Why isn't Pauli Exclusion Principle a force?

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Discussion Overview

The discussion centers around the nature of the Pauli exclusion principle and why it is not classified as a force. Participants explore the implications of the principle in quantum mechanics, its relationship to other physical phenomena, and the foundational axioms of physics that might underlie it.

Discussion Character

  • Conceptual clarification
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants question whether the Pauli exclusion principle is misunderstood in its classification as a force, suggesting a need for clarification on the definitions of "force" and "principle."
  • Others argue that the Pauli exclusion principle leads to degeneracy pressure, which behaves like a force, but this arises from the quantization of states rather than an external field acting on particles.
  • A participant explains that the Pauli exclusion principle is inherently present in the free theory without requiring specific interactions, emphasizing its algebraic nature through the anti-commutation relations of fermionic operators.
  • Another participant expresses dissatisfaction with the idea that physical phenomena can be explained solely by algebra, suggesting that the algebra should describe phenomena rather than be seen as the cause, and inquires about the fundamental physical axioms that might underpin the principle.
  • One participant notes that the Pauli exclusion principle is linked to the spin-statistics theorem, which is fundamental to the quantization of fermions, but admits a lack of expertise in the formal aspects of axiomatic quantum field theory.

Areas of Agreement / Disagreement

Participants express differing views on the classification of the Pauli exclusion principle, with some seeing it as a fundamental axiom while others focus on its algebraic properties. The discussion remains unresolved regarding whether the principle can be considered a force or if it should be understood through different foundational concepts.

Contextual Notes

Participants highlight the dependence on definitions and the unresolved nature of the relationship between algebraic formulations and physical phenomena. There is also a mention of limitations in expertise regarding formal proofs in quantum field theory.

azabak
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In the same way we could create "principles" for the other forces which would not make them not forces. Is it a misunderstanding of the meaning of a force or principle? Could someone clarify this for me.
 
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The Pauli exclusion principle leads to degeneracy pressure, which acts sort of like a force. That's related to the Casimir effect, which also acts like a force. But these are both derived from the quantization of available states of the system, and not due to some field acting on the particles. I guess you are suggesting that we could "derive" other forces in a similar manner? Eric Verlinde published an article suggesting that gravity was due to entropy, and therefore also some result of quantization of available states. I don't know of any treatment of electroweak/strong in any such manner. But maybe you could try inventing it.
 
The Pauli principle is not a force b/c it is already present in the free theory w/o any specific interaction; it holds purely algebraically w/o specifying a dynamics i.e. w/o specifying a Hamiltonian.

Suppose you have fermionic creation and annihilation operators [itex]b_i^\dagger[/itex] and [itex]b_i[/itex] with the usual anti-commutators. Here 'i' is a general index containing all relevant numbers specifying a state like momentum, spin, isospin etc.

The relevant identity which follows from the anti-commutators is

[tex]\left(b_i^\dagger\right)^2 = 0[/tex]

It says that you cannot create a two-particle state with two fermions having both the same state 'i'.

Of course you can construct arbitrary complex interaction terms

[tex]\sum_{ijk, \ldots pqr \ldots}h_{ijk, \ldots pqr \ldots} b_i^\dagger b_j^\dagger b_k^\dagger \ldots b_p b_q b_r \ldots[/tex]

but in all those interactions every diagonal term with (e.g.) i=j vanishes

[tex]h_{iik, \ldots pqr \ldots} b_i^\dagger b_i^\dagger b_k^\dagger \ldots b_p b_q b_r \ldots = 0[/tex]

So the Pauli principle eliminates all these terms from the theory w/o requiring a specific interaction; the number hiik...pqr... need not be zero; it's the anti-commutator itself that makes this term vanish.
 
tom.stoer said:
it holds purely algebraically w/o specifying a dynamics i.e. w/o specifying a Hamiltonian.

But saying that a physical phenomena is caused by humanly invented algebra is to me not very satisfying explanation. Shouldn't it be more accurate to say that the algebra describes the phenomena, but that the cause is a (a combination of) certain physical axiom(s)?

Could you say anything about which those more fundamental physical axioms would be? Or alternatively, could it be that the Pauli exclusion principle is a fundamental physical axiom in itself? (meaning that the creation and annihilation operators and their commutators was designed to with the need to fulfill the PEP in mind.)
 
The Pauli exclusion principle is due to the anti-commutators or Grassmann fields to be used for quantizing fermions; these anti-commutators or Grassmann fields are due to the spin-statistics theorem

Have a look at Wikipedia and references therein: http://en.wikipedia.org/wiki/Spin-statistics_theorem

I have to admit that I am not an expert in axiomatic quantum field theory and that I am not able to comment on formal aspects of these proofs. But up to my knowledge the spin-statistics-theorem is the most fundamental starting point
 
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