2022
DOI: 10.1103/physrevlett.128.087701
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Pushing the Limits in Real-Time Measurements of Quantum Dynamics

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Cited by 18 publications
(13 citation statements)
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“…Similar RTS phenomena are discerned in superconducting qubits [14], single photon avalanche diodes [15], ultrasensitive biosensors [16], and single-cell activities in ion channels [17]. Real-time dynamics in quantum electrical devices also reveal rapid jumping sequences [18,19]. Furthermore these bursting events can represent biological and biochemical processes like spontaneous transitions in gene-regulation network [20,21], where RTS models are adopted to explain stochastic individual gene activation and deactivation processes well.…”
mentioning
confidence: 74%
“…Similar RTS phenomena are discerned in superconducting qubits [14], single photon avalanche diodes [15], ultrasensitive biosensors [16], and single-cell activities in ion channels [17]. Real-time dynamics in quantum electrical devices also reveal rapid jumping sequences [18,19]. Furthermore these bursting events can represent biological and biochemical processes like spontaneous transitions in gene-regulation network [20,21], where RTS models are adopted to explain stochastic individual gene activation and deactivation processes well.…”
mentioning
confidence: 74%
“…For example, for the Fermi-Hubbard trimer with a built-in charge detector realized in Ref. 27 , extraction of the waiting time distribution requires time-resolved current measurements that have with very high accuracy been performed for simpler systems [67][68][69][70][71] . For larger systems, the relaxation time scales could be obtained by pumpprobe schemes, e.g., in the 1T-TaS 2 system.…”
Section: Discussionmentioning
confidence: 99%
“…As we will see in the following, the factorial moments and cumulants provide a convenient description of the single-electron micromaser. In particular, while ordinary cumulants are useful to describe continuous random variables, factorial cumulants are in some cases better suited to characterize discrete random variables, such as the number of counted electrons or photons [60][61][62][63][64][65][66][67][68][69][70][71].…”
Section: Full Counting Statisticsmentioning
confidence: 99%
“…Having characterized each of the two dynamical phases, we now go on to investigate the transition between them. To this end, we make use of Lee-Yang theory [30][31][32][33][34][35][36] by considering the zeros of the factorial moment generating function [60][61][62][63][64][65][66][67][68][69][70][71], which for our purposes plays the role of the partition function in equilibrium statistical mechanics [40][41][42][43][44][45][46][47][48]. However, in contrast to thermal phase transitions, we are not considering transitions between different equilibrium phases such as spin lattices with a vanishing or a finite average magnetization.…”
Section: Nonequilibrium Phase Transitionmentioning
confidence: 99%
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