Is the Moon a Boson? Astronomy & Quantum Spin Explained

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    Boson Moon
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Discussion Overview

The discussion revolves around the question of whether the Moon can be characterized as a boson based on the sum of the quantum spins of its constituent particles. Participants explore the implications of quantum spin in the context of large, complex objects like the Moon, considering both theoretical and conceptual aspects.

Discussion Character

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

Main Points Raised

  • One participant questions the total quantum spin of all particles making up the Moon and suggests that if the sum were a whole number, it might imply a bosonic nature.
  • Another participant challenges the relevance of the Moon as an example, suggesting that defining the particle set for any object is complex due to the uncertainty principle.
  • A later reply rephrases the question to inquire about the probabilities of the total spin being an integer, an integer plus one-half, or a real number.
  • Some participants argue that the Moon, like any object with many interacting degrees of freedom, is not in a spin eigenstate, which complicates its classification as a boson or fermion.
  • There is a discussion about specific quantum states and their classifications, with examples provided to illustrate the distinction between fermions and bosons based on their spin states.
  • One participant notes that the Moon is constantly exchanging particles with its environment, which may affect its status as being in a particle number eigenstate.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of boson or fermion classification to the Moon, with some asserting that it cannot be classified due to its complex nature, while others explore the implications of quantum states without reaching a consensus.

Contextual Notes

The discussion highlights limitations in defining the particle set for large objects and the impact of the uncertainty principle on characterizing quantum states.

Mentz114
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This could be an astronomically stupid question but I cannot think of a sensible answer. What is the sum of all the quantum spins of all the particles that make up the moon ? If it was a whole number I suppose the answer would be 'yes'.
 
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The moon? Why the moon?
 
Why the moon? Probably just to attempt to characterize the presented example object as an "isolated" object; but it's not really. No more easy or clear to define the set of particles that make up the moon at any instant than it is to consider the same for an apple or a chair.

One might try to get to the sense of the question by stipulating an object free of influences (shielded from radiation and placed free of gravitational influence in deep space... etc.), or stipulate the particle count for an otherwise compromised object at an instant in time, but I don't think those work either because of uncertainty principle, at least.
 
Let me rephrase the question. If we counted up all the spins in one instant, what is probability that it will be 1) and integer 2) an integer + 1/2 3) a real number ?
 
Mentz114 said:
Let me rephrase the question. If we counted up all the spins in one instant, what is probability that it will be 1) and integer 2) an integer + 1/2 3) a real number ?

Neither. The moon, or any other object with sufficiently many interacting degrees of freedom, is not in a spin eigenstate. Therefore the characterisation as boson or fermion doesn't apply.
 
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Great.
Is it the same for a small saucepan?
 
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Jazzdude said:
Neither. The moon, or any other object with sufficiently many interacting degrees of freedom, is not in a spin eigenstate. Therefore the characterisation as boson or fermion doesn't apply.
Thank you.
 
If you have something like
##\frac{1}{\sqrt{2}} \left(\left|\mathrm{spin 1/2}\right> + \left|\mathrm{spin 3/2}\right>\right)##
that's still a fermion, right?
And
##\frac{1}{\sqrt{2}} \left(\left|\mathrm{spin 2}\right> + \left|\mathrm{spin 3}\right>\right)##
is still a boson, right?
As long as you are in an eigenstate of particle number, the total spin still has to come out either a superposition of integers or a superposition of integer+1/2.
Of course, the moon is constantly exchanging particles with the surroundings, so maybe it's not in a particle number eigenstate.
 
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