Momentum measurement of a particle in Quantum Mechanics

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Homework Help Overview

The discussion revolves around the momentum measurement of a particle in quantum mechanics, specifically focusing on a wave function given by ## \psi = e^{i3x} + 2e^{ix} ##. Participants explore the implications of this wave function for determining momentum and sketching the probability distribution over a specified range.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the eigenfunctions of the momentum operator and their corresponding eigenvalues, questioning the nature of these values in relation to the wave function. There is also exploration of the probability density derived from the wave function and its implications for measurement.

Discussion Status

Some participants have offered insights regarding the normalization of wave functions and the interpretation of coefficients as probability amplitudes. There is an ongoing examination of the relationship between the wave function and the probability distribution, with various interpretations being explored.

Contextual Notes

Participants note the challenge of dealing with continuous eigenvalues and the implications for probability calculations. There is also mention of the need to sketch the probability distribution, which adds another layer to the problem context.

Pushoam
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Homework Statement



What will momentum measurement of a particle whose wave - function is given by ## \psi = e^{i3x} + 2e^{ix} ## yield?
Sketch the probability distribution of finding the particle between x = 0 to x = 2π.

Homework Equations


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The Attempt at a Solution


The eigenfunctions of momentum operator is given by ## A e^{ikx}## where k = ## \frac p {\hbar} ## with eigen value p = ## {\hbar} k##.
Thus eigenvalue of ##e^{i3x}## is ## 3 \hbar ## and ##e^{ix}## is ## \hbar ##. I feel myself tempted to take the eigenvalues of momentum operator to be discrete and say that the momentum measurement will be either ## 3 \hbar ## or ## \hbar ##.
As the eigenvalue of momentum operator is continuous, I should use equation. (3.56) to answer the question.

Assuming that the question asks to calculate the probability distribution at t = 0, probability density would be given by ## | \psi |^2 = 3 + 2 ( e^{ i2x} +e^{-i2x} )##., a complex function. But, the probability density should be a real valued function.
Is this correct?
 

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Plane waves are not normalizable so you really cannot write the probability in that manner (the wave function in momentum space is a sum of two delta functions). However, given the coefficients you should be able to deduce the probabilities (the coefficients are the probability amplitudes) by assuming that the total probability is one.
 
Orodruin said:
the coefficients are the probability amplitudes
How does one get to know this in case of continuous eigenvalues?
 
Pushoam said:
Assuming that the question asks to calculate the probability distribution at t = 0, probability density would be given by ## | \psi |^2 = 3 + 2 ( e^{ i2x} +e^{-i2x} )##., a complex function. But, the probability density should be a real valued function.
Is this correct?
I think you made a slight error. Anyway, your expression for ##| \psi |^2## is real.
 
vela said:
I think you made a slight error. Anyway, your expression for ##| \psi |^2## is real.
However, it does not answer the question since it is the momenta that are asked for, not the position.
 
Part of the question asked for a sketch of the probability as a function of ##x##.
 
vela said:
Part of the question asked for a sketch of the probability as a function of ##x##.
That's what I get for reading too fast ...
 

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