pith. sign in

arxiv: 2403.07110 · v2 · pith:FURIKOCYnew · submitted 2024-03-11 · 🪐 quant-ph · cond-mat.mes-hall

Multimode-cavity picture of non-Markovian waveguide QED

classification 🪐 quant-ph cond-mat.mes-hall
keywords cavitynon-markovianwaveguidedynamicseffectiveevenmodesonly
0
0 comments X p. Extension
pith:FURIKOCY Add to your LaTeX paper What is a Pith Number?
\usepackage{pith}
\pithnumber{FURIKOCY}

Prints a linked pith:FURIKOCY badge after your title and writes the identifier into PDF metadata. Compiles on arXiv with no extra files. Learn more

read the original abstract

We introduce a picture to describe and intrepret waveguide-QED problems in the non-Markovian regime of long photonic retardation times resulting in delayed coherent feedback. The framework is based on an intuitive spatial decomposition of the waveguide into blocks. Among these, the block directly coupled to the atoms embodies an effective lossy multimode cavity leaking into the rest of the waveguide, in turn embodying an effective white-noise bath. The dynamics can be approximated by retaining only a finite number of cavity modes which grows with the time delay. This description captures the atomic as well as the field's dynamics, even with many excitations, in both emission and scattering processes. As an application, we show that the recently identified non-Markovian steady states can be understood by retaining very few or even only one cavity modes.

This paper has not been read by Pith yet.

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. Non-Markovian delay-assisted sensing with waveguide-coupled quantum emitters

    quant-ph 2026-05 unverdicted novelty 6.0

    Non-Markovian delays in two waveguide-coupled emitters create atom-photon quasi-bound states and multimode interactions that boost quantum Fisher information for sensing field gradients.