2012
DOI: 10.1103/physreve.86.056708
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Analysis of the loop length distribution for the negative-weight percolation problem in dimensionsd=2throughd=6

Abstract: We consider the negative weight percolation (NWP) problem on hypercubic lattice graphs with fully periodic boundary conditions in all relevant dimensions from d=2 to the upper critical dimension d=6. The problem exhibits edge weights drawn from disorder distributions that allow for weights of either sign. We are interested in the full ensemble of loops with negative weight, i.e., nontrivial (system spanning) loops as well as topologically trivial ("small") loops. The NWP phenomenon refers to the disorder drive… Show more

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Cited by 5 publications
(7 citation statements)
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References 30 publications
(62 reference statements)
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“…The result for two-dimensional NWP with mixed Gaussian disorder is shown in Figure 18 . By the analysis of the distribution of loop sizes [ 66 ], two more critical exponents come into play. Right at the critical point , the distribution exhibits a power law, governed by the exponent .…”
Section: Results For Nwpmentioning
confidence: 99%
See 1 more Smart Citation
“…The result for two-dimensional NWP with mixed Gaussian disorder is shown in Figure 18 . By the analysis of the distribution of loop sizes [ 66 ], two more critical exponents come into play. Right at the critical point , the distribution exhibits a power law, governed by the exponent .…”
Section: Results For Nwpmentioning
confidence: 99%
“…Now, we will actually introduce the model for negative-weight percolation (NWP) [ 62 , 63 , 64 , 65 , 66 , 67 , 68 ]. This model exhibits some differences in comparison with other percolation models involving string-like objects.…”
Section: Negative-weight Percolationmentioning
confidence: 99%
“…This leads, interestingly, to a new type of behavior giving rise to a different universality class compared to standard percolation. In a series of papers [7][8][9][10][11][12][13], NWP has been studied in different dimensions and different variants.…”
Section: Introductionmentioning
confidence: 99%
“…[6] the disorder-driven phase transition was investigated by means of finite-size scaling analyses and it turned out that the critical exponents were universal in 2D (different lattice geometries and disorder distribution were studied). Further studies regarding isotropic NWP address the influence of dilution on the critical properties [7], the upper critical dimension (d u = 6) [8], another upper critical dimension (d DPL u = 3) for densely packed loops far above the critical point [9], the meanfield behavior on a random graph with fixed connectivity [10], the Schramm-Loewner evolution properties of paths in 2D lattices [12], and loop-length distributions in several dimensions [11].…”
Section: Introductionmentioning
confidence: 99%
“…If the disorder is drawn from a distribution that allows for nonegative edge energy only, as for the canonical "directed polymer in a random medium" (DPRM), the groundstate configuration of the polymer can be computed efficiently using Dijkstra's algorithm [10,11]. However, if the disorder distribution allows for edge-energies of either sign, as for the problem of finding a minimum energy domain wall in 2D Ising spin glasses [7,8,12] (given that there is no * Electronic address: oliver.melchert@uni-oldenburg.de † Electronic address: alexander.hartmann@uni-oldenburg.de closed path with a negative energy) or more generally for the negative-weight percolation (NWP) problem [13][14][15][16][17][18], the solution of the MWP problem requires a nontrivial transformation to an auxiliary minimum-weight perfect matching problem [19]. Furthermore, the properties of MWPs with negative edges are fundamentally different from the case where all edge energies are non-negative [7,8,12].…”
Section: Introductionmentioning
confidence: 99%