Abstract

It is one of the most important and long-standing issues of physics to derive the irreversibility out of a time-reversal symmetric equation of motion. The present paper considers the breaking of the time-reversal symmetry in open quantum systems and the emergence of an arrow of time. We claim that the time-reversal symmetric Schrödinger equation can have eigenstates that break the time-reversal symmetry if the system is open in the sense that it has at least a countably infinite number of states. Such eigenstates, namely the resonant and anti-resonant states, have complex eigenvalues. We show that, although these states are often called “unphysical”, they observe the probability conservation in a particular way. We also comment that the seemingly Hermitian Hamiltonian is non-Hermitian in the functional space of the resonant and anti-resonant states, and hence there is no contradiction in the fact that it has complex eigenvalues. We finally show how the existence of the states that break the time-reversal symmetry affects the quantum dynamics. The dynamics that starts from a time-reversal symmetric initial state is dominated by the resonant states for ; this explains the phenomenon of the arrow of time, in which the decay excels the growth. The time-reversal symmetry holds in that the dynamic ending at a time-reversal symmetric final state is dominated by the anti-resonant states for .

Highlights

  • All microscopic equations of motion, only with a slight exception of the weak interaction, have the time-reversal symmetry

  • The equation can have eigenstates that break the time-reversal symmetry, namely the resonant states that decay in time and the anti-resonant states that grow in time, both of which we showed are very much physical

  • We have argued that the arrow of time in open quantum systems emerges naturally in terms of resonant and anti-resonant state components of quantum states

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Summary

Introduction

All microscopic equations of motion, only with a slight exception of the weak interaction, have the time-reversal symmetry. Such states must have complex eigenvalues, as pointed out by other authors [5,6,15,16]. The Hamiltonian operator for the open quantum system is Hermitian in the standard Hilbert space with normalizable eigenfunctions, but not Hermitian in the functional space that contains the states that break the time-reversal symmetry, and there is no contradiction if the symmetry-breaking eigenstates have complex eigenvalues [12,13,14,16].

Time-Reversal Operator
Complex Eigenvalues
Why Complex Eigenvalues for “Hermitian” Hamiltonian?
One More Element for “Arrow of Time”
Summary and Discussion
Full Text
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