Pith. sign in

REVIEW 3 minor 1 cited by

Time-periodic Lindblad equations for driven open systems map to static non-Hermitian eigenvalue problems in extended space.

Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →

T0 review · grok-4.3

2026-06-27 16:35 UTC pith:XUD7JK35

load-bearing objection The paper maps periodic Lindblad dynamics to a static non-Hermitian problem in Sambe-Liouville space and adds a continued-fraction resummation for harmonic drives that works directly in physical space.

arxiv 2606.09727 v1 pith:XUD7JK35 submitted 2026-06-08 quant-ph cond-mat.mes-hall

Sambe Approach to Floquet-Lindblad Open Quantum Systems

classification quant-ph cond-mat.mes-hall
keywords floquet theorylindblad master equationopen quantum systemsperiodic drivingsambe spaceresonance fluorescencequantum dotscorrelation functions
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper seeks to generalize Floquet engineering from closed to open quantum systems by constructing an effective time-independent generator for the stroboscopic dynamics of a time-periodic Lindblad master equation. It does so by embedding the problem in an extended Sambe-Liouville space where the periodic drive is absorbed into the basis states, converting the time-dependent evolution into a time-independent non-Hermitian eigenvalue problem. A matrix continued fraction technique is introduced for harmonic drives to resum all multiphoton processes and obtain an effective Lindbladian restricted to the physical space. A sympathetic reader would care because this supplies a practical route to compute steady states, correlation functions, and observables such as spectra without integrating the full time-dependent equation.

Core claim

By applying Floquet theory in the Sambe-Liouville space, the authors construct a well-defined time-independent Floquet Lindbladian, transforming the initial time-dependent problem to a static and non-Hermitian eigenvalue problem. For harmonic driving a matrix continued fraction method nonperturbatively resums multiphoton processes to build an effective Floquet Lindbladian acting only on the physical Liouville space. A resolvent formalism then yields a spectral Floquet representation of correlation functions, which is applied to compute the resonance fluorescence spectrum of a driven dissipative two-level system and the spectral function plus current-voltage curve of a parametrically driven q

What carries the argument

The Sambe-Liouville space extension of Floquet theory, which absorbs the periodic time dependence into an infinite tower of replicas so that the Lindbladian becomes a static non-Hermitian operator whose eigenvalues generate the stroboscopic map.

Load-bearing premise

The time-periodic Lindblad master equation remains valid under periodic driving and the Sambe-Liouville extension produces a generator whose restriction to the physical subspace reproduces the true reduced dynamics.

What would settle it

Numerical integration of the original time-dependent Lindblad equation over many drive periods for the driven two-level system, followed by comparison of the resulting stroboscopic map or fluorescence spectrum against the eigenvalues and eigenvectors of the constructed Floquet Lindbladian; any systematic mismatch falsifies the claim.

Watch this falsifier — get emailed when new claim-graph text bears on it.

If this is right

  • Stroboscopic evolution is obtained directly from the spectrum of the effective non-Hermitian operator without time-stepping.
  • Correlation functions of the open system admit an explicit spectral decomposition in terms of the resolvent of the Floquet Lindbladian.
  • Resonance fluorescence spectra and current-voltage characteristics become computable for concrete driven dissipative models.
  • The continued-fraction resummation supplies the entire infinite multiphoton series at once rather than order by order.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The method could be used to design periodic drives that steer open-system steady states or dissipative phases.
  • Direct comparison with exact short-time numerics on small systems would provide an immediate consistency check.
  • Generalization to non-harmonic periodic drives would require alternative resummation schemes beyond continued fractions.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

0 major / 3 minor

Summary. The paper develops a Floquet-theoretic construction for time-periodic Lindblad master equations by embedding the dynamics in an extended Sambe-Liouville space, yielding a static non-Hermitian eigenvalue problem whose solution defines an effective time-independent Floquet Lindbladian. For harmonic driving, a matrix continued-fraction resummation is introduced that acts only in the physical Liouville space and captures the full multiphoton series. The method is used to obtain a spectral representation of correlation functions and is applied to compute the resonance fluorescence spectrum of a driven dissipative two-level system and the spectral function plus I-V characteristics of a parametrically driven quantum dot with pump and loss.

Significance. If the central construction holds, the work supplies a parameter-free, non-perturbative route to effective generators for periodically driven open systems, extending standard Floquet engineering beyond closed systems. The matrix continued-fraction technique is a concrete technical strength, as it resums the entire infinite series at once rather than truncating at finite order. The resolvent-based spectral representation of correlation functions and the concrete applications to fluorescence and transport observables further demonstrate utility.

minor comments (3)
  1. [Introduction] The abstract states that the time-periodic Lindblad equation is assumed valid under driving, yet the manuscript does not explicitly discuss the regime of validity (e.g., Markovianity under strong driving) or cite supporting literature; adding a short paragraph in the introduction would strengthen the foundation.
  2. [Harmonic drive continued fraction] In the harmonic-drive continued-fraction section, the truncation criterion for the matrix fractions and the convergence test against the infinite continued fraction are not stated; an explicit statement or numerical convergence plot would clarify the practical implementation.
  3. [Application to two-level system] The two-level-system application reports the resonance fluorescence spectrum but does not compare the Floquet-Lindblad result against direct numerical integration of the original time-dependent master equation over one or more periods; such a benchmark would directly test the accuracy of the effective generator.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the detailed and positive summary of our manuscript, as well as for the favorable assessment of its significance. We note the recommendation for minor revision and will incorporate appropriate improvements in the revised version.

Circularity Check

0 steps flagged

No significant circularity; direct Floquet extension

full rationale

The central construction maps the time-periodic Lindblad master equation to a static non-Hermitian eigenvalue problem in the extended Sambe-Liouville space via standard Floquet theory, followed by a matrix continued-fraction resummation for harmonic drives. This is presented as a parameter-free mathematical transformation with no fitted inputs renamed as predictions, no load-bearing self-citations, and no ansatz smuggled via prior work. The derivation remains self-contained against the stated assumptions of the master equation and periodic steady state, with no reduction of claims to their own inputs by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central construction rests on the assumption that a time-periodic Lindblad master equation governs the driven open system and that the Sambe extension produces a valid generator; no free parameters or new entities are introduced in the abstract.

axioms (1)
  • domain assumption The driven open system is described by a time-periodic Lindblad master equation
    Stated as the starting point in the first sentence of the abstract.

pith-pipeline@v0.9.1-grok · 5769 in / 1119 out tokens · 20060 ms · 2026-06-27T16:35:40.336355+00:00 · methodology

0 comments
read the original abstract

We study driven and open quantum systems described by a time-periodic Lindblad master equation. In closed systems, the stroboscopic dynamics can always be described by an effective time-independent Floquet Hamiltonian; this idea is the basis of Floquet engineering. However, in the presence of dissipation, the existence of an effective time-independent Floquet Lindbladian is not guaranteed due to the non-unitary nature of the evolution. Using Floquet theory, we construct a well-defined time-independent Floquet Lindbladian in an extended Sambe-Liouville space, transforming the initial time-dependent problem to a static and non-Hermitian eigenvalue problem. For harmonic driving, we introduce a matrix continued fraction method to nonperturbatively resum multiphoton processes and construct an effective Floquet Lindbladian acting only on the physical Liouville space. Compared to other high-frequency expansions, this method has the advantage of providing the whole infinite series expansion at once. Using a resolvent formalism, we show how to obtain a spectral Floquet representation of correlation functions of an open quantum system. As an application, we consider a dissipating two-level system in a linearly polarized field and calculate its resonance fluorescence spectrum. Furthermore, we consider a parametrically driven quantum dot with pump and loss for which we calculate its spectral function and current-voltage characteristics.

Figures

Figures reproduced from arXiv: 2606.09727 by Andriani Keliri, Marco Schir\`o.

Figure 1
Figure 1. Figure 1: FIG. 1: (a) The spectrum of the Floquet-Lindbladian in the extended space [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: Spectrum of the stroboscopic evolution oper [PITH_FULL_IMAGE:figures/full_fig_p008_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: (a),(c): Emission spectra of the periodically driven TLS as a function of the emission frequency [PITH_FULL_IMAGE:figures/full_fig_p009_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: Spectral function [PITH_FULL_IMAGE:figures/full_fig_p010_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6: Current-voltage characteristics for different driv [PITH_FULL_IMAGE:figures/full_fig_p011_6.png] view at source ↗

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Gorini-Kossakowski-Sudarshan-Lindblad equation in different bases: application to driven-dissipative two- and multilevel systems

    quant-ph 2026-07 accept novelty 3.5

    Correct choice and unitary transformation of the computational basis for the GKSL equation is essential to obtain physically consistent dynamics of driven-dissipative qubits and multilevel systems.

Reference graph

Works this paper leans on

95 extracted references · 2 canonical work pages · cited by 1 Pith paper · 2 internal anchors

  1. [1]

    Superfermion representation One vectorization approach is the superfermion rep- resentation [59], also presented in [61, 62]. The density matrixρ(t) is an operator in a Fock space spanned by states|M⟩, I= P |M⟩ ⟨M|,⟨N|M⟩=δ N M.One then makes a copy of the initial Fock space, a so-called ‘tilde’ Fock space where ˜I= P | ˜M⟩ ⟨˜M|,⟨ ˜N| ˜M⟩=δ N M.The left va...

  2. [2]

    Trace preservation For a time periodic Lindbladian L(t)•=−i[H(t),•] + X i γi(t) Li •L † i − 1 2 n L† i Li,• o (B4) every harmonic is trace preserving: Tr(Lmρ) =−iTr([H m, ρ]) + X i γm i Tr LiρL† i − 1 2 L† i Liρ− 1 2 ρL† i Li = 0 (B5) where the cyclicity of the trace was used. In vectorized form the trace preservation is equivalent to the vector- ized ide...

  3. [3]

    Complex-conjugated spectrum The time-periodic Lindbladian superoperatorL t has the Hermiticity-preserving property (L t(A))† =L t(A†) for any operatorA.This implies that the harmonics of the Lindbladian obey the relation (Lm(A))† =L −m(A†).(B6) From this we conclude that only the zero-harmonic is Hermiticity-preserving. Moreover, it is easy to check that ...

  4. [4]

    Oka and S

    T. Oka and S. Kitamura, Floquet engineering of quantum materials, Annual Review of Condensed Matter Physics 10, 387 (2019). 17

  5. [5]

    Holthaus, Floquet engineering with quasienergy bands of periodically driven optical lattices, Journal of Physics B: Atomic, Molecular and Optical Physics49, 013001 (2015)

    M. Holthaus, Floquet engineering with quasienergy bands of periodically driven optical lattices, Journal of Physics B: Atomic, Molecular and Optical Physics49, 013001 (2015)

  6. [6]

    L. D. Marin Bukov and A. Polkovnikov, Universal high- frequency behavior of periodically driven systems: from dynamical stabilization to Floquet engineering, Advances in Physics64, 139 (2015)

  7. [7]

    Basov, R

    D. Basov, R. Averitt, and D. Hsieh, Towards properties on demand in quantum materials, Nature materials16, 1077 (2017)

  8. [8]

    Goldman and J

    N. Goldman and J. Dalibard, Periodically driven quan- tum systems: Effective Hamiltonians and engineered gauge fields, Phys. Rev. X4, 031027 (2014)

  9. [9]

    Eckardt, Colloquium: Atomic quantum gases in pe- riodically driven optical lattices, Rev

    A. Eckardt, Colloquium: Atomic quantum gases in pe- riodically driven optical lattices, Rev. Mod. Phys.89, 011004 (2017)

  10. [10]

    Oka and H

    T. Oka and H. Aoki, Photovoltaic Hall effect in graphene, Phys. Rev. B79, 081406 (2009)

  11. [11]

    Broers and L

    L. Broers and L. Mathey, Observing light-induced Flo- quet band gaps in the longitudinal conductivity of graphene, Communications Physics4, 1 (2021)

  12. [12]

    F. Wang, X. Cai, X. Tang, J. Lu, W. Chen, T. Sheng, R. Feng, H. Zhong, H. Zhang, P. Yu,et al., Observation of Floquet-induced gap in graphene, Nature Materials , 1 (2026)

  13. [13]

    N. H. Lindner, G. Refael, and V. Galitski, Floquet topo- logical insulator in semiconductor quantum wells, Nature Physics7, 490 (2011)

  14. [14]

    J. W. McIver, B. Schulte, F.-U. Stein, T. Matsuyama, G. Jotzu, G. Meier, and A. Cavalleri, Light-induced anomalous Hall effect in graphene, Nature physics16, 38 (2020)

  15. [15]

    M. S. Rudner and N. H. Lindner, Band structure engi- neering and non-equilibrium dynamics in Floquet topo- logical insulators, Nature reviews physics2, 229 (2020)

  16. [16]

    D. V. Else, B. Bauer, and C. Nayak, Floquet time crys- tals, Phys. Rev. Lett.117, 090402 (2016)

  17. [17]

    Zhang, P

    J. Zhang, P. W. Hess, A. Kyprianidis, P. Becker, A. Lee, J. Smith, G. Pagano, I.-D. Potirniche, A. C. Potter, A. Vishwanath,et al., Observation of a discrete time crys- tal, Nature543, 217 (2017)

  18. [18]

    Huang, P

    Z. Huang, P. S. Mundada, A. Gyenis, D. I. Schuster, A. A. Houck, and J. Koch, Engineering dynamical sweet spots to protect qubits from 1/fnoise, Phys. Rev. Ap- plied15, 034065 (2021)

  19. [19]

    Gandon, C

    A. Gandon, C. Le Calonnec, R. Shillito, A. Petrescu, and A. Blais, Engineering, control, and longitudinal readout of Floquet qubits, Phys. Rev. Applied17, 064006 (2022)

  20. [20]

    Sameti and M

    M. Sameti and M. J. Hartmann, Floquet engineering in superconducting circuits: From arbitrary spin-spin in- teractions to the Kitaev honeycomb model, Phys. Rev. A99, 012333 (2019)

  21. [21]

    L. B. Nguyen, Y. Kim, A. Hashim, N. Goss, B. Marinelli, B. Bhandari, D. Das, R. K. Naik, J. M. Kreike- baum, A. N. Jordan, D. I. Santiago, and I. Siddiqi, Programmable Heisenberg interactions between Floquet qubits, Nature Physics20, 240 (2024)

  22. [22]

    Chessari, E

    A. Chessari, E. A. Rodr´ ıguez-Mena, J. C. Abadillo-Uriel, V. Champain, S. Zihlmann, R. Maurand, Y.-M. Niquet, and M. Filippone, Unifying Floquet theory of longitudi- nal and dispersive readout, Phys. Rev. Lett.134, 037003 (2025)

  23. [23]

    D’Alessio and M

    L. D’Alessio and M. Rigol, Long-time behavior of isolated periodically driven interacting lattice systems, Phys. Rev. X4, 041048 (2014)

  24. [24]

    Lazarides, A

    A. Lazarides, A. Das, and R. Moessner, Equilibrium states of generic quantum systems subject to periodic driving, Phys. Rev. E90, 012110 (2014)

  25. [25]

    D. A. Abanin, W. De Roeck, and F. Huveneers, Expo- nentially slow heating in periodically driven many-body systems, Phys. Rev. Lett.115, 256803 (2015)

  26. [26]

    T. Mori, T. Kuwahara, and K. Saito, Rigorous bound on energy absorption and generic relaxation in periodically driven quantum systems, Phys. Rev. Lett.116, 120401 (2016)

  27. [27]

    Mori, Floquet states in open quantum systems, An- nual Review of Condensed Matter Physics14, 35 (2023)

    T. Mori, Floquet states in open quantum systems, An- nual Review of Condensed Matter Physics14, 35 (2023)

  28. [28]

    Tsuji, Floquet states, inEncyclopedia of con- densed matter physics (second edition), edited by T

    N. Tsuji, Floquet states, inEncyclopedia of con- densed matter physics (second edition), edited by T. Chakraborty (Academic Press, Oxford, 2024) second edition ed., pp. 967–980

  29. [29]

    K. I. Seetharam, C.-E. Bardyn, N. H. Lindner, M. S. Rudner, and G. Refael, Controlled population of Floquet- Bloch states via coupling to Bose and Fermi baths, Phys. Rev. X5, 041050 (2015)

  30. [30]

    Cohen, A

    J. Cohen, A. Petrescu, R. Shillito, and A. Blais, Reminis- cence of classical chaos in driven transmons, PRX Quan- tum4, 020312 (2023)

  31. [31]

    A. Riva, P. Gogoi, N. Gheeraert, S. Florens, A. W. Chin, A. Sarlette, and A. Petrescu, First-principles study of dis- persive readout in circuit qed (2026), arXiv:2604.11722 [quant-ph]

  32. [32]

    Ritter, D

    M. Ritter, D. M. Long, Q. Yue, A. Chandran, and A. J. Koll´ ar, Autonomous stabilization of Floquet states using static dissipation, Phys. Rev. X15, 031028 (2025)

  33. [33]

    Lindblad, On the generators of quantum dynamical semigroups, Communications in mathematical physics 48, 119 (1976)

    G. Lindblad, On the generators of quantum dynamical semigroups, Communications in mathematical physics 48, 119 (1976)

  34. [34]

    Gorini, A

    V. Gorini, A. Kossakowski, and E. C. G. Sudarshan, Completely positive dynamical semigroups of N-level sys- tems, Journal of Mathematical Physics17, 821 (1976)

  35. [35]

    Haddadfarshi, J

    F. Haddadfarshi, J. Cui, and F. Mintert, Completely pos- itive approximate solutions of driven open quantum sys- tems, Phys. Rev. Lett.114, 130402 (2015)

  36. [36]

    Schnell, A

    A. Schnell, A. Eckardt, and S. Denisov, Is there a Floquet Lindbladian?, Physical Review B101, 100301 (2020)

  37. [37]

    Wei and E

    J. Wei and E. Norman, Lie Algebraic Solution of Linear Differential Equations, Journal of Mathematical Physics 4, 575 (1963)

  38. [38]

    General form of quantum evolution

    D. Chruscinski and A. Kossakowski, General form of quantum evolution (2010), arXiv:1006.2764 [quant-ph]

  39. [39]

    Scopa, G

    S. Scopa, G. T. Landi, A. Hammoumi, and D. Karevski, Exact solution of time-dependent Lindblad equations with closed algebras, Physical Review A99, 022105 (2019)

  40. [40]

    L. R. Bakker, V. I. Yashin, D. V. Kurlov, A. K. Fe- dorov, and V. Gritsev, Lie-algebraic approach to one- dimensional translationally invariant free-fermionic dis- sipative systems, Physical Review A102, 052220 (2020)

  41. [41]

    Z.-X. Lin, B. Lapierre, P. Moosavi, and S. Ryu, Chiral instabilities in driven-dissipative quantum liquids, Phys. Rev. B111, 165131 (2025)

  42. [42]

    Qvarfort and I

    S. Qvarfort and I. Pikovski, Solving Quantum Dynamics with a Lie-Algebra Decoupling Method, PRX Quantum 6, 010201 (2025)

  43. [43]

    Schnell, S

    A. Schnell, S. Denisov, and A. Eckardt, High-frequency expansions for time-periodic Lindblad generators, Phys- 18 ical Review B104, 165414 (2021)

  44. [44]

    Mizuta, K

    K. Mizuta, K. Takasan, and N. Kawakami, Breakdown of Markovianity by interactions in stroboscopic Floquet- Lindblad dynamics under high-frequency drive, Physical Review A103, L020202 (2021)

  45. [45]

    Ikeda, K

    T. Ikeda, K. Chinzei, and M. Sato, Nonequilibrium steady states in the Floquet-Lindblad systems: van Vleck’s high-frequency expansion approach, SciPost Physics Core4, 033 (2021)

  46. [46]

    J. H. Shirley, Solution of the Schr¨ odinger Equation with a Hamiltonian Periodic in Time, Physical Review138, B979 (1965)

  47. [47]

    Sambe, Steady States and Quasienergies of a Quantum-Mechanical System in an Oscillating Field, Physical Review A7, 2203 (1973)

    H. Sambe, Steady States and Quasienergies of a Quantum-Mechanical System in an Oscillating Field, Physical Review A7, 2203 (1973)

  48. [48]

    Chen, Y.-M

    H. Chen, Y.-M. Hu, W. Zhang, M. A. Kurniawan, Y. Shao, X. Chen, A. Prem, and X. Dai, Periodically Driven Open Quantum Systems: Spectral Properties and Non-Equilibrium Steady States, Physical Review B109, 184309 (2024)

  49. [49]

    Szczygielski, On the Floquet analysis of commutative periodic Lindbladians in finite dimension, Linear Algebra and its Applications609, 176 (2021)

    K. Szczygielski, On the Floquet analysis of commutative periodic Lindbladians in finite dimension, Linear Algebra and its Applications609, 176 (2021)

  50. [50]

    T.-S. Ho, K. Wang, and S.-I. Chu, Floquet-Liouville supermatrix approach: Time development of density- matrix operator and multiphoton resonance fluorescence spectra in intense laser fields, Physical Review A33, 1798 (1986)

  51. [51]

    Szczygielski and R

    K. Szczygielski and R. Alicki, On Howland time- independent formulation of CP-divisible quantum evo- lutions, Reviews in Mathematical Physics32, 2050021 (2020)

  52. [52]

    B. R. Mollow, Power spectrum of light scattered by two- level systems, Phys. Rev.188, 1969 (1969)

  53. [53]

    H. J. Kimble and L. Mandel, Theory of resonance fluo- rescence, Phys. Rev. A13, 2123 (1976)

  54. [54]

    D. F. Walls and G. J. Milburn,Quantum optics, 2nd ed. (Springer, Berlin, 2008)

  55. [55]

    Rivas, S

    ´A. Rivas, S. F. Huelga, and M. B. Plenio, Quantum non-Markovianity: characterization, quantification and detection, Reports on Progress in Physics77, 094001 (2014)

  56. [56]

    Chru´ sci´ nski and A

    D. Chru´ sci´ nski and A. Kossakowski, Markovianity crite- ria for quantum evolution, Journal of Physics B: Atomic, Molecular and Optical Physics45, 154002 (2012)

  57. [57]

    Floquet, Sur les ´ equations diff´ erentielles lin´ eaires ` a coefficients p´ eriodiques, Annales scientifiques de l’´Ecole normale sup´ erieure12, 47 (1883)

    G. Floquet, Sur les ´ equations diff´ erentielles lin´ eaires ` a coefficients p´ eriodiques, Annales scientifiques de l’´Ecole normale sup´ erieure12, 47 (1883)

  58. [58]

    Hartmann, D

    M. Hartmann, D. Poletti, M. Ivanchenko, S. Denisov, and P. H¨ anggi, Asymptotic Floquet states of open quantum systems: the role of interaction, New Journal of Physics 19, 083011 (2017)

  59. [59]

    M. M. Wolf, J. Eisert, T. S. Cubitt, and J. I. Cirac, Assessing Non-Markovian Quantum Dynamics, Physical Review Letters101, 150402 (2008)

  60. [60]

    T. S. Cubitt, J. Eisert, and M. M. Wolf, The complexity of relating quantum channels to master equations, Com- munications in Mathematical Physics310, 383 (2012)

  61. [61]

    Prosen, Third quantization: a general method to solve master equations for quadratic open Fermi systems, New Journal of Physics10, 043026 (2008)

    T. Prosen, Third quantization: a general method to solve master equations for quadratic open Fermi systems, New Journal of Physics10, 043026 (2008)

  62. [62]

    A. A. Dzhioev and D. S. Kosov, Super-fermion rep- resentation of quantum kinetic equations for the elec- tron transport problem, The Journal of Chemical Physics 134, 044121 (2011)

  63. [63]

    Harbola and S

    U. Harbola and S. Mukamel, Superoperator nonequilib- rium Green’s function theory of many-body systems; ap- plications to charge transfer and transport in open junc- tions, Physics Reports465, 191 (2008)

  64. [64]

    Dorda, M

    A. Dorda, M. Nuss, W. Von Der Linden, and E. Ar- rigoni, Auxiliary master equation approach to nonequi- librium correlated impurities, Physical Review B89, 165105 (2014)

  65. [65]

    Arrigoni and A

    E. Arrigoni and A. Dorda, Master Equations Versus Keldysh Green’s Functions for Correlated Quantum Sys- tems Out of Equilibrium, inOut-of-Equilibrium Physics of Correlated Electron Systems, edited by R. Citro and F. Mancini (Springer International Publishing, Cham,

  66. [66]

    Takahashi and H

    Y. Takahashi and H. Umezawa, Thermo field dynamics, Int. J. Mod. Phys. B10, 1755 (1996)

  67. [67]

    Thermo field dynamics

    I. Ojima, Gauge fields at finite temperatures—“Thermo field dynamics” and the KMS condition and their exten- sion to gauge theories, Annals of Physics137, 1 (1981)

  68. [68]

    Fazio, J

    R. Fazio, J. Keeling, L. Mazza, and M. Schir` o, Many- body open quantum systems, SciPost Physics Lecture Notes , 099 (2025)

  69. [69]

    Szczygielski, On the application of Floquet theorem in development of time-dependent Lindbladians, Journal of Mathematical Physics55, 083506 (2014)

    K. Szczygielski, On the application of Floquet theorem in development of time-dependent Lindbladians, Journal of Mathematical Physics55, 083506 (2014)

  70. [70]

    Ashida, Z

    Y. Ashida, Z. Gong, and M. Ueda, Non-Hermitian Physics, Advances in Physics69, 249 (2020)

  71. [71]

    D. C. Brody, Biorthogonal quantum mechanics, Journal of Physics A: Mathematical and Theoretical47, 035305 (2013)

  72. [72]

    Ozawa, H

    T. Ozawa, H. M. Price, N. Goldman, O. Zilberberg, and I. Carusotto, Synthetic dimensions in integrated photon- ics: From optical isolation to four-dimensional quantum hall physics, Phys. Rev. A93, 043827 (2016)

  73. [73]

    Q. Lin, M. Xiao, L. Yuan, and S. Fan, Photonic Weyl point in a two-dimensional resonator lattice with a syn- thetic frequency dimension, Nature Communications7, 13731 (2016)

  74. [74]

    Martin, G

    I. Martin, G. Refael, and B. Halperin, Topological fre- quency conversion in strongly driven quantum systems, Phys. Rev. X7, 041008 (2017)

  75. [75]

    Ozawa and H

    T. Ozawa and H. M. Price, Topological quantum matter in synthetic dimensions, Nature Reviews Physics1, 349 (2019)

  76. [76]

    G. H. Wannier, Wave Functions and Effective Hamilto- nian for Bloch Electrons in an Electric Field, Physical Review117, 432 (1960)

  77. [77]

    Glueck, A

    M. Glueck, A. R. Kolovsky, and H. J. Korsch, Wannier- Stark resonances in optical and semiconductor superlat- tices, Physics Reports366, 103 (2002)

  78. [78]

    Dittrich, P

    T. Dittrich, P. H¨ anggi, G.-L. Ingold, B. Kramer, G. Sch¨ on, and W. Zwerger,Quantum transport and dis- sipation, Vol. 3 (Wiley-Vch Weinheim, 1998)

  79. [79]

    D. F. Martinez, Floquet–Green function formalism for harmonically driven Hamiltonians, Journal of Physics A: Mathematical and General36, 9827 (2003)

  80. [80]

    U. D. Giovannini and H. H¨ ubener, Floquet analysis of excitations in materials, Journal of Physics: Materials3, 012001 (2020)

Showing first 80 references.