uranium138 said:
When ,say heilium, goes in a super fluid state can a batch of it occupy the same amount of space as one atom of heilium? if it can't, why not because the exculsion principle is no longer obeyed so can't it all merge together to only occupy a point in space.
Here's the problem with your question.
Fermi-Dirac and Bose-Einstein statistics kick in when the particles' wavefunction make a significant overlap. When this happens, something call
indistinguishibility of the particles becomes important. Now this doesn't mean the particles all look the same. We have the same thing in classical statistics. What this means in this case is that you cannot, even in principle, distinguish one particle with the next. You cannot tag a particle and follow it along anymore.
So the question on whether they all "occupy a point in space" is meaningless because you can't look at one particle, point to where it is, and look at another and point to where it is.
The BE statistics indicates that the overall wavefunction must be even. Note that this overall wavefunction includes the product of the spin part and the spatial part. What this means is that they can all occupy the SAME state, and be described by the SAME wavefunction.
There is an added complication here that I am hesitating to get into, so I'll mention it only in passing. While each of the fermions form a composite wavefunction, the fermions themselves STILL MAINTAIN their F-D statistics. In other words, if one electron has a k1up and the other pair has a -k1down configuration, the OTHER pair of electrons can only have k2up,-k2down, etc... I.e. each of the fermions in the whole condensate STILL can only occupy a unique state to maintain the fermionic statistics. so while the composite boson can all condense to the same state, the consituent fermions cannot. This already prevents things from "occuping the same point" in space, which in itself is difficult already due to local coulomb repulsion.
Zz.