Quantum transport of electrons through a molecule is a series of individual electron tunneling events separated by stochastic waiting time intervals. We study the emergence of temporal correlations between successive waiting times for the electron transport in a vibrating molecular junction. Using the master equation approach, we compute the joint probability distribution for waiting times of two successive tunneling events. We show that the probability distribution is completely reset after each tunneling event if molecular vibrations are thermally equilibrated. If we treat vibrational dynamics exactly without imposing the equilibration constraint, the statistics of electron tunneling events become non-renewal. Non-renewal statistics between two waiting times τ and τ means that the density matrix of the molecule is not fully renewed after time τ and the probability of observing waiting time τ for the second electron transfer depends on the previous electron waiting time τ. The strong electron-vibration coupling is required for the emergence of the non-renewal statistics. We show that in the Franck-Condon blockade regime, extremely rare tunneling events become positively correlated.
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Sensors (Basel)
January 2025
Acropolis Restoration Service, Hellenic Ministry of Culture, 10555 Athens, Greece.
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January 2025
Experimental Psychology, Faculty of Social Sciences, Helmholtz Institute, Utrecht University, Utrecht, The Netherlands.
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Digestive Disease and Surgery Institute, Cleveland Clinic London, UK.
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View Article and Find Full Text PDFPhys Rev Lett
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Google Quantum AI, Santa Barbara, California 93117, USA.
Quantum error correction (QEC) provides a practical path to fault-tolerant quantum computing through scaling to large qubit numbers, assuming that physical errors are sufficiently uncorrelated in time and space. In superconducting qubit arrays, high-energy impact events can produce correlated errors, violating this key assumption. Following such an event, phonons with energy above the superconducting gap propagate throughout the device substrate, which in turn generate a temporary surge in quasiparticle (QP) density throughout the array.
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