We investigate the superfluid (SF) to Bose glass (BG) quantum phase
transition using extensive quantum Monte Carlo simulations of two-dimensional
hard-core bosons in a random box potential. T=0 critical properties are
studied by thorough finite-size scaling of condensate and SF densities, both
vanishing at the same critical disorder Wc=4.80(5). Our results give the
following estimates for the critical exponents: z=1.85(15), ν=1.20(12),
η=−0.40(15). Furthermore, the probability distribution of the SF response
P(lnρsf) displays striking differences across the transition:
while it narrows with increasing system sizes L in the SF phase, it broadens
in the BG regime, indicating an absence of self-averaging, and at the critical
point P(lnρsf+zlnL) is scale invariant. Finally, high-precision
measurements of the local density rule out a percolation picture for the SF-BG
transition.Comment: 4 pages, 5 figures + supplementary materia