On one hand, describing bosons as "fields" is a little misleading, because fermions are also described as fields in QFT. The reason light is classically thought of as a "field" instead of a particle has as much to do with the fact that the photon is massless (hence long-range, hence classically detectable as a field) as the fact that it is a boson. So the distinction isn't too clear.
On the other hand, describing bosons as "energy" is also misleading, because obviously fermions carry energy just as well as bosons.
Thoughts? CYD
I changed "fields" to "non-matter".
Unfortunately, the only mathematics presented to support this was a calculation of the amount of overlap in probability densities between distant electrons.
That's as much as I know - I couldn't write an authoritative summary on the matter. If true, it would impact on not only this article, but also identical particles and fermions, and perhaps others.
-- Tim Starling 11 Oct. 2002
I believe he's saying that, under certain circumstances, you can make an approximation of ignoring antisymmetrization. -- CYD
"The question arises whether we really have to worry about this when we consider a hydrogen atom on earth and another one on the moon. If they are both in the ground state, do they necessarily have to have opposite spin states? What then happens when we consider a third hydrogen atom in its ground state?"
I'll try to find some more authoritative information on this. -- Tim
Okay, CYD is right. Sorry everyone. -- Tim
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