Expectation value of momentum operator

In summary: You can use Wolfram Alpha or some other graphing tool to look at this function. Note that it is real and has a maximum at ##x = 0##. Therefore, <p> must be 0.Try ##\psi(x) = e^{-x^2}## and don't worry about the normalisation constant. You can use Wolfram Alpha or some other graphing tool to look at this function. Note that it is real and has a maximum at ##x = 0##. Therefore, <p> must be 0.In summary, the eigenstates of the momentum operator are given by exp(ikx). To construct a real-valued and normalized wavefunction out of these
  • #1
tanaygupta2000
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14
Homework Statement
Find the expectation value of momentum operator in a normalized real-valued wavefunction
Relevant Equations
momentum eigenstates = exp(ikx)
Q2.PNG


I know that the eigenstates of momentum operator are given by exp(ikx)
To construct a real-valued and normalized wavefunction out of these eigenstates,
I have,
psi(x) = [exp(ikx) + exp(-ikx)]/ sqrt(2)

But my trouble is, how do I find the expectation value of momentum operator <p> using this psi(x)?
On applying momentum operator, my integral is divergent.
I think that since there are equal probabilities in psi, <p> will be 0.
But how do I show it by calculations?
Please help!
 
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  • #2
[tex]<p>=\int \psi^*(x) \frac{\hbar}{i}\frac{d}{dx} \psi(x) dx[/tex]
is usual way of momentum calculation. Say ##\psi(x)## is real function ?
 
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  • #3
tanaygupta2000 said:
Homework Statement:: Find the expectation value of momentum operator in a normalized real-valued wavefunction
Relevant Equations:: momentum eigenstates = exp(ikx)

View attachment 278349

I know that the eigenstates of momentum operator are given by exp(ikx)
To construct a real-valued and normalized wavefunction out of these eigenstates,
I have,
psi(x) = [exp(ikx) + exp(-ikx)]/ sqrt(2)

But my trouble is, how do I find the expectation value of momentum operator <p> using this psi(x)?
On applying momentum operator, my integral is divergent.
I think that since there are equal probabilities in psi, <p> will be 0.
But how do I show it by calculations?
Please help!
The problem says nothing about using the momentum eigenstates - which cannot be normalized in any case.
 
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  • #5

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  • #6
You are asked to calculate the integral in post #2:

anuttarasammyak said:
[tex]<p>=\int \psi^*(x) \frac{\hbar}{i}\frac{d}{dx} \psi(x) dx[/tex]
is usual way of momentum calculation. Say ##\psi(x)## is real function ?

This has nothing to do with momentum eigenfunctions.
 
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  • #7
@tanaygupta If you are keen on momentum eigenfunction, you may expand the state by momentum eigenfunciton, say ##\phi(p)## instead of expansion of the state by coordinate eigenfunction ##\psi(x)##.

Momentum expectation value is
[tex]<p>=\int \phi^*(p) p \phi(p) dp[/tex]
The relation of ##\phi(p)## and ##\psi(x)## is
[tex]\phi(p)=\frac{1}{\sqrt{2\pi\hbar}}\int e^{-ipx/\hbar}\psi(x) dx[/tex]
[tex]\psi(x)=\frac{1}{\sqrt{2\pi\hbar}}\int e^{ipx/\hbar}\phi(p) dp[/tex]

You see the last equation tells ##\phi(p)## is a kind of amplitude for momentum eigenfunction component, i.e. ## e^{ipx/\hbar}##, of the state.

As ##\psi(x)## is real you observe
[tex]\phi^*(p)=\phi(-p)[/tex]
[tex]<p>=\int \phi(-p) p \phi(p) dp[/tex]

How do you estimate this integral ?
 
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  • #8
anuttarasammyak said:
[tex]<p>=\int \psi^*(x) \frac{\hbar}{i}\frac{d}{dx} \psi(x) dx[/tex]
is usual way of momentum calculation. Say ##\psi(x)## is real function ?
I think it will be easier to go with this one.
 
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  • #9
tanaygupta2000 said:
I think it will be easier to go with this one.
What should I assume psi(x) to be?
 
  • #10
I just looked another question which was like this so I did like that.
 

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  • #11
tanaygupta2000 said:
What should I assume psi(x) to be?
Any real-valued function!
 
  • #12
PeroK said:
Any real-valued function!
Can I simply take sqrt(2/L) sin(n pi x/L)?
What should I get the value for <p>?
 
  • #13
By "any" we mean "arbitrary". You have to calculate the integral for any function. You can of course try a specific function to see what you get. But, the general solution is fairly easy.
 
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  • #14
PeroK said:
By "any" we mean "arbitrary". You have to calculate the integral for any function. You can of course try a specific function to see what you get. But, the general solution is fairly easy.
Can I simply take sin(x), cos(x) etc. ?
Please suggest me some easy function for calculating <p>.
 
  • #15
tanaygupta2000 said:
Can I simply take sin(x), cos(x) etc. ?
Please suggest me some easy function for calculating <p>.
Try ##\psi(x) = e^{-x^2}## and don't worry about the normalisation constant.
 
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What is the expectation value of momentum operator?

The expectation value of momentum operator is a measure of the average momentum of a particle in a given quantum state. It represents the most probable value of momentum that a particle will have when measured.

How is the expectation value of momentum operator calculated?

The expectation value of momentum operator is calculated by taking the inner product of the wave function with the momentum operator, and then integrating over all possible values of momentum.

What is the physical significance of the expectation value of momentum operator?

The expectation value of momentum operator is physically significant because it provides information about the average momentum of a particle in a given quantum state. It is also related to the uncertainty in the measurement of momentum.

How does the expectation value of momentum operator relate to Heisenberg's uncertainty principle?

The expectation value of momentum operator is related to Heisenberg's uncertainty principle as it is used to calculate the uncertainty in the measurement of momentum. According to the uncertainty principle, the more precisely the momentum of a particle is known, the less precisely its position can be known.

Can the expectation value of momentum operator be negative?

Yes, the expectation value of momentum operator can be negative. This means that there is a probability for the particle to have a negative momentum when measured, although it is less probable than having a positive momentum.

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