establishes correspondence between equilibrium Majorana zero modes and non-equilibrium kinetic zero modes in dissipative topological superconductors, derives algebraic relation for their numbers, and proposes dissipation engineering recipes demonstrated on Kitaev chain.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2502.18246","ref_index":44,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Reaction-diffusion dynamics of the weakly dissipative Fermi gas","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-02-25T14:25:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"The weakly dissipative 1D Fermi gas exhibits algebraic density decay for annihilation and coagulation reactions and a mean-field directed percolation absorbing-state phase transition, extending previous lattice results to continuous space.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1906.08165","ref_index":65,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Phase-space modelling of solid-state plasmas","primary_cat":"cond-mat.mes-hall","submitted_at":"2019-06-19T15:43:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Phase-space kinetic modeling with distribution function f(r,p,t) is applied to solid-state plasmas in nano-objects, adding quantum, spin, relativistic and dissipative features for linear and nonlinear response examples.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"the experience acquired in plasma physics. Generally speaking, the relevant kinetic equation (Vlasov, Wigner) may be augmented by a collision term of the form: (∂f ∂t ) coll . We also note that it is conceptually harder to include collisions in fully quantum models. A significant constraint is that non-unitary corrections to the Wigner equation should be written in Lindblad form [65], which guarantees that the evolved Wigner function always corresponds to a positive-definite density matrix. This constraint is not always satisfied for the models described below. In the following, we will discuss three different collision integrals for e-e and e-ph collisions, based on a relaxation term, a Boltzmann-like approach, and a Fokker-Planck approach."}],"limit":50,"offset":0}