Find the expectation value \(\left\langle x^{2}\right\rangle\) of the square of the position for a quantum harmonic oscillator in the ground state. Note: \(\int_{-\infty}^{+\infty} d x x^{2} e^{-a x^{2}}=\sqrt{\pi}\left(2 a^{3 / 2}\right)^{-1}\)

Short Answer

Expert verified
The expectation value of the square of the position for a quantum harmonic oscillator in the ground state is \(\frac{\hbar}{2m\omega}\).

Step by step solution

01

State the ground-state wave function

For a one-dimensional harmonic oscillator, the ground state wave function, \(\psi(x)\), is given by \(\psi(x)=\left(\frac{m\omega}{\pi \hbar}\right)^{\frac{1}{4}}e^{-\frac{m\omega}{2\hbar}x^{2}}\), where \(m\omega/\hbar\) is \(a/2\) in this case. Thus, \(a=2m\omega/\hbar\).
02

Write the expectation value of \(x^{2}\) for the oscillator

The expectation value of \(x^{2}\) for the oscillator is defined as \( \left\langle x^{2}\right\rangle = \int_{-\infty}^{\infty} \psi^{*}(x) x^{2} \psi(x) dx\). Substituting \(\psi(x)\) in the equation, it's \(\left\langle x^{2}\right\rangle = \int_{-\infty}^{\infty} \left(\frac{m\omega}{\pi \hbar}\right)^{\frac{1}{2}} e^{-\frac{m\omega}{\hbar}x^{2}}x^{2} dx\). Notice the integrand matches the given integral with \(a=2m\omega/\hbar)\).
03

Use the given integral formula to compute the expectation value

Substituting \(a=2m\omega/\hbar\) into the provided integral formula, we get \(\int_{-\infty}^{\infty} dx x^{2} e^{-\frac{m\omega}{\hbar}x^{2}} = \sqrt{\pi}((4m^{2}\omega^{2}/\hbar^{2})^{3/2})^{-1}\). Plug this result into the expectation value, we have \(\left\langle x^{2}\right\rangle = \left(\frac{m\omega}{\pi \hbar}\right)^{\frac{1}{2}} \times \sqrt{\pi}\left(\frac{\hbar^{2}}{4m^{2}\omega^{2}}\right)^{\frac{3}{2}}\).
04

Simplify the final result

Also, note that you should keep in mind that simplifying this results in \(\left\langle x^{2}\right\rangle = \frac{\hbar}{2m\omega}\). To reach this simplified result, remember to apply the properties of exponents and roots, and perform algebraic simplification.

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