A Time Reversal and initial conditions

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The discussion centers on the implications of time reversal in the context of the Schrödinger equation, specifically regarding the solutions derived from initial conditions. It is established that while the conjugate wave function ##\psi^*(x,-t)## is indeed a valid solution of the Schrödinger equation, it does not satisfy the same initial conditions as ##\psi(x,t)##. This discrepancy arises because the initial time changes under time reversal, leading to different initial conditions for the two solutions. Participants clarify that having two solutions does not imply degeneracy, as they correspond to different initial states. The conversation highlights the complexities of time reversal symmetry in quantum mechanics.
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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 Schrodinger 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 Schrodinger equation with specific initial conditions?

In the solution of Schrodinger 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.
 
hokhani said:
TL;DR Summary: How can ##\psi^*(x,-t)## be a solution of the Schrodinger equation with specific initial conditions?

In the solution of Schrodinger 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 Schrodinger equation, although with a different initial condition. But since it satisfies the Schrodinger equation, it is a solution. A solution, not the solution.
 
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