A new MQMF-LME framework derives closed-form T1 and T2 expressions for interacting qubit ensembles and identifies long-range FRET as the dominant decoherence mechanism in Er3+-doped CeO2 by matching concentration dependence.
Quantum Noise in Quantum Optics: the Stochastic Schr\"odinger Equation
4 Pith papers cite this work. Polarity classification is still indexing.
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abstract
Lecture Notes for the Les Houches Summer School LXIII on Quantum Fluctuations in July 1995 to appear in Elsevier Science Publishers B.V. 1997, edited by E. Giacobino and S. Reynaud.
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For compact A,B in R² and 1≤p<∞, (d_lp(A+B))^p is at most max{1,2^{p-2}} times the sum of the p-powers of d_lp(A) and d_lp(B), with a sharp constant.
Derives closed-form expressions for squeezing, second-order correlation, and joint spectral intensity between signal and idler modes in quantum frequency combs from microring resonators.
The Lindblad equation is valid only within a finite time window controlled by the timescales of the bath, the system, and the rotating-wave approximation, with failure at early and late times.
citing papers explorer
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A Mean-Field Lindblad Master Equation Framework for Interaction-Driven Decoherence in Solid-State Qubit Ensembles
A new MQMF-LME framework derives closed-form T1 and T2 expressions for interacting qubit ensembles and identifies long-range FRET as the dominant decoherence mechanism in Er3+-doped CeO2 by matching concentration dependence.
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Quantum Optical Signatures of Band Topology in Solid-State High Harmonics
For compact A,B in R² and 1≤p<∞, (d_lp(A+B))^p is at most max{1,2^{p-2}} times the sum of the p-powers of d_lp(A) and d_lp(B), with a sharp constant.
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Steady-state dynamics of quantum frequency combs in microring resonators
Derives closed-form expressions for squeezing, second-order correlation, and joint spectral intensity between signal and idler modes in quantum frequency combs from microring resonators.
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Is Lindblad for me?
The Lindblad equation is valid only within a finite time window controlled by the timescales of the bath, the system, and the rotating-wave approximation, with failure at early and late times.