Identical particles distinguished by their trajectory?

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Discussion Overview

The discussion revolves around the concept of indistinguishability of identical particles, specifically electrons, and whether their trajectories can be used to distinguish them in certain scenarios. Participants explore theoretical implications and interpretations of quantum mechanics related to particle exchange and measurement.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant proposes that if two electrons are placed at opposite ends of a long line and their positions and velocities are measured, it may be possible to distinguish them based on their trajectories, assuming they have not moved too far apart in a short time.
  • Another participant challenges this idea, suggesting that the scenario presented does not address the fundamental principle of indistinguishability in quantum mechanics and characterizes it as a strawman argument.
  • A different participant clarifies that indistinguishability is a statistical property of identical particles, expressed mathematically, and emphasizes that exchanging two identical particles does not change the probability of the system's state.
  • Further, a participant explains that in a hypothetical scenario where two indistinguishable particles are labeled and measured, the quantum mechanical description leads to both particles being in a superposition of states, making it impossible to assign a definite label to either particle based on their trajectories.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of classical analogies to the quantum concept of indistinguishability. There is no consensus on whether the original proposal about distinguishing electrons based on trajectory is valid, as some participants argue against it while others seek clarification.

Contextual Notes

Participants reference the Born rule and the mathematical framework of quantum mechanics, indicating that the discussion is grounded in theoretical concepts that may not be fully resolved in the context of the proposed scenario.

Bootleg
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Hello.
It is said that if we exchange two electrons, we can't tell which is which. Identical mass, charge, etc. So if I hold two electrons, one in each hand, and someone switched them, I wouldn't be able to know. But one way to distinguish particles is their trajectory. If I have a very long 1D line with an electron at each end, and I measure their kinetic energies, and a very short while after, I measure their positions again. I can see both of them have moved, but their positions can be related to their velocities times the time interval, i.e d=v*t for each electron... Now I can pretty confidently say that the electron to the right is still to the right, and the electron that was to the left before is still to the left, because let's say their speed was small. Or alternatively, it would break the speed of light if the left electron had moved all the way to the other end of the 1D line in that small time interval and vice versa, and hence I can distinguish the two electrons. Maybe a long time after, the wave functions would overlap due to Schrödinger equation, and then they would be truly indistinguishable.
So is it possible in situations like these to actually distinguish two electrons, or did I mess up?
 
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Sure, but having "a thing over here" and "a thing over there" has nothing to do with the indistinguishably of electrons so you are setting up a strawman.
 
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I think strawman is something people use in a fallacious argument, not a question asking for understanding.

Bootleg, indistinguishabililty comes into play from the statistics of the states, and is expressed in terms of math. It states that if you exchange the two identical particles with each other, the probability of the state doesn't change. By the Born rule, this means the norm of the wavefunction must not change. Since two exchanges is equivalent to no exchanges, this means that the wavefunction must stay the same or be multiplied by -1 during exchange. It's not something that can be explained by a classical analogy.
 
Khashishi said:
I think strawman is something people use in a fallacious argument ...
which is, I think, exactly what he presented although I do see how you interpret it more as just a question.
 
I think I can make it a little clearer. Suppose you have two particles which are indistinguishable, and you hypothetically label them 1 and 2. In an experiment, you have a particle go left and a particle go right. Classically, you would think that either 1 went left and 2 went right, or 1 went right and 2 went left. But the math of indistinguishability says that both situations are equally probable. Before you make a measurement, there is no randomness and therefore the left particle has to be a superposition of 1 and 2, and the right has to also be in a superposition of 1 and 2. You can't say the left particle is 1 and the right particle is 2, because why would 1 be biased to go left and 2 biased to go right, if they are identical? Now since both left and right are both superpositions of 1 and 2, there's no (measurable) change if you swap 1 and 2.
 
Thanks guys this helped.
 

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