Research graph
References from Non-secular polariton leakage and dark-state protection in hybrid plasmonic cavities. Local targets link to admitted publications; unresolved targets remain external evidence.
Springer Tracts in Modern Physics
1988 · External reference
Nanoantennas for visible and infrared radiation
10.1088/0034-4885/75/2/024402 · 2012 · External reference
Patch antenna terahertz photodetectors
10.1063/1.4918983 · 2015 · External reference
Optimization of 1D plasmonic grating of nanostructured devices for the investigation of plasmonic bandgap
10.1007/s11468-018-0857-5 · 2019 · External reference
Ultrastrong coupling between light and matter
10.1038/s42254-018-0006-2 · 2019 · External reference
Ultrastrong coupling between nanoparticle plasmons and cavity photons at ambient conditions
10.1038/s41467-020-16524-x · 2020 · External reference
Ultrastrong plasmon–phonon coupling via epsilon-near-zero nanocavities
10.1038/s41566-020-00731-5 · 2021 · External reference
Manipulating light-matter interaction into strong coupling regime for photon entanglement in plasmonic lattices
10.1063/5.0135493 · 2023 · External reference
Theory of the contribution of excitons to the complex dielectric constant of crystals
10.1103/physrev.112.1555 · 1958 · External reference
Quantum vacuum properties of the intersubband cavity polariton field
10.1103/physrevb.72.115303 · 2005 · External reference
Ultra-strong light-matter coupling and superradiance using dense electron gases
10.1016/j.crhy.2016.05.001 · 2016 · External reference
Rabi splitting of the optical intersubband absorption line of multiple quantum wells inside a Fabry-Pérot microcavity
10.1103/physrevb.55.7101 · 1997 · External reference
Optical properties of metal-dielectric-metal microcavities in the THz frequency range
10.1364/oe.18.013886 · 2010 · External reference
Strong near field enhancement in THz nano-antenna arrays
10.1038/srep01361 · 2013 · External reference
Immunity of intersubband polaritons to inhomogeneous broadening
10.1103/physrevb.96.235301 · 2017 · External reference
Quantum well infrared photo-detectors operating in the strong light-matter coupling regime
10.1063/1.5084112 · 2019 · External reference
Electronic transport driven by collective light-matter coupled states in a quantum device
10.1038/s41467-023-39594-z · 2023 · External reference
Quantum open system description of a hybrid plasmonic cavity
10.1103/2xfb-jcgy · 2026 · External reference
On the generators of quantum dynamical semigroups
10.1007/bf01608499 · 1976 · External reference
Completely positive dynamical semigroups of n-level systems
10.1063/1.522979 · 1976 · External reference
Unresolved reference
2007 · External reference
Renormalized photon propagator in quantum electrodynamics of plasmonic cavities
10.1088/1367-2630/add496 · 2025 · External reference
Dissipation and ultrastrong coupling in circuit QED
10.1103/physreva.84.043832 · 2011 · External reference
Quantum coherence in ultrastrong optomechanics
10.1103/physreva.91.013812 · 2015 · External reference
Breakdown of gauge invariance in ultrastrong-coupling cavity QED
10.1103/physreva.98.053819 · 2018 · External reference
Recovering an accurate Lindblad equation from the Bloch-Redfield equation for general open quantum systems
10.1103/physreva.109.062225 · 2024 · External reference
Lindblad master equation capable of describing hybrid quantum systems in the ultrastrong coupling regime
10.1103/physrevlett.132.106902 · 2024 · External reference
Dark-state polaritons in single- and double- Λ media
10.1103/physreva.77.013823 · 2008 · External reference
Experimental demonstration of stationary dark-state polaritons dressed by dipole-dipole interaction
10.1103/physrevlett.131.133001 · 2023 · External reference
Simultaneous observation of bright and dark polariton states in subwavelength gratings made from quasi-bulk WS2
10.1364/oe.553437 · 2025 · External reference
Interaction of a two-level atom with single-mode optical field beyond the rotating wave approximation
10.1364/oe.22.028671 · 2014 · External reference
Fano resonance Rabi splitting of surface plasmons
10.1038/s41598-017-08221-5 · 2017 · External reference
Intersubband polaritons in the electrical dipole gauge
10.1103/physrevb.85.045304 · 2012 · External reference
The gauge-invariant Lagrangian, the Power-Zienau-Woolley picture and the choices of field momenta in nonrelativistic quantum electrodynamics
10.1038/s41598-021-94405-z · 2021 · External reference
Accuracy assessment of perturbative master equations: embracing nonpositivity
10.1103/physreva.101.012103 · 2020 · External reference
Bath-induced coherence and the secular approximation
10.1103/physreva.94.012110 · 2016 · External reference
Irreversibility and generalized noise
10.1103/physrev.83.34 · 1951 · External reference
The fluctuation-dissipation theorem
10.1088/0034-4885/29/1/306 · 1966 · External reference
Unresolved reference
2012 · External reference
More specifically, we define ∫0∞dτeiωτC(τ)=12γ(ω)+iλ(ω). For a bosonic bath with spectral density J(ω) in thermal equilibrium, C(t)=∫0∞dω′J(ω′){[n(ω′)+1]e−iω′t+n(ω′)eiω′t}., where n(ω) is the Bose distribution. This yields γ(ω)∝J(ω)[n(ω)+1] for ω>0 and γ(ω)∝J(|ω|)n(|ω|) for ω<0, while λ(ω) is a principal-value integral over J(ω) (its Hilbert transform). At zero temperature, equations (14) and (15) follow.
External reference
Inserting H^int(t)=X^(t)⊗B^(t) into the Born–Markov master equation and tracing over the environment, characterized by a density operator ρ^env, yields bath correlation functions C(τ)=Trenv[B^(τ)B^(0)ρ^env] multiplied by products of system operators X^(t) and X^(t−τ) [21] Thus, the reservoir operator B^ disappears from the reduced dynamics, surviving only through the scalar functions γ(ω) and λ(ω) obtained from C(τ) (or equivalently from the spectral density J(ω) associated with the Drude–Lorentz susceptibility), while the Bloch–Redfield tensors Γij(ω) and Λij(ω) arise from combining these scalar kernels with the system coefficients Ai∗Aj that weight the transition operators σ^j.
External reference
QuTiP: an open-source python framework for the dynamics of open quantum systems
10.1016/j.cpc.2012.02.021 · 2012 · External reference
QuTiP 2: a python framework for the dynamics of open quantum systems
10.1016/j.cpc.2012.11.019 · 2013 · External reference
Generic method for integrating Lindblad master equations
10.1103/vnhp-fnl3 · 2025 · External reference
Three approaches for representing Lindblad dynamics by a matrix-vector notation
2015 · External reference
For a lorentzian spectrum of FWHM γD the bath correlation function decays as C(τ)∝e−(γD/2)τ (up to a carrier oscillation at ωpl), and the oscillatory cross term carrying the beat phase eiDeltaτ is reduced by the normalized overlap κc=∫0∞dτe−(γD/2)τcos(Δτ)∫0∞dτe−(γD/2)τ=(γD/2)2(γD/2)2+Δ2.
External reference
For a single-peaked spectral density, e.g., a Lorentzian J(ω)=J0ω/[(ω−ω0)2+γD2], taking two transition frequencies ωi=ω0 and ωj=ω0+Δ gives J(ωi)J(ωj)=J0[1+(Δ/γD)2]−1/2, which is suppressed by a factor approximately equal to γD/|Δ| when |Δ|≫γD.
External reference
Stimulated scattering and its dynamics in semiconductor microcavities at 80 k under nonresonant excitation conditions
10.1103/physrevb.64.233318 · 2001 · External reference
Ultrafast polariton relaxation dynamics in an organic semiconductor microcavity
10.1103/physrevb.83.245309 · 2011 · External reference
