Time Reversal and initial conditions

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Discussion Overview

The discussion revolves around the implications of time reversal in the context of the Schrödinger equation, specifically examining the relationship between the wave function solutions and their initial conditions. Participants explore how the conjugate wave function behaves under time reversal and the consistency of initial conditions for different solutions.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants note that the solution ##\psi(x,t)## of the Schrödinger equation depends on the initial condition at time ##t=t_0##, and question how ##\psi^*(x,-t)## can be a solution while not satisfying the same initial conditions.
  • Others argue that for certain cases, such as when considering a time-independent Hamiltonian, the initial conditions can lead to different wave functions, specifically noting that ##\psi^*(x,-t_0) \ne \psi(x,t_0)##.
  • One participant highlights that time reversal changes the initial time, thus affecting the initial conditions associated with the wave function.
  • Another participant emphasizes that while ##\psi^*(x,-t)## satisfies the Schrödinger equation, it does so under different initial conditions, leading to the conclusion that it is a solution but not necessarily the same solution as ##\psi(x,t)##.
  • There is a discussion about whether the existence of two solutions for a single initial condition implies double degeneracy for time-independent Hamiltonians, with participants expressing differing views on this point.

Areas of Agreement / Disagreement

Participants generally disagree on the implications of time reversal and the relationship between the initial conditions of the wave functions. There is no consensus on whether the existence of two solutions implies double degeneracy, and the discussion remains unresolved regarding the nature of the solutions under time reversal.

Contextual Notes

Participants acknowledge that the initial conditions must be conjugated under time reversal, but the specifics of how this affects the solutions remain contested. The discussion also touches on the implications of different initial times and their effects on the wave functions.

hokhani
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TL;DR
How can ##\psi^*(x,-t)## be a solution of the Schrodinger equation with specific initial conditions?
In the solution of Schrödinger equation, ##H\psi =i\hbar \frac{\partial \psi}{\partial t}##, the solution ##\psi(x,t)## depends on the initial condition at ##t=t_0##. It is mentioned in the literatures that if ##H=H^*## then ##\psi^*(x,-t)## is another solution. However, ##\psi^*(x,-t)## is not consistent with the initial condition. In other words, ##\psi^*(x,-t_0) \ne \psi(x,t_0) ##! Any help is appreciated.
 
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hokhani said:
In other words, ##\psi^*(x,-t_0) \ne \psi(x,t_0) ##!
Why not? For the simplest case, consider a time-dependent part of the wave function at ##t = t_0## to have a well-known form ##\psi(t_0) = \exp\left(-\frac{\mathrm{i}}{\hbar} E t_0\right)##, with ##E## the eigenvalue of the Hamiltonian. Now, write down the corresponding ##\psi^*(-t_0)## and make use of the fact that ##E## is a real number (because it is an eigenvalue of the Hermitian operator). You will immediately see that, in fact, ##\psi^*(-t_0) = \psi(t_0)##.
 
div_grad said:
Why not? For the simplest case, consider a time-dependent part of the wave function at ##t = t_0## to have a well-known form ##\psi(t_0) = \exp\left(-\frac{\mathrm{i}}{\hbar} E t_0\right)##, with ##E## the eigenvalue of the Hamiltonian. Now, write down the corresponding ##\psi^*(-t_0)## and make use of the fact that ##E## is a real number (because it is an eigenvalue of the Hermitian operator). You will immediately see that, in fact, ##\psi^*(-t_0) = \psi(t_0)##.
Thanks, you have considered only the time-dependent part of the simplest case of time-independent Hamiltonian. Consider the free particle case with the initial condition ##\psi(x,t_0=0)=e^{ikx}## and then,
$$\psi(x,t)=e^{- \frac{iEt}{\hbar}} e^{ikx}$$ and so $$\psi^*(x,-t)=e^{- \frac{iEt}{\hbar}} e^{-ikx}.$$ In this case: ##\psi^*(x,0)=e^{-ikx} \ne \psi(x,0) =e^{ikx}##.
 
hokhani said:
TL;DR Summary: How can ##\psi^*(x,-t)## be a solution of the Schrödinger equation with specific initial conditions?

In the solution of Schrödinger equation, ##H\psi =i\hbar \frac{\partial \psi}{\partial t}##, the solution ##\psi(x,t)## depends on the initial condition at ##t=t_0##. It is mentioned in the literatures that if ##H=H^*## then ##\psi^*(x,-t)## is another solution. However, ##\psi^*(x,-t)## is not consistent with the initial condition. In other words, ##\psi^*(x,-t_0) \ne \psi(x,t_0) ##! Any help is appreciated.
"Initial conditions" means the state of the system at some "initial" time, ##t_0##. Unless ##t_0 = 0##, then the initial time changes under time reversal. The initial time is now at ##-t_0##.

The same applies to parabolic motion under gravity. There is time reversal symmetry, but the time coordinate associated with "initial" conditions must change.

More generally, under any transformation, the coordinates of the initial event change. If an initial event is at the spatial origin and you move the origin of your coordinate system, then the initial event is longer at the origin. That should be clear.
 
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PeroK said:
"Initial conditions" means the state of the system at some "initial" time, ##t_0##. Unless ##t_0 = 0##, then the initial time changes under time reversal. The initial time is now at ##-t_0##.
In the example I sent in the post #3 the initial time is ##t_0=0## which gives different initial conditions for the two solutions.
 
hokhani said:
In the example I sent in the post #3 the initial time is ##t_0=0## which gives different initial conditions for the two solutions.
Time reversal in the SDE requires the conjugate wavefunction - as stated.
 
PeroK said:
Time reversal in the SDE requires the conjugate wavefunction - as stated.
Thanks, do you approve that the initial condition for time reversal solution is different from the main solution? If no, can we say that for one initial condition we have two solutions for SDE? If yes, we would have at least double degeneracy for most of time independent Hamiltonians!
 
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hokhani said:
Thanks, do you approve that the initial condition for time reversal solution is different from the main solution? If no, can we say that for one initial condition we have two solutions for SDE? If yes, we would have at least double degeneracy for most of time independent Hamiltonians!
You can't ask whether the conjugate wavefunction is a solution and demand that at some initial time it is not the conjugate. The initial condition is the wavefunction at some chosen time. That must also be conjugated.
 
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hokhani said:
TL;DR Summary: How can ##\psi^*(x,-t)## be a solution of the Schrödinger equation with specific initial conditions?

In the solution of Schrödinger equation, ##H\psi =i\hbar \frac{\partial \psi}{\partial t}##, the solution ##\psi(x,t)## depends on the initial condition at ##t=t_0##. It is mentioned in the literatures that if ##H=H^*## then ##\psi^*(x,-t)## is another solution. However, ##\psi^*(x,-t)## is not consistent with the initial condition. In other words, ##\psi^*(x,-t_0) \ne \psi(x,t_0) ##! Any help is appreciated.
Nobody said that ##\psi^*(x,-t)## satisfies the same initial conditions as ##\psi(x,t)##. It doesn't. ##\psi^*(x,-t)## satisfies the same Schrödinger equation, although with a different initial condition. But since it satisfies the Schrödinger equation, it is a solution. A solution, not the solution.
 
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