Skip to content
DraconiticResearch
Search Sources API
201,642 studies31 sourcesUpdated 13 min ago
PreprintarXiv licencearXiv

How I Learned to Stop Worrying and Love the Redfield Equation: Completely-Positive Resummation of Non-Markovian Dynamics

Abstract

The Redfield equation with time-dependent coefficients (or TCL2 equation) gives one of the simplest perturbative descriptions of open quantum system dynamics derived from a microscopic theory. Its status as an approximation is nevertheless subtle: while perturbation theory fixes the reduced dynamics order-by-order in the system-environment coupling, solving the Redfield equation yields a particular resummation that need not preserve complete positivity. Here we compare Redfield evolution with an exponentiated (Magnus) resummation of the same second-order perturbative map, which is completely positive and trace preserving (CPTP) for a broad class of physical conditions. We also construct a simple CPTP resolvent resummation, illustrating the non-uniqueness of resummations of the same perturbative map. The Redfield and Magnus prescriptions agree to second order but differ through time-ordering corrections at higher orders. We exhibit a weak-coupling criterion which guarantees that Redfield evolution, even when non-Markovian, remains close to a CPTP map. We illustrate the criterion in two examples, focusing on finite-dimensional (qubit) systems. Our results clarify when, and why, Redfield evolution can remain reliable even when it is highly non-Lindbladian.

Related

  1. Heat transport in driven quantum systems: Comparison between the Floquet-Redfield equation and the master equation in the instantaneous eigenbasis
    Luca Magazzù, Christoforus Dimas Satrya, Aleksandr S. Strelnikov +2
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
  2. An efficient variational polaron master equation for non-Markovian spin-boson dynamics: Transformed initial states and general observables
    Chien-Chang Chen, Hsi-Sheng Goan
    arXivPreprintCC BY 4.0Full textCondensed matterQuantum physics & quantum informationarXiv
  3. Quantum optomechanics with arbitrary mirror displacement: nonlinear Langevin equation with non-Markovian back-action noises
    Adrian E. Rubio Lopez, Hing-Tong Cho, Bei-Lok Hu
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsQuantum physics & quantum informationarXiv
  4. Agentic AI for QCD perturbation theory or: how I learned to stop worrying and love the bot
    Erik Lundstrum
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsarXiv
  5. Revealing Hidden Orbital Pathways in NonThermal Hot Carrier Relaxation of MXenes via NonSecular Redfield Quantum Kinetics
    Ali Asghar Molavi Choobini, Abbas Chimeh, Jinhui Zhong
    arXivPreprintarXiv licenceFull textAtomic, molecular & optical physicsComputational physicsarXiv
BibTeX
@misc{kaplanek2026learned,
  title = {{How I Learned to Stop Worrying and Love the Redfield Equation: Completely-Positive Resummation of Non-Markovian Dynamics}},
  author = {Greg Kaplanek and Jason Pollack},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.03676},
  eprint = {2610.03676},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.03676},
}
RIS
TY  - UNPB
TI  - How I Learned to Stop Worrying and Love the Redfield Equation: Completely-Positive Resummation of Non-Markovian Dynamics
AU  - Greg Kaplanek
AU  - Jason Pollack
PY  - 2026
DA  - 2026/10/02
PB  - arXiv
DO  - 10.48550/arxiv.2610.03676
UR  - https://arxiv.org/abs/2610.03676
AB  - The Redfield equation with time-dependent coefficients (or TCL2 equation) gives one of the simplest perturbative descriptions of open quantum system dynamics derived from a microscopic theory. Its status as an approximation is nevertheless subtle: while perturbation theory fixes the reduced dynamics order-by-order in the system-environment coupling, solving the Redfield equation yields a particular resummation that need not preserve complete positivity. Here we compare Redfield evolution with an exponentiated (Magnus) resummation of the same second-order perturbative map, which is completely positive and trace preserving (CPTP) for a broad class of physical conditions. We also construct a simple CPTP resolvent resummation, illustrating the non-uniqueness of resummations of the same perturbative map. The Redfield and Magnus prescriptions agree to second order but differ through time-ordering corrections at higher orders. We exhibit a weak-coupling criterion which guarantees that Redfield evolution, even when non-Markovian, remains close to a CPTP map. We illustrate the criterion in two examples, focusing on finite-dimensional (qubit) systems. Our results clarify when, and why, Redfield evolution can remain reliable even when it is highly non-Lindbladian.
ER  -