Expectation value of momentum for bound states

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SUMMARY

The expectation value of momentum for any bound state in quantum mechanics is definitively zero. This conclusion is derived from the integral formulation involving the wavefunction, where the wavefunction's parity (even or odd) leads to the first derivative having opposite parity, resulting in a zero integral. For symmetric potentials, all bound states exhibit definite parity, confirming the zero expectation value of momentum. However, for asymmetric potentials, while the eigenfunctions lack definite parity, the expectation value of momentum may still be zero under certain conditions, as clarified by Ehrenfest's theorem.

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  • Understanding of quantum mechanics principles, particularly wavefunctions and their properties.
  • Familiarity with the concept of parity in quantum states.
  • Knowledge of Ehrenfest's theorem and its implications in quantum mechanics.
  • Basic calculus for evaluating integrals involving wavefunctions.
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blue_leaf77
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Homework Statement


I'm curious in proving that expectation value of momentum for any bound state is zero. So the problem is how to prove this.

Homework Equations


$$ \langle \mathbf{p_n} \rangle \propto \int \psi^*(\mathbf{r_1}, \dots ,\mathbf{r_N}) \nabla_n \psi(\mathbf{r_1}, \dots ,\mathbf{r_N}) d^3\mathbf{r_1} \dots d^3\mathbf{r_N} $$
where ## n = 1,2, \dots N ##.

The Attempt at a Solution


If I assume that ## \psi(\mathbf{r_1}, \dots ,\mathbf{r_N}) ## is either even or odd then its first derivative will be its counterpart, so ## \nabla_n \psi(\mathbf{r_1}, \dots ,\mathbf{r_N}) ## has opposite parity in ## \mathbf{r_n} ##. Thus the integral will result zero.
My question is that is this true that all bound states can only be even or odd? If yes why?
 
Last edited:
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All bound states of symmetric potentials have a definite parity.

This can be shown because in that case the entire Hamiltonian will have even parity, and will be invariant under a coordinate swap.

Whether this is true for bound states of asymmetric potentials (say three randomly placed square wells), I couldn't say. The wavefunctions would no longer have definite parity, but it may yet be the case that the expectation of the momentum is still zero.
 
Last edited:
Okay, the eigenfunctions would definitely not have a definite parity if the potential is asymmetric. As an extreme example, consider the potential, which is an infinite square well for x<0, and is a quadratic potential (a quantum spring) for x\geq 0. Here the eigenfunctions are definitely zero for x\leq 0, and nonzero for x> 0.
 
So is there a more formal way to prove that expectation value of momentum for bound states is zero?
 
Yes there is.
Ehrenfest's theorem.
 
Ok thank you very much, now it's pretty clear why it should be zero for bound states. But first my question is does this theorem also applicable to free particle? If yes then the momentum of free particle is zero??
 
For the free particle, the expectation of the position need not be a constant value like it would need to be for a bound state. Because of this, the expectation for the momentum need not be zero.

Whenever the expectation of the position is constant, the expectation of the momentum will be zero.
 
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