2013
DOI: 10.1103/physrevb.88.134206
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Breakdown of self-averaging in the Bose glass

Abstract: We study the square-lattice Bose-Hubbard model with bounded random on-site energies at zero temperature. Starting from a dual representation obtained from a strong-coupling expansion around the atomic limit, we employ a real-space block decimation scheme. This approach is non-perturbative in the disorder and enables us to study the renormalization-group flow of the induced random-mass distribution. In both insulating phases, the Mott insulator and the Bose glass, the average mass diverges, signaling short rang… Show more

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Cited by 11 publications
(10 citation statements)
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References 39 publications
(75 reference statements)
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“…Then the inhomogeneous nature of the SF and BG phases is addressed through the study of the probability distribution of the SF response which shows strikingly different proper ties when increasing lattice sizes. Shrinking in the SF phase, it clearly broadens in the BG regime, thus indicating the absence of self-averaging [52], We also demonstrate that all sites remain compressible, ruling out a percolation picture. Our conclusions are supported by careful groundstate (GS) simulations through the so-called /^-doubling scheme, disorder averaging over a very large number of realizations, detailed error bar evaluation, and systematic finite-size scaling analysis.…”
mentioning
confidence: 57%
“…Then the inhomogeneous nature of the SF and BG phases is addressed through the study of the probability distribution of the SF response which shows strikingly different proper ties when increasing lattice sizes. Shrinking in the SF phase, it clearly broadens in the BG regime, thus indicating the absence of self-averaging [52], We also demonstrate that all sites remain compressible, ruling out a percolation picture. Our conclusions are supported by careful groundstate (GS) simulations through the so-called /^-doubling scheme, disorder averaging over a very large number of realizations, detailed error bar evaluation, and systematic finite-size scaling analysis.…”
mentioning
confidence: 57%
“…It has been argued by various authors [1,13,20,21] that the BG is a Griffiths phase [34], with the behavior dominated by the existence of rare SF regions. As pointed out recently [35,36], the existence of rare SF regions is intimately related to a breakdown of self-averaging. Although the lack of ergodicity and selfaveraging are common features of conventional spin glasses [37,38] and despite the fact that the BG is dubbed a 'glass', an Edwards-Anderson-like glassy order parameter has not yet been shown to exist in this phase.…”
mentioning
confidence: 89%
“…Despite intense analytical [56][57][58][59][60][61][62][63][64][65][66][67][68][69][70][71][72] and numerical [73][74][75][76][77][78][79][80][81][82][83][84] study, many questions as to the nature of the BG remain. Various theoretical proposals have been put forward suggesting ways to observe the BG in experiments [70,[83][84][85][86][87][88][89].…”
Section: The Disordered Bose-hubbard Modelmentioning
confidence: 99%