Central limit conjecture for mean-field interacting boson random point fields

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Let uκ,β,μ u_{\kappa,\beta,\mu} be the distribution of the random point measure 4ξκ44\xi_{\kappa}4 on 4Rd44\mathbb{R}^d4 for 4κ>044\kappa>04, and let 4L44\mathfrak{L}4 denote Lebesgue measure on 4Rd44\mathbb{R}^d4. Write 4G(β)44G(\beta)4 for the operator appearing in the covariance expression. Central limit conjecture. As 4κ→∞44\kappa\to\infty4, the random field

πd/4κd/4(λμ−μλ,c(β))1/2(ξκ−κd/2πd/2μ−μλ,c(β)λL)\frac{\pi^{d/4}}{\kappa^{d/4}}\Big(\frac{\lambda}{\mu-\mu_{\lambda,c}(\beta)}\Big)^{1/2}\Big(\xi_{\kappa}-\frac{\kappa^{d/2}}{\pi^{d/2}}\frac{\mu-\mu_{\lambda,c}(\beta)}{\lambda}\mathfrak{L}\Big)

converges in distribution to the Gaussian random field on 4Rd44\mathbb{R}^d4 with covariance

(1+G(β))(1−G(β))−1.(1+G(\beta))(1-G(\beta))^{-1}.

This is suggested by the small-test-function expansion of the generating functional and expresses Gaussian fluctuations around the macroscopic mean density in the condensed regime; the paper presents it as a conjectural central limit theorem rather than proving it.

References

Primary source

Hiroshi Tamura and Valentin Zagrebnov, “Mean-Field Interacting Boson Random Point Fields in Weak Harmonic Traps”, arXiv:0807.3530 (2008).

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