Quantum uncertainty after passing through a slit

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Homework Help Overview

The problem involves a particle, specifically a proton, transitioning from a confined potential to free fall under gravity after passing through a slit. The initial conditions include a specific speed and the width of the slit, raising questions about the spatial uncertainty associated with the particle's position in the y direction over time.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between spatial uncertainty in the y direction and momentum uncertainty, referencing the uncertainty principle. There is an exploration of how to propagate uncertainty and the implications of initial conditions on future positions.

Discussion Status

Participants are actively engaging with the problem, questioning assumptions about initial velocities and discussing methods for calculating uncertainty over time. Some have proposed expressions for uncertainty and are seeking clarification on their reasoning and calculations.

Contextual Notes

There is a focus on the propagation of uncertainty and how it relates to the movement of the particle along the z axis, while the y axis remains a point of confusion. Participants are also considering the implications of the particle's initial conditions on its future behavior.

md.xavier
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Homework Statement



A given particle is confined to a certain potential. At a given instant that potential is turned off and the particle is accelerated by gravity. In the initial instant t = 0, when the potential is turned off, it has an initial speed of vz = 1 m/s.

In the instant t = 0 the particle goes through a slit with width y = 1 mm = 10^-3 m in the y axis. How much time does it take for the spatial uncertainty associated with y to double? Consider the law of propagation of uncertainty for the calculation of the spatial uncertainty of y at a given instant. Consider the particle a proton.

Homework Equations



[;\sigma_{x}\sigma_{p} \geq \frac{\hbar}{2};]

[;\mathbf{p} = m\mathbf{v};]

[;v = v_0+at \,;]

[;\left |\Delta X\right |=\left |\frac{\partial f}{\partial A}\right |\cdot \left |\Delta A\right |+\left |\frac{\partial f}{\partial B}\right |\cdot \left |\Delta B\right |+\left |\frac{\partial f}{\partial C}\right |\cdot \left |\Delta C\right |+\cdots;]

The Attempt at a Solution



I understood that, as the particle passes through the slit, we have [;\Delta y\right;] equal to the slit's width.

But, from that, I don't really get how to proceed, considering the particle is moving along the z axis. I can relate the errors along the z axis, but since there's no momentum along the y axis, I am kind of lost.

How am I supposed to use the propagation of uncertainty?

Thank you in advance. I don't expect to be just given the solution, I just want a little push forward. (I am new here, so please tell me if I'm doing anything wrong!)
 
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I'm not sure I understand this problem entirely but...

To start, ignore the z axis. What does the uncertainty in y position tell you about the uncertainty in y momentum?
 
I'm not sure either, actually!

And well, according to the Uncertainty principle:

[;\sigma_{py} \geq \frac{\hbar}{2\sigma_{y}};]

But since they mention the propagation, and even with this info, I'm really lost.
 
Ok, that's right. (I think you should check that it's really supposed to be an initial v_z and not an initial v_y)

If you have a range of potential initial y positions, and a range of potential y velocities, how would you compute the range of potential y positions in the future?
 
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(Confirmed! It really is an initial v_z.)

So, taking this:

[;\sigma_{py} \geq \frac{\hbar}{2\sigma_{y}};]

[;\sigma_{y_0} = 10^{-3};]

[;\sigma_{py_0} \geq 5.275 \times 10^{-32} ;]

Which means... (dividing by the proton mass)

[;\sigma_{vy_0} \geq 3.153 \times 10^{-5};]

Do I propagate to [;\sigma_{y};], using the info I have from [;\sigma_{vy_0};] and [;\sigma_{y_0};]? (using a normal position equation, like [; x = x_0 + v_0 \times t + 0.5 \times a \times t^2 ;])
 
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Yeah that's the idea. Basically, what I'm thinking is: what's the furthest in one direction it could be? what's the furthest in the other direction? Presumably the particle is somewhere in between these two points.

Also I figured out why the v_z matters: if there was no v_z, then the particle would still be in the slit, and the y position uncertainty would never change.
 
That's the uncertainty, no? For example, in the y direction, at t = 0, the particle could be anywhere within the slit, from one border to the other.

The thing is, now that I propagated (using the partial derivatives of y in respect to y_0 and vy_0), I have a few questions: are the initial position / velocity null? I now have an expression for [;\sigma_{y};] with respect to t, y_0, vy_0, and a. Considering none of those apart from t really apply to the y-axis in this problem, I'm kind of confused. I got an expression similar to:

[;\sigma_{y}^{2}(t) = (1 + v_y_0 \times t + 0.5 \times a \times t^2)^{2} \times (\sigma_{y_0})^{2} + (y_0 + t + 0.5 \times a \times t^{2})^{2} \times (\sigma_{v_y_0})^{2} ;]

Am I making a complete mess of things or am I going the right way? I'm definitely understanding the problem better, but the way to get there I'm quite not grasping yet.
 

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