
arXiv: 1905.11291
A dynamical system is said to be reversible if, given an output, the input can always be recovered in a well-posed manner. Nevertheless, we argue that reversible systems that have a time-reversal symmetry, such as the Nonlinear Schr{ö}dinger equation and the $ϕ^4$ equation can become "physically irreversible". By this, we mean that realistically-small experimental errors in measuring the output can lead to dramatic differences between the recovered input and the original one. The loss of reversibility reveals a natural "arrow of time", reminiscent of the thermodynamic one, which is the direction in which the radiation is emitted outward. Our results are relevant to imaging and reversal applications in nonlinear optics.
NLS equations (nonlinear Schrödinger equations), FOS: Physical sciences, Lasers, masers, optical bistability, nonlinear optics, stability, nonlinear dynamics, Mathematics - Analysis of PDEs, KdV equations (Korteweg-de Vries equations), reversibility, Soliton solutions, Radiative heat transfer, Time-dependent Schrödinger equations and Dirac equations, FOS: Mathematics, \(\phi^4\)-equation, nonlinear Schrödinger, 35Q55, 35Q60, 78A60,, Physics - Optics, Analysis of PDEs (math.AP), Optics (physics.optics)
NLS equations (nonlinear Schrödinger equations), FOS: Physical sciences, Lasers, masers, optical bistability, nonlinear optics, stability, nonlinear dynamics, Mathematics - Analysis of PDEs, KdV equations (Korteweg-de Vries equations), reversibility, Soliton solutions, Radiative heat transfer, Time-dependent Schrödinger equations and Dirac equations, FOS: Mathematics, \(\phi^4\)-equation, nonlinear Schrödinger, 35Q55, 35Q60, 78A60,, Physics - Optics, Analysis of PDEs (math.AP), Optics (physics.optics)
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