Help Proving the Momentum Shift Operator

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SUMMARY

The discussion focuses on proving the momentum expectation value shift under the transformation of the wave function by a phase factor, specifically showing that <p_x> transforms to <p_x> + p_0 when ψ(x) → e^{i p_0 x / ħ} ψ(x). Using the momentum operator &hat;p_x = (ħ/i) ∂/∂x and the product rule for differentiation, the key step is recognizing that the derivative of the exponential factor introduces the additive p_0 term. The textbook referenced is "A Modern Approach to Quantum Mechanics, 2nd edition" by John S. Townsend. The final conclusion confirms that the momentum expectation value shifts by p_0 due to the phase factor multiplication in the position basis wave function.

PREREQUISITES

  • Quantum mechanics operator formalism, specifically momentum operator &hat;p_x = (ħ/i) ∂/∂x
  • Wave function transformations in position representation
  • Application of the product rule in differentiation of complex exponentials
  • Understanding of expectation value calculations in quantum mechanics

NEXT STEPS

  • Study the derivation of momentum operator expectation values in position space
  • Review the product rule for differentiation applied to complex exponential functions
  • Explore phase transformations and their effects on quantum observables
  • Consult "A Modern Approach to Quantum Mechanics" by John S. Townsend for detailed operator proofs

USEFUL FOR

Quantum mechanics students, physics educators, and researchers working on operator methods and wave function transformations will benefit from this discussion. It is particularly useful for those studying momentum operator properties and phase shift effects in quantum systems.

Danielk010
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I need help proving given
I am stuck on proving:
##\langle p_x \rangle \rightarrow \langle p_x \rangle + p_0## given ##\langle x \mid \psi \rangle \;\rightarrow\; e^{i p_0 x / \hbar}\,\langle x \mid \psi \rangle##
I was able to prove given the change in wave function mentioned above: ##\langle x \rangle \rightarrow\; \langle x \rangle## by using
$$ \langle x \rangle = \int dx \, \langle \psi | x \rangle x \langle x | \psi \rangle $$ and plugging in the modified wave function and the complex conjugate of the modified wave function.

The textbook, A Modern Approach to Quantum Mechanics, 2nd edition by John S. Townsend, gives me these equations:

$$
\langle p_x \rangle = \langle \psi | \hat{p}_x | \psi \rangle = \int dx' \, \langle \psi | x' \rangle \frac{\hbar}{i} \frac{\partial}{\partial x'} \langle x' | \psi \rangle

= \int dx' \, \psi^*(x') \frac{\hbar}{i} \frac{\partial}{\partial x'} \psi(x') = \int dx \, \psi^*(x) \frac{\hbar}{i} \frac{\partial}{\partial x} \psi(x)
$$
I tried taking the deriative of ##e^{i p_0 x / \hbar}## to get the ##p_0## term, but that changes the ##\langle p_x \rangle## equation. Am I looking at the right equations or was I going in the right direction? Is there any hint you could give for this problem? Thank you any help on this problem.
 
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Danielk010 said:
Is there any hint you could give for this problem? Thank you any help on this problem.
Under the transformation ##\psi\left(x\right)\rightarrow e^{ip_{0}x/\hbar}\,\psi\left(x\right)## we have:$$\left\langle p_{x}\right\rangle \equiv\int dx\,\psi^{*}\left(x\right)\frac{\hbar}{i}\frac{d}{dx}\psi\left(x\right)\rightarrow\int dx\,\left[e^{-ip_{0}x/\hbar}\,\psi^{*}\left(x\right)\right]\frac{\hbar}{i}\frac{d}{dx}\left[e^{ip_{0}x/\hbar}\,\psi\left(x\right)\right]=\,?$$Can you "turn the crank" from here to finish the derivation?
 
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renormalize said:
Under the transformation ##\psi\left(x\right)\rightarrow e^{ip_{0}x/\hbar}\,\psi\left(x\right)## we have:$$\left\langle p_{x}\right\rangle \equiv\int dx\,\psi^{*}\left(x\right)\frac{\hbar}{i}\frac{d}{dx}\psi\left(x\right)\rightarrow\int dx\,\left[e^{-ip_{0}x/\hbar}\,\psi^{*}\left(x\right)\right]\frac{\hbar}{i}\frac{d}{dx}\left[e^{ip_{0}x/\hbar}\,\psi\left(x\right)\right]=\,?$$Can you "turn the crank" from here to finish the derivation?

From the rightmost part of the equation,
$$\int dx \, \psi^*(x) \frac{\hbar}{i} \frac{\partial}{\partial x} \psi(x) (e^{{-i p_0 x / \hbar} + {i p_0 x / \hbar}})$$
which should make ## \langle p \rangle ## = ## \langle p \rangle ##, not ## \langle p \rangle ## = ## \langle p \rangle + p_0 ##. Did I make a mistake in my calculation? Is this what you meant by "turn the crank"? Am I missing some mathematic trick? There is probably something wrong with my calculation given the problem statement. Thank you for the help.
 
Danielk010 said:
Did I make a mistake in my calculation?
Yes you did. You should have:$$\frac{\hbar}{i}\frac{d}{dx}\left[e^{ip_{0}x/\hbar}\,\psi\left(x\right)\right]=e^{ip_{0}x/\hbar}\left[p_{0}\psi\left(x\right)+\frac{\hbar}{i}\frac{d}{dx}\psi\left(x\right)\right]$$Do you understand how to apply the product rule for differentiation and how to take the derivative of an exponential function?
 
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I do understand how to apply the product rule for differentiation and take the derivative of the exponential function. Thank you so much for the help. I got the answer.
 
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