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Grand condensate variance remains macroscopic

Physical scope

The grand-ensemble ground-mode variance and tail at a fixed positive excess density above the ideal critical density, as a direct instance of the linked theorem. It makes no canonical or interacting-gas claim.

Example

In the three-dimensional ideal Bose grand ensemble at fixed density ρ>ρc, put ρ0=ρ−ρc>0. The ground-mode mean is asymptotic to ρ0V, but Var⁡L(N0/V)→ρ02, and for every x>0 in m−3 its density tail satisfies PL(N0/V≥x)→e−x/ρ0. Thus the condensate density does not concentrate at its mean limit in this grand ensemble.

Verification

Given: ACω (The Axiom of Countable Choice (ACω)), V=L3 in m3, ρ0>0 in m−3, x>0 in m−3, and the grand geometric ground-mode law in Dimension-restricted fixed-mean-density Bose condensation.

[F1] Dimension-restricted fixed-mean-density Bose condensation, Statement: ELN0/V→ρ0, Var⁡L(N0/V)→ρ02, and PL(N0/V≥x)→e−x/ρ0.

1.1givenF1algebra

The linked theorem gives ELN0=ρ0V+o(V). Substitution into the geometric variance nˉ0,L(1+nˉ0,L) and division by V2 gives limit ρ02.

2.1givenF1algebra∎

At x=2ρ0, PL(N0/V≥2ρ0)→e−2>0. Every such event differs from the limiting mean density ρ0 by at least ρ0, so convergence in probability to ρ0 is impossible. This conclusion is specific to the grand preparation; a fixed-number state has N0 constrained by total number.

Depends on

Dependency tree · 2 levels

Sources