Answer on Question #85011 Physics / Quantum Mechanics
Calculate the mean kinetic and potential energies of a simple harmonic oscillator which is in its ground state.
Solution:
In the ground state the wave function and energy of a simple harmonic oscillator
ψ 0 ( x ) = ( m ω π ℏ ) 1 4 exp ( − m ω x 2 2 ℏ ) \psi_ {0} (x) = \left(\frac {m \omega}{\pi \hbar}\right) ^ {\frac {1}{4}} \exp \left(- \frac {m \omega x ^ {2}}{2 \hbar}\right) ψ 0 ( x ) = ( π ℏ mω ) 4 1 exp ( − 2ℏ mω x 2 ) E 0 = ℏ ω 2 E _ {0} = \frac {\hbar \omega}{2} E 0 = 2 ℏ ω
The mean kinetic energy
⟨ K ⟩ = ∫ − ∞ ∞ ψ 0 ( x ) ( − ℏ 2 2 m d 2 d x 2 ) ψ 0 ( x ) d x = ℏ 2 2 m ( m ω π ℏ ) 1 2 ∫ − ∞ ∞ exp ( − m ω x 2 ℏ ) ( m ω ℏ − m 2 ω 2 ℏ 2 x 2 ) d x = ℏ 2 2 m ( m ω π ℏ ) 1 2 ( m ω ℏ π ℏ m ω − m 2 ω 2 ℏ 2 ℏ 2 m ω π ℏ m ω ) = ℏ ω 4 \begin{aligned}
\langle K \rangle &= \int_{-\infty}^{\infty} \psi_ {0} (x) \left(- \frac {\hbar^ {2}}{2 m} \frac {d ^ {2}}{d x ^ {2}}\right) \psi_ {0} (x) d x \\
&= \frac {\hbar^ {2}}{2 m} \left(\frac {m \omega}{\pi \hbar}\right) ^ {\frac {1}{2}} \int_{-\infty}^{\infty} \exp \left(- \frac {m \omega x ^ {2}}{\hbar}\right) \left(\frac {m \omega}{\hbar} - \frac {m ^ {2} \omega ^ {2}}{\hbar^ {2}} x ^ {2}\right) d x \\
&= \frac {\hbar^ {2}}{2 m} \left(\frac {m \omega}{\pi \hbar}\right) ^ {\frac {1}{2}} \left(\frac {m \omega}{\hbar} \sqrt {\frac {\pi \hbar}{m \omega}} - \frac {m ^ {2} \omega^ {2}}{\hbar^ {2}} \frac {\hbar}{2 m \omega} \sqrt {\frac {\pi \hbar}{m \omega}}\right) = \frac {\hbar \omega}{4}
\end{aligned} ⟨ K ⟩ = ∫ − ∞ ∞ ψ 0 ( x ) ( − 2 m ℏ 2 d x 2 d 2 ) ψ 0 ( x ) d x = 2 m ℏ 2 ( π ℏ mω ) 2 1 ∫ − ∞ ∞ exp ( − ℏ mω x 2 ) ( ℏ mω − ℏ 2 m 2 ω 2 x 2 ) d x = 2 m ℏ 2 ( π ℏ mω ) 2 1 ( ℏ mω mω π ℏ − ℏ 2 m 2 ω 2 2 mω ℏ mω π ℏ ) = 4 ℏ ω
The mean potential energy
⟨ V ⟩ = E 0 − ⟨ K ⟩ = ℏ ω 2 − ℏ ω 4 = ℏ ω 4 \langle V \rangle = E _ {0} - \langle K \rangle = \frac {\hbar \omega}{2} - \frac {\hbar \omega}{4} = \frac {\hbar \omega}{4} ⟨ V ⟩ = E 0 − ⟨ K ⟩ = 2 ℏ ω − 4 ℏ ω = 4 ℏ ω
Answer: ⟨ K ⟩ = ⟨ V ⟩ = ℏ ω 4 \langle K\rangle = \langle V\rangle = \frac{\hbar\omega}{4} ⟨ K ⟩ = ⟨ V ⟩ = 4 ℏ ω
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