Are spin-up and spin-down electrons distinguishable or indistinguishable?

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Discussion Overview

The discussion revolves around the distinguishability of spin-up and spin-down electrons within the context of quantum mechanics and statistical mechanics. Participants explore the implications of measurements, conservation laws, and the nature of identical particles, addressing both theoretical and practical aspects of the topic.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants propose that electrons are indistinguishable if they have the same spin or if a measurement is made that places their spin in a superposition, while they can be considered distinguishable under certain conditions, such as when specific spin measurements are not performed.
  • Others argue that the total spin of a system is conserved, meaning that while the number of spin-up and spin-down electrons remains constant, individual electrons cannot be distinguished due to their ability to swap spins during interactions.
  • A participant suggests that in statistical mechanics, indistinguishability applies to particles of the same spin, complicating the distribution of spins among electrons in a system.
  • Another viewpoint emphasizes that two quantum systems are considered identical if their intrinsic attributes are the same, referencing Wigner's criteria for elementary particles.
  • A later reply introduces a question about the spin of protons in helium nuclei, exploring whether Pauli's exclusion principle applies to them and how quark swapping affects their distinguishability.

Areas of Agreement / Disagreement

Participants express differing views on the conditions under which electrons can be considered distinguishable or indistinguishable, indicating that the discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Limitations include the dependence on specific measurement conditions, the interpretation of indistinguishability in different contexts (quantum vs. statistical mechanics), and the implications of conservation laws on particle identity.

wdlang
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i am puzzled by this problem
 
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They are indistinguishable if they have the same spin or a measurement is done such that their spin is a superposition (like an Sx measurement). In theory though they are distinguishable between each other (i.e. a spin, Sz=+1/2 is distinguishable from an Sz=-1/2) provided, as I said, something like an Sx measurement is not done.
 
Depends on the context, doesn't it? The total spin of a system is conserved (non-relativistically), so if you have 5 up and 3 down, you'll always have 5 up and 3 down.

But for any interacting electrons they can swap spins, so you can never tell which one is or was which.
So they're 'distinguishable' from the thermodynamic sense since the total number of each spin is conserved,
and you have Fermi-Dirac statistics and all that. But they're not distinguishable in the sense that you can tell one from the other.
 
Well I feel like you're muddling picture here. In statistical mechanics we have an indistinguishability amongst those of the same spin. Thus, it's essentially, how can you distribute 5 ups amongst 8 spins. However, if we treat this instead with pure quantum with the Schrödinger (or Dirac) solution of 8 distinct electrons it's different. Our solutions must be the same under permutation of ups and downs but it's a different situation where we have initial values conditions and such. Of course I could just be talking out of my arse here.
 
The trick with distinguishable or not is simple: two quantum systems are identical, if their intrinsical attributes are the same. For elementary particles a\ la Wigner, two elementary particles are identical/indistinguishable, iff they have the same mass and eigenvalue of the squared Pauli-Lubanski pseudovector.
 
Do the protons in a helium nuclei have spin 0 in the ground state? Or does Pauli's exclusion principle only apply to elementary particles, thus allowing the protons to have spin 1?

Is the correct interpretation to say that the protons are made from 3 quarks, so swapping the two protons swaps 3 quarks (u of one with the u of the other, d of one with d of the other) which produces a negative sign since 3 is an odd number of swaps?
 

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