Stationary State: Energy & Time-Independent Wave Function

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In summary, in quantum mechanics, the wave function of a stationary state has a time-dependent exponential factor that has no physical significance and is just a mathematical redundancy. This factor also does not affect the probability or energy of the system. In non-stationary states, the time-dependent factor still exists and can affect the state's energy, but it is not considered a physical state in the Hilbert space. The true representation of a state is a ray, where all vectors with a time-dependent phase factor belong to the same ray and do not affect the expectation values of operators.
  • #1
KFC
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For stationary state, the energy of the system is constant and time-independent, so for some specific form of potential, the Schrodinger can be variable separated such that the general solution will be


[tex]
\psi(x, t) = \phi(x) \exp(-iE t /\hbar)
[/tex]

The probability is given by the square of the wave function so the arbitrary phase factor [tex]\exp(iE t/\hbar)[/tex] in above solution doesn't matter. However, if we consider the wave function itself, what's the meaning of the time-dependent factor [tex]\exp(iE t/\hbar)[/tex]. If it is stationary, why wavefunction is depending on time?


By the way, if the solution is non-stationary, is it no more any definite energy level? So in this case, there is no corresponding eigenvalue problem?
 
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  • #2
In quantum mechanics, wave function is actually not a good description of a quantum state. It is a redundant description. Two wave functions that differ only by a multiplicative (phase) factor correspond to the same physical state. So, the exponential time-dependent factor present in the wave function of any stationary state has no physical significance. It is just a mathematical redundancy.
 
  • #3
KFC said:
For stationary state, the energy of the system is constant and time-independent, so for some specific form of potential, the Schrodinger can be variable separated such that the general solution will be


[tex]
\psi(x, t) = \phi(x) \exp(-iE t /\hbar)
[/tex]

The probability is given by the square of the wave function so the arbitrary phase factor [tex]\exp(iE t/\hbar)[/tex] in above solution doesn't matter. However, if we consider the wave function itself, what's the meaning of the time-dependent factor [tex]\exp(iE t/\hbar)[/tex].

The meaning is just what you have indicated by using the symbol 'E'; the time-dependence of the state tells us the energy 'E'.

If it is stationary, why wavefunction is depending on time?

Even the "stationary" state depends on time but the dependence is "trivial". I.e., a simple exponential e^(-iEt).


By the way, if the solution is non-stationary, is it no more any definite energy level? So in this case, there is no corresponding eigenvalue problem?

You can still solve the eigenvalue problem
[tex]
\hat H \psi = E \psi\;,
[/tex]
and obtain the energy eigenvalues and they are still useful. For example, suppose you know that the state of the systems at t=0 is
[tex]
\Phi=a\phi_1+b\phi_2\;,
[/tex]
where \phi_1 and \phi_2 are eigenfunctions of the eigenvalue problem with eigenvalues E_1 and E_2, respectively. Knowing this you can determine the time dependence of the state \Phi, which is not "trivial" since \Phi is not an eigenstate of the hamiltonian (unless E_1=E_2).
 
  • #4
KFC said:
The probability is given by the square of the wave function
No it's not, it's given by the square of the modulus of the wave function. The modulus of exp(ikt) will always be 1, so it has no direct affect on the probabilities. However, when you combine two systems, then there is a possibility of interference, which is explained by the combination of the phases.
 
  • #5
meopemuk said:
So, the exponential time-dependent factor present in the wave function of any stationary state has no physical significance. It is just a mathematical redundancy.

Time dependent phase factors are not redundant. A constant phase factor is redundant, but multiplying by a time dependent factor changes many things of physical relevance, such as the energy.
 
  • #6
dx said:
Time dependent phase factors are not redundant. A constant phase factor is redundant, but multiplying by a time dependent factor changes many things of physical relevance, such as the energy.

In the Hilbert space the true representation of a state is not a vector [tex] |\Psi \rangle[/tex] but a ray (1-dimensional subspace containing [tex] |\Psi \rangle[/tex]). All vectors of the form [tex] \alpha(t)|\Psi \rangle[/tex] (where [tex]\alpha(t) [/tex] is any numerical function of [tex]t[/tex]) belong to the same ray. Expectation values of all operators (e.g., energy) do not depend on the form of [tex]\alpha(t) [/tex], so this phase factor is completely irrelevant for physics.
 

1. What is a stationary state in quantum mechanics?

A stationary state in quantum mechanics refers to a state in which a physical system has a constant value of energy and does not change over time. This is described by a wave function that is time-independent.

2. How is energy related to stationary states?

In quantum mechanics, energy is a measurable quantity that is associated with a stationary state. The energy of a stationary state is constant and does not change over time.

3. What is the significance of time-independence in stationary states?

The time-independence of a stationary state means that the state remains the same over time. This is important because it allows us to make predictions about the behavior of a system without having to constantly consider changes in time.

4. How is the wave function related to stationary states?

The wave function is a mathematical representation of a quantum system, and in stationary states it is time-independent. This means that the wave function does not change over time and can be used to describe the energy and behavior of the system.

5. Can a physical system be in more than one stationary state at a time?

Yes, a physical system can be in a superposition of multiple stationary states at once. This means that it has a combination of energies and behaviors from each state, and the overall wave function is a combination of the individual stationary state wave functions.

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