What are the Expectations for Momentum and Energy in Quantum Mechanics?

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The discussion focuses on calculating the expectation values for momentum and energy in quantum mechanics using the defined operators. The momentum operator is expressed as \(\hat{p} = \hbar / i \frac{\partial }{\partial x}\) and the energy operator as \(\hat{E} = i \hbar \frac{\partial }{\partial t}\). The expectation values are derived using the wave function \(\psi(x,t)\) through integrals involving the wave function and its derivatives. Specifically, the formulas for \(\langle p \rangle\), \(\langle E \rangle\), and \(\langle p^2 \rangle\) are provided, emphasizing the integration of the wave function's complex conjugate with respect to position and time. This discussion highlights the mathematical framework for determining momentum and energy expectations in quantum systems.
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Homework Statement


We have a particle of mass m and potential energy V(x), wavefn \psi(x,t)
What are the expectations for the momentum p_x, p_x^2 and the energy.
 
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We have momentum and energy operators that we can use here. The momentum operator is \hat{p} and the energy operator is \hat{E} where
\hat{p} = \hbar / i \frac{\partial }{\partial x}
and
\hat{E} = i \hbar \frac{\partial }{\partial t}

For any function g(x) we have the expectation value as:

\langle g(x) \rangle = \int^{\infty}_{-\infty} \psi^\star (x,t) g(x) \psi (x,t)\,dx

Then we have

\langle p \rangle = \hbar / i \int^\infty_{-\infty} \psi^\star (x,t) \frac{\partial }{\partial x} \psi (x,t)\,dx

and

\langle E \rangle = i \hbar \int^\infty_{-\infty} \psi^\star (x,t) \frac{\partial }{\partial t} \psi (x,t)\,dx

and also

\langle p^2 \rangle = \hbar^2 \int^\infty_{-\infty} \psi^\star (x,t) \frac{\partial^2 }{\partial x^2} \psi (x,t)\,dx
 
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