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Bulletin of the American Physical Society

Finite-size scaling of the chemical potential of bosonic quantum fluids

C.M. Herdman, Adrian Del Maestro

Published Mar 20, 2013• 0 citations
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We investigate the critical properties of cold bosonic gases in three dimensions, confined by an external quadratic potential coupled to the particle density, and realistically described by the Bose-Hubbard (BH) model. The trapping potential is often included in experiments with cold atoms and modifies the critical finite-size scaling of the homogeneous system in a nontrivial way. The trap-size scaling (TSS) theory accounts for this effect through the exponent $\ensuremath{\theta}$. We perform extensive simulations of the BH model at the critical temperature, in the presence of harmonic traps. We find that the TSS predictions are universal once we account for the effective way in which the trap locally modifies the chemical potential $\ensuremath{\mu}$ of the system. The trap exponent for the BH model at $\ensuremath{\mu}=0$ is the one corresponding to an effective quartic potential. At positive $\ensuremath{\mu}$, evidence suggests that TSS breaks down sufficiently far from the center of the trap, as the system encounters an effective phase boundary.
A finite-size scaling is applied to the Yang-Lee zeros of the grand canonical partition function for the two-dimensional Hubbard model in the complex chemical potential plane. The logarithmic scaling of the imaginary part of the zeros with the system size indicates a singular dependence of the carrier density on the chemical potential. Our analysis points to a second-order phase transition with critical exponent 1/\ensuremath{\delta}=1/2\ifmmode\pm\else\textpm\fi{}1/3, which leads to a divergence of the electronic susceptibility. We interpret these results as reflecting the singular behavior of the density of states in the quasiparticle spectrum. \textcopyright{} 1996 The American Physical Society.