Double slit probability question

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Discussion Overview

The discussion centers on the double slit experiment, particularly the implications of detecting particles (electrons) at one of the slits and how this affects the probability of detection at the other slit. Participants explore concepts related to measurement, wavefunction collapse, and the nature of particles in quantum mechanics.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether detecting an electron at one slit means it will always be detected there or if it could be detected at the other slit 50% of the time.
  • Others argue that if electrons are fired symmetrically, the detection probabilities should reflect that symmetry.
  • One participant suggests that not measuring at one slit constitutes a measurement, as it implies knowledge about the electron's path.
  • Another participant posits that the electron's behavior is independent of the measurement, suggesting a sequence of events where the electron acts freely until detected.
  • Some participants assert that the presence of a detector at one slit will collapse the wavefunction, affecting the interference pattern observed.
  • A hypothetical scenario is presented where two screens are used, leading to questions about the probabilities of detection and the nature of wavefunction collapse.
  • There are discussions about whether the number of screens influences the path taken by the particle and how this relates to interference patterns.
  • Several participants express uncertainty about the implications of their setups and the nature of measurements in quantum mechanics.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of measurement in the double slit experiment. Multiple competing views remain regarding the nature of particles, the role of measurement, and the interpretation of results.

Contextual Notes

Limitations include assumptions about the experimental setup, the definitions of measurement, and the conditions under which particles are detected. The discussion does not resolve the mathematical or conceptual complexities involved.

entropy1
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Consider the double slit experiment; if we position a detector at, say, the left slit, will a single particle, say, an electron, when fired at the slits, always be detected at the left slit, or will it be detected at the left slit 50% of the time? (so that it is 50% of the time at the right slit)
 
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If the electrons are fired at the two sits in a symmetrical manner, 50%
Is that really what you wanted to ask ?
 
BvU said:
If the electrons are fired at the two sits in a symmetrical manner, 50%
Is that really what you wanted to ask ?
Yes, I think so. I seems to me that, then, not measuring at the left slit is a measurement also, for we now know that the electron has to be on the right slit. It that correct?
 
If you know it's passed a slit and hasn't passed the left slit, then yes. Am I painting myself in a corner now ?

(PS there are more ways than one to interpret 'not measuring' !)
 
:smile: The electron doesn't know. There's a sequence in time here: the electron does whatever it pleases and the detector detects -- or not.

But now I sense we aren't communicating -- I wrongly assumed your detector sits after the slit (*). You have something else in mind

(*) Feynman influence: to see through which slit the electron passes
 
This is a simple classical question containing no special quantum behavior.

Most will not pass through either slit. The slits merely select two trajectories. The detector at the slit merely marks the electron state as having passed through that slit. The result will be the same as throwing golf balls randomly at a fence with two missing planks. A screen on the other side which notices all electrons that have passed through both slits will see 50% from the left slit. But the detector at the left slit or any other apparatus on the other side that ignores all electrons from the right slit, will record 100% of the electrons it notices as having have passed through that left slit.
 
entropy1 said:
I seems to me that, then, not measuring at the left slit is a measurement also

It depends on what you mean by "not measuring". If there is no detector at either slit, then you don't know which slit the electron went through. If there is a detector at the right slit but not the left slit, then you do know which slit the electron went through. Note that both of these statements assume that there is a detector well after the slits, where all electrons are detected (and where we can see if their points of impact build up an interference pattern or not). (And it also assumes that we do not consider any runs of the experiment where no electron is detected at all, because it hit something else and never reached any detectors that are present--as mikeyork pointed out, in a real version of this experiment, many electrons will end up this way.)
 
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The following occurred to me:

If we have slit A with a screen A, and slit B with screen B, both A en B setting isolated from each other. Now, screen B is twice as far behind its slit as screen A from its.

We now fire an electron that passes boh slits. Then after a while, the the electron could hit screen A. The probability is 50% that it actually does.

If the electron does not impact screen A, the probability it will impact screen B is 100%!

So, if the electron does not impact screen A, it always impacts screen B.

On the other hand, if screen B is passed, then screen A must have been hit.

So, what does select which screen, A or B, will be hit? If it is collapse, why does screen A collapse the wavefunction 50% of the time, and when it doesn't, why does it collapse at screen B 100% of the time left? Or do both screens collapse 50% of the time and is there retrocausality from B to A? Or is there no collapse? Is there a non-local effect? Et cetera. Or is it just the way it is (do the math and so forth :wink: )

It does resemble entanglement to me. Is that correct?

Sorry if I misunderstand completely.
 
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The which path info will cause a collapse regardless if you measure only 1 slit. Any attempt to get the which path info will lead to the same thing even if no direct measurment was made (ex: delayed choice experiement)
 
  • #10
Have a look at this paper, especially fig. 2, looking experimentally at multi-slit interferometry with C70 molecules.

What you see in fig. 2 is what happens as the proportion of molecules that gets excited increases: the contrast of the fringes diminishes, until it vanishes completely. This is because an excited molecule has a significant probability of emitting a photon, which would result in which-way information (even if the photon is not actually detected). Only the molecules that do not emit contribute to the fringe pattern. The others simply add to the constant background.
 
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  • #11
Ostrados said:
The which path info will cause a collapse regardless if you measure only 1 slit. Any attempt to get the which path info will lead to the same thing even if no direct measurment was made (ex: delayed choice experiement)
In my example setup there are no extra detectors. The screens are the detectors. I am wondering why:
  • Screen A absorbs only 50% of the particles, while screen B always absorbs (all of the leftover) particles.
A view on this is that screen B equally absorbs only 50% of its particles, and screen A is the one absorbing the leftover 100%. A symmetrical situation, but mutually exclusive. So this resembles to me the collapsing of two entangles particles, where neither is determining the other's measured value.

The local interaction between particle and screen doesn't seem to explain what is happening (of course). :smile:
 
  • #12
Can you post a drawing of what you mean ? Again, it sounds like you have a totally different setup as thte one I read from your description. A screen as a detector ? why not call it a screen, then ?
 
  • #13
BvU said:
A screen as a detector ? why not call it a screen, then ?
I do call it a screen. It was ment to explain to Ostrados, who talked about detectors. (He talked about measurements, I assumed wrongly detectors I see now).

BvU said:
Can you post a drawing of what you mean ?

pf-illustration-1-png.113916.png


You can imagine the left side as a screen and the right side too.
 

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  • #15
entropy1 said:
We now fire an electron that passes both slits
And how do you know that ?
 
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  • #16
BvU said:
And how do you know that ?
I think I reason this way: the setup between the slits and the two (in this case) separated screens is identical to a setup that could have only one screen. With only one screen there would be an interference pattern, which means that the particle would have passed both slits. (one should do violence to the picture I posted, but I hope you know what I mean :wink: )

And besides that, the particle is only that at the moment it is detected, right?
 
  • #17
No. Only a small fraction of the electrons make it to the single screen.
mikeyork said:
This is a simple classical question containing no special quantum behavior.
Most will not pass through either slit.
To get an interference pattern, the slits need to be very narrow and very close together (of the order of the De Broglie wavelength)
 
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  • #18
BvU said:
No. Only a small fraction of the electrons make it to the single screen.
Am I right about this then?
entropy1 said:
And besides that, the particle is only that at the moment it is detected, right?
 
  • #19
You mean to say that the particle is not a particle until it is hitting a screen ? What would the source of the particle have to say about that ?
 
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  • #20
If a particle is a particle from the start, and it travels through only one slit, how can there exist something as an interference pattern?

  • In case of two separated screens, the particle travels through one of the two slits;
  • In case of one screen, the particle travels through both slits (interference)?
Does the number of screens determine how the particle travels?

I guess what I ask is: what determines which path(s) the particle will take?
 
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  • #21
Wouldn't you simply see an interference pattern across screens A and B (a bit out of alignment between the screens, though)?
 
  • #22
StevieTNZ said:
Wouldn't you simply see an interference pattern across screens A and B (a bit out of alignment between the screens, though)?
Yes, that's pretty much it.
 
  • #23
entropy1 said:
If a particle is a particle from the start
Yes.
entropy1 said:
and it travels through only one slit
No.
entropy1 said:
I guess what I ask is: what determines which path(s) the particle will take
Can't ask that. The probability the particle ends up somewhere is the outcome of a calculation that involves both slits. Same as a water wave with comparable geometry. It is a particle but it obeys a wave equation.
 
  • #24
If you split the screens using a physical barrier then the interference pattern will disappear because there will be no interference between the 2 slits.

But if you are talking about splitting the screens without physical barrier (by putting the screen further away like you did) then that will not make any difference in the interference pattern (why would it make a difference?)
 
  • #25
Ostrados said:
If you split the screens using a physical barrier then the interference pattern will disappear because there will be no interference between the 2 slits.

But if you are talking about splitting the screens without physical barrier (by putting the screen further away like you did) then that will not make any difference in the interference pattern (why would it make a difference?)
In my setup the 'screens' are ment to be physically separated. So then there is no interference pattern on either screen, right? In that case my issue #8 applies.
 
  • #26
entropy1 said:
In my setup the 'screens' are ment to be physically separated. So then there is no interference pattern on either screen, right? In that case my issue #8 applies.
It is not clear what your point is in #8. Why screen A is special? the particles will go into A or B randomly at 50:50 chance.

Because you are physically separating the screens then there will always be no interference between the slits, so screen A being closer will not make any difference.
 
  • #27
Ostrados said:
It is not clear what your point is in #8. Why screen A is special? the particles will go into A or B randomly at 50:50 chance.
My point is more or less: if the electron hits screen A, then it won't hit screen B, and vice-versa. So they are mutually exclusive events, and I was wondering how the electron makes the choice for screen A or screen B,or what is making it for it. :wink:
 
  • #28
P(A) = P(~B) = 1 - P(B)

Nothing makes it chose it is just probability. your question is like saying why a coin chooses header or tale.
 
  • #29
Ostrados said:
P(A) = P(~B) = 1 - P(B)

Nothing makes it chose it is just probability. your question is like saying why a coin chooses header or tale.
The point I was trying to make at #8, is that screen A is first-in-line because it is closer, so the 'particle' (wavefunction) has to 'decide' to impact there or travel some further to screen B. In effect, both screens are hit 50% of the time. So, what makes screen A decide to let 50% of the electrons go? Then screen B obviously decides to keep 100% of the ones let through by screen A, while it is an exactly identical screen. (I realize screen A and B are physically separated - I hope you understand what I mean)
 
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  • #30
entropy1 said:
The point I was trying to make at #8, is that screen A is first-in-line because it is closer, so the 'particle' (wavefunction) has to 'decide' to impact there or travel some further to screen B. In effect, both screens are hit 50% of the time. So, what makes screen A decide to let 50% of the electrons go? Then screen B obviously decides to keep 100% of the ones let through by screen A, while it is an exactly identical screen. (I realize screen A and B are physically separated - I hope you understand what I mean)
Nothing is "deciding."

Imagine that, in your setup, the electrons are fired at precise time intervals, with a determined speed, and that you know immediately when an electron hits the screen. After each firing, you will either detect the electron at screen A after a certain amount of time, or a little bit later at screen B. Nothing weird there. After having done this a million times, you look at where on the two screens the electrons hit, and you will find an interference pattern, which looks as if each electron went through both slits an interfered with itself. The results are consistent with the QM prediction, where the wave function evolves through all of space, and thus there can be interference because of the two slits, but detection always takes place randomly at one particular point on one of the screens. Generally speaking, QM has nothing to say about which path the electron actually took in each case.
 

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