TheBigDig
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1. The problem statement
Consider a particle of mass m under the action of the one-dimensional harmonic oscillator potential. The Hamiltonian is given by
H = \frac{p^2}{2m} + \frac{m \omega ^2 x^2}{2}
Knowing that the ground state of the particle at a certain instant is described by the wave function
\psi(x) = (\frac{m \omega}{\pi \hbar})^\frac{1}{4} e^{-\frac{m \omega x^2}{2 \hbar}}
calculate (for the ground state)
a) the mean value of the position <x>
b) the mean value of the position squared <x2>
c) the mean value of the momentum <p>
d) the mean value of the momentum squared <p2>
H = \frac{p^2}{2m} + \frac{m \omega ^2 x^2}{2}
<x^2> = \int_{-\infty}^{\infty} \psi^*(x) x^2 \psi(x) dx
<p^2> = - \hbar ^2 \int_{-\infty}^{\infty} \psi^*(x) \frac{\partial^2 \psi(x)}{\partial x^2} dx
My question relates to the fourth part of the question so I'll give the first three answers here.
a) <x> = 0
b) <x^2> = \frac{\hbar}{2m \omega}
c) <p> = 0
I attempted to relate <p2> to <x2> by assuming that
H = E = E_k + V = \frac{p^2}{2m} + \frac{1}{2} m \omega^2 x^2 and using the ground state energy of a harmonic oscillator:
E = \frac{1}{2} \hbar \omega
I then took the expectation value of both sides
<E> = \frac{1}{2} \hbar \omega = \frac{1}{2m} <p^2> + \frac{1}{2} m \omega^2 <x^2>
\frac{1}{2} \hbar \omega = \frac{1}{2m}<p^2>+\frac{1}{2}m \omega^2 \frac{\hbar}{2m\omega}
\frac{1}{2} \hbar \omega = \frac{1}{2m}<p^2> + \frac{1}{4}\hbar \omega
<p^2> = \frac{1}{2} m \omega \hbar
I'm just not sure if I'm correct in my assumptions. Can I assume H = E in this situation?
Consider a particle of mass m under the action of the one-dimensional harmonic oscillator potential. The Hamiltonian is given by
H = \frac{p^2}{2m} + \frac{m \omega ^2 x^2}{2}
Knowing that the ground state of the particle at a certain instant is described by the wave function
\psi(x) = (\frac{m \omega}{\pi \hbar})^\frac{1}{4} e^{-\frac{m \omega x^2}{2 \hbar}}
calculate (for the ground state)
a) the mean value of the position <x>
b) the mean value of the position squared <x2>
c) the mean value of the momentum <p>
d) the mean value of the momentum squared <p2>
Homework Equations
H = \frac{p^2}{2m} + \frac{m \omega ^2 x^2}{2}
<x^2> = \int_{-\infty}^{\infty} \psi^*(x) x^2 \psi(x) dx
<p^2> = - \hbar ^2 \int_{-\infty}^{\infty} \psi^*(x) \frac{\partial^2 \psi(x)}{\partial x^2} dx
The Attempt at a Solution
My question relates to the fourth part of the question so I'll give the first three answers here.
a) <x> = 0
b) <x^2> = \frac{\hbar}{2m \omega}
c) <p> = 0
I attempted to relate <p2> to <x2> by assuming that
H = E = E_k + V = \frac{p^2}{2m} + \frac{1}{2} m \omega^2 x^2 and using the ground state energy of a harmonic oscillator:
E = \frac{1}{2} \hbar \omega
I then took the expectation value of both sides
<E> = \frac{1}{2} \hbar \omega = \frac{1}{2m} <p^2> + \frac{1}{2} m \omega^2 <x^2>
\frac{1}{2} \hbar \omega = \frac{1}{2m}<p^2>+\frac{1}{2}m \omega^2 \frac{\hbar}{2m\omega}
\frac{1}{2} \hbar \omega = \frac{1}{2m}<p^2> + \frac{1}{4}\hbar \omega
<p^2> = \frac{1}{2} m \omega \hbar
I'm just not sure if I'm correct in my assumptions. Can I assume H = E in this situation?