Question #44133

For the ground state of linear harmonic oscillator calculate average value of "x" and "x^2".

Expert's answer

Answer on Question #44133-Physics-Quantum Mechanics

For the ground state of linear harmonic oscillator calculate average value of "x" and "x^2".

Solution

For the ground state of the harmonic oscillator, the expectation value of the position operator xx is given by


<x>0=ψ0(x)xψ0(x)dx,< x >_0 = \int \psi_0^*(x) \cdot x \cdot \psi_0(x) \, dx,


where


ψ0(x)=(mωπ)14emω2x2.\psi_0(x) = \left(\frac{m\omega}{\pi\hbar}\right)^{\frac{1}{4}} e^{-\frac{m\omega}{2\hbar}x^2}.<x>0=mωπxemωx2dx=0.< x >_0 = \int_{-\infty}^{\infty} \sqrt{\frac{m\omega}{\pi\hbar}} \cdot x \cdot e^{-\frac{m\omega}{\hbar}x^2} \, dx = 0.


The fact that this expression vanishes can be seen either by brute force calculation, or by symmetry (the integrand is odd and the limits of integration are symmetric).

The expectation value of x2x^2, however, doesn't vanish:


<x2>0=ψ0(x)x2ψ0(x)dx=mωπx2emωx2dx.< x^2 >_0 = \int \psi_0^*(x) \cdot x^2 \cdot \psi_0(x) \, dx = \int_{-\infty}^{\infty} \sqrt{\frac{m\omega}{\pi\hbar}} \cdot x^2 \cdot e^{-\frac{m\omega}{\hbar}x^2} \, dx.


Here is a useful trick: knowing the fundamental integral ecx2dx=πc\int_{-\infty}^{\infty} e^{-cx^2} \, dx = \sqrt{\frac{\pi}{c}}, we can take a derivative with respect to cc to obtain


x2ecx2dx=ddcecx2dx=ddc(πc)=π2c2.\int_{-\infty}^{\infty} x^2 e^{-cx^2} \, dx = -\frac{d}{dc} \int_{-\infty}^{\infty} e^{-cx^2} \, dx = -\frac{d}{dc} \left(\sqrt{\frac{\pi}{c}}\right) = \frac{\sqrt{\pi}}{2c^2}.


Here c=mωc = \frac{m\omega}{\hbar}, and thus


<x2>0=mωπx2emωx2dx=mωπ12π3m3ω3=2mω.< x^2 >_0 = \int_{-\infty}^{\infty} \sqrt{\frac{m\omega}{\pi\hbar}} \cdot x^2 \cdot e^{-\frac{m\omega}{\hbar}x^2} \, dx = \sqrt{\frac{m\omega}{\pi\hbar}} \frac{1}{2} \sqrt{\frac{\pi\hbar^3}{m^3\omega^3}} = \frac{\hbar}{2m\omega}.


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