Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:1401.0410 · Physics Letters A

Effective Hamiltonians for fastly driven tight-binding chains

A. P. Itin, Анатолий Исерович Нейштадт

Published Jan 10, 2014• 16 citations
arXivHTMLPDF
DOI
10.1016/j.physleta.2014.01.007

Related papers

Driven Tight-Binding Chain — A Quantum Paradigm

Sushanta Dattagupta

Resonance•Apr 1, 2022•7 citations

Effective Hamiltonians and Phase Diagrams for Tight-Binding Models

Nilanjana Datta, Roberto Fernández, Jürg Martin Fröhlich

arXiv:math-ph/9809007•Journal of Statistical Physics•Aug 1, 1999•41 citations

Green’s Functions for Tight-Binding Hamiltonians

Eleftherios N. Economou

Springer series in solid-state sciences•Jan 1, 1983•2 citations

Ab-initio quantum transport simulations with tight-binding-like Hamiltonians

Christian Stieger

•Jan 1, 2019•2 citations

Large Scale Quantum Simulations Using Tight-Binding Hamiltonians and Linear Scaling Methods

Giulia Galli, Jeongnim Kim, Andrew Canning +1 more

MRS Proceedings•Jan 1, 1997•0 citations

Stochastic resets in the context of a tight-binding chain driven by an oscillating field

Sushanta Dattagupta, Debraj Das, Shamik Gupta

Abstract In this work, we study in the framework of the so-called driven tight-binding chain (TBC) the issue of quantum unitary dynamics interspersed at random times with stochastic resets mimicking non-unitary evolution due to interactions with the external environment, the driven TBC involves a quantum particle hopping between the nearest-neighbour sites of a one-dimensional lattice and subject to an external forcing field that is periodic in time. We consider the resets to be taking place at exponentially-distributed random times. Using the method of stochastic Liouville equation, we derive exact results for the probability at a given time for the particle to be found on different sites and averaged with respect to different realizations of the dynamics. We establish the remarkable effect of localization of the TBC particle on the sites of the underlying lattice at long times. The system in the absence of stochastic resets exhibits delocalization of the particle, whereby the particle does not have a time-independent probability distribution of being found on different sites even at long times, and, consequently, the mean-squared displacement of the particle about its initial location has an unbounded growth in time. One may induce localization in the bare model only through tuning the ratio of the strength to the frequency of the field to have a special value, namely, equal to one of the zeros of the zeroth order Bessel function of the first kind. We show here that localization may be induced by a far simpler procedure of subjecting the system to stochastic resets.

arXiv:2209.14117•Journal of Statistical Mechanics Theory and Experiment•Oct 1, 2022•15 citations
Abstract In this work, we study in the framework of the so-called driven tight-binding chain (TBC) the issue of quantum unitary dynamics interspersed at random times with stochastic resets mimicking non-unitary evolution due to interactions with the external environment, the driven TBC involves a quantum particle hopping between the nearest-neighbour sites of a one-dimensional lattice and subject to an external forcing field that is periodic in time. We consider the resets to be taking place at exponentially-distributed random times. Using the method of stochastic Liouville equation, we derive exact results for the probability at a given time for the particle to be found on different sites and averaged with respect to different realizations of the dynamics. We establish the remarkable effect of localization of the TBC particle on the sites of the underlying lattice at long times. The system in the absence of stochastic resets exhibits delocalization of the particle, whereby the particle does not have a time-independent probability distribution of being found on different sites even at long times, and, consequently, the mean-squared displacement of the particle about its initial location has an unbounded growth in time. One may induce localization in the bare model only through tuning the ratio of the strength to the frequency of the field to have a special value, namely, equal to one of the zeros of the zeroth order Bessel function of the first kind. We show here that localization may be induced by a far simpler procedure of subjecting the system to stochastic resets.