How Do You Calculate the X-Component Probability Distribution in Momentum Space?

In summary, the conversation discusses finding the momentum space wave function for the hydrogen atom and determining the probability distribution for the x-component of momentum. This requires using the Fourier transform and inserting a complete set in order to calculate the probability distribution.
  • #1
BLaH!
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0
Hey,
We are given the 1s spatial wave function for the hydrogen atom:

[tex]\psi(\vec{r}) = \frac{1}{\sqrt{a_{0}^3r}}e^{-r/a_{0}[/tex]

We are asked to find the momentum space wave function [tex]\phi(\vec{p})[/tex]. Obviously this is just the Fourier transform of the spatial wave function. In calculating [tex]\phi(\vec{p})[/tex] I used the following theorem:

[tex]For f(\vec{r}) = f(r), \rightarrow F(\vec{q}) = \frac{4\pi}{q}\int_{0}^{\infty} sin(qr) f(r) r dr[/tex]

Here [tex]F(\vec{q})[/tex] is simply the Fourier transform of [tex]f(\vec{r})[/tex]Anyway, this will give you the momentum space wave function in terms of the magnitude of momentum [tex]p[/tex]. After we find this, how do we find what the probability distribution is for the x-component of momentum [tex]p_{x}[/tex].

What should I do? Insert a complete set? Do another transformation? Any help would be appreciated.
 
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  • #2
Thanks!Yes, you should insert a complete set in order to find the probability distribution of the x-component of the momentum. Specifically, you need to calculate the following: \phi(p_x) = \int \phi(\vec{p}) e^{i p_x x} dp_x where \phi(\vec{p}) is the momentum space wave function you obtained from the Fourier transform. The result of this integration will be the probability distribution of the x-component of momentum.
 
  • #3


Hi there,

To find the momentum space wave function \phi(\vec{p}), we can use the Fourier transform as you mentioned. However, we need to take into account the three-dimensional nature of the problem. This means that we need to use the three-dimensional Fourier transform, which is given by:

\phi(\vec{p}) = \frac{1}{(2\pi)^{3/2}} \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} \psi(\vec{r}) e^{-i\vec{p}\cdot\vec{r}} dxdydz

This will give us the momentum space wave function in terms of the three components of momentum (p_x, p_y, p_z). To find the probability distribution for the x-component of momentum p_x, we can use the Born rule, which states that the probability of finding a particle in a particular state is proportional to the square of the magnitude of the wave function in that state.

In this case, we can find the probability distribution for p_x by taking the square of the magnitude of the momentum space wave function with p_y and p_z integrated out:

P(p_x) = \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} |\phi(\vec{p})|^2 dp_y dp_z

This will give us the probability distribution for the x-component of momentum p_x. Keep in mind that this is only for the 1s state, and for other states, the probability distribution may be different. I hope this helps! Let me know if you have any other questions.
 
  • #4


Hi there,

Yes, you are correct in using the Fourier transform to find the momentum space wave function. However, in order to find the probability distribution for the x-component of momentum, we need to use the momentum operator \hat{p_{x}}. This operator acts on the momentum space wave function \phi(\vec{p}) to give us the probability distribution for the x-component of momentum.

To do this, we can use the following formula:

\langle p_{x} \rangle = \int \phi(\vec{p})^* \hat{p_{x}} \phi(\vec{p}) d\vec{p}

Where the integral is over all possible values of momentum p. This will give us the expectation value for the x-component of momentum, which is related to the probability distribution.

Alternatively, we can also use the position operator \hat{x} to find the probability distribution for the x-component of momentum. This can be done using the following formula:

P(p_{x}) = \int |\phi(\vec{p})|^2 |\psi(\vec{x})|^2 d\vec{x}

Where \psi(\vec{x}) is the position space wave function, given by the inverse Fourier transform of \phi(\vec{p}). This method gives us the probability distribution directly, without having to calculate the expectation value first.

I hope this helps clarify the process for finding the probability distribution for the x-component of momentum using the momentum space wave function. Let me know if you have any further questions.
 

Related to How Do You Calculate the X-Component Probability Distribution in Momentum Space?

What is momentum space wave function?

Momentum space wave function is a mathematical representation of a quantum state in terms of momentum rather than position. It describes the probability of a particle having a specific momentum value.

How is momentum space wave function related to position space wave function?

The momentum space wave function is the Fourier transform of the position space wave function. This means that the momentum space wave function can be obtained from the position space wave function and vice versa through a mathematical transformation.

What is the physical significance of momentum space wave function?

The momentum space wave function provides information about the momentum of a particle, which is a fundamental quantity in quantum mechanics. It can be used to calculate the average momentum and uncertainty in momentum of a particle.

Can the momentum space wave function be measured experimentally?

No, the momentum space wave function cannot be directly measured in experiments. It is a mathematical representation used to describe the quantum state of a particle. However, the momentum of a particle can be measured experimentally, and this information can be used to calculate the momentum space wave function.

How does the normalization of momentum space wave function differ from that of position space wave function?

The normalization of the momentum space wave function is different from that of the position space wave function. While the position space wave function is normalized to 1, the momentum space wave function is normalized to the total momentum of the particle. This is because the probability of a particle having any momentum value in momentum space is equal to 1, rather than the probability of being at any position in position space.

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