Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theorem

Adiabatic approximations break down classically when a constant-energy contour splits into separate contours, forcing the system to choose which daughter contour to follow; the choices often represent qualitatively different behavior, so that slowly changing conditions induce a sudden and drastic ch...

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Main Authors: Peter Stabel, James R Anglin
Format: Article
Language:English
Published: IOP Publishing 2022-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/aca557
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author Peter Stabel
James R Anglin
author_facet Peter Stabel
James R Anglin
author_sort Peter Stabel
collection DOAJ
description Adiabatic approximations break down classically when a constant-energy contour splits into separate contours, forcing the system to choose which daughter contour to follow; the choices often represent qualitatively different behavior, so that slowly changing conditions induce a sudden and drastic change in dynamics. The Kruskal–Neishtadt–Henrard (KNH) theorem relates the probability of each choice to the rates at which the phase space areas enclosed by the different contours are changing. This represents a connection within closed-system mechanics, and without dynamical chaos, between spontaneous change and increase in phase space measure, as required by the Second Law of Thermodynamics. Quantum mechanically, in contrast, dynamical tunneling allows adiabaticity to persist, for very slow parameter change, through a classical splitting of energy contours; the classical and adiabatic limits fail to commute. Here we show that a quantum form of the KNH theorem holds nonetheless, due to unitarity.
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spelling doaj.art-8b268585046b4813843c0669cbe012642023-08-09T14:11:16ZengIOP PublishingNew Journal of Physics1367-26302022-01-01241111305210.1088/1367-2630/aca557Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theoremPeter Stabel0https://orcid.org/0000-0001-6852-6090James R Anglin1State Research Center, OPTIMAS and Fachbereich Physik, Technische Universität Kaiserslautern , D-67663 Kaiserslautern, GermanyState Research Center, OPTIMAS and Fachbereich Physik, Technische Universität Kaiserslautern , D-67663 Kaiserslautern, GermanyAdiabatic approximations break down classically when a constant-energy contour splits into separate contours, forcing the system to choose which daughter contour to follow; the choices often represent qualitatively different behavior, so that slowly changing conditions induce a sudden and drastic change in dynamics. The Kruskal–Neishtadt–Henrard (KNH) theorem relates the probability of each choice to the rates at which the phase space areas enclosed by the different contours are changing. This represents a connection within closed-system mechanics, and without dynamical chaos, between spontaneous change and increase in phase space measure, as required by the Second Law of Thermodynamics. Quantum mechanically, in contrast, dynamical tunneling allows adiabaticity to persist, for very slow parameter change, through a classical splitting of energy contours; the classical and adiabatic limits fail to commute. Here we show that a quantum form of the KNH theorem holds nonetheless, due to unitarity.https://doi.org/10.1088/1367-2630/aca557quantum mechanicssemi-classical methodsquantum–classical correspondenceadiabatic theoryLandau–Zener avoided crossingsKruskal–Neishstadt–Henrard theorem
spellingShingle Peter Stabel
James R Anglin
Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theorem
New Journal of Physics
quantum mechanics
semi-classical methods
quantum–classical correspondence
adiabatic theory
Landau–Zener avoided crossings
Kruskal–Neishstadt–Henrard theorem
title Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theorem
title_full Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theorem
title_fullStr Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theorem
title_full_unstemmed Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theorem
title_short Dynamical change under slowly changing conditions: the quantum Kruskal–Neishtadt–Henrard theorem
title_sort dynamical change under slowly changing conditions the quantum kruskal neishtadt henrard theorem
topic quantum mechanics
semi-classical methods
quantum–classical correspondence
adiabatic theory
Landau–Zener avoided crossings
Kruskal–Neishstadt–Henrard theorem
url https://doi.org/10.1088/1367-2630/aca557
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AT jamesranglin dynamicalchangeunderslowlychangingconditionsthequantumkruskalneishtadthenrardtheorem