Answer to Question #163897 in Quantum Mechanics for Nidhin S

Question #163897

 Show that < 𝑥𝑝 > − < 𝑝𝑥 > = 𝑖ħ for the ground state wave function of the Quantum 

Harmonic Oscillator (QHO)


1
Expert's answer
2021-02-16T10:28:41-0500

The QHO ground state wave function is given by ψ(x)=(mωπ)1/4emωx22\psi(x) = (\frac{m\omega}{\pi \hbar})^{1/4} e^{-\frac{m \omega x^2}{2\hbar}}. In coordinate representation, x^=x,p^=ix\hat{x} = x, \hat{p} =- i\hbar \frac{\partial}{\partial x} and thus we find :

<x^p^>ψ=+x(imωx)ψ2(x)dx<\hat x \hat p >_\psi = \int_{-\infty}^{+\infty} x\cdot (i\hbar\frac{m\omega x}{\hbar})\cdot \psi^2(x) dx, applying the integration by parts (u=x,dv=imωxψ2dxu = x, dv = im\omega x \psi^2 dx) we find <x^p^>ψ=[12xψ2]++12iψ2dx=i2<\hat x \hat p >_\psi = [\frac{1}{2}x\psi^2]^{+\infty}_{-\infty} + \frac{1}{2}i\hbar \int \psi^2 dx =\frac{ i\hbar}{2} as ψ\psi is a normalised wave function.

Now we calculate <p^x^>ψ=i(ψ2+xψψ)dx<\hat p \hat x>_\psi = -i\hbar \int (\psi^2+x\psi \psi')dx. The integral iψ2dx=i-i\hbar \int \psi^2dx =-i\hbar is given by the normalisation of ψ\psi. The second integral was calculated previously. Thus we find <p^x^>ψ=i/2<\hat p \hat x>_\psi = -i\hbar /2 .

Thus <xppx>ψ=i<xp-px>_\psi = i\hbar which is coherent with the fact that [x,p]=iId[x,p]=i\hbar \cdot Id and thus <[x,p]>ψ=i<[x,p]>_\psi = i\hbar for any normalised wave function ψ\psi.


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