Percolation, a paradigmatic geometric system in various branches of physical sciences, is known to possess logarithmic factors in its correlators. Starting from its definition, as the Q → 1 limit of the Q-state Potts model with SQ symmetry, in terms of geometrical clusters, its operator content as N -cluster observables has been classified. We extensively simulate critical bond percolation in two and three dimensions and determine with high precision the N -cluster exponents and non-scalar features up to N = 4 (2D) and N = 3 (3D). The results are in excellent agreement with the predicted exact values in 2D, while such families of critical exponents have not been reported in 3D, to our knowledge. Finally, we demonstrate the validity of predictions about the logarithmic structure between the energy and two-cluster operators in 3D.
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We propose the clock Monte Carlo technique for sampling each successive chain step in constant time. It is built on a recently proposed factorized transition filter and its core features include its O(1) computational complexity and its generality. We elaborate how it leads to the clock factorized Metropolis (clock FMet) method, and discuss its application in other update schemes. By grouping interaction terms into boxes of tunable sizes, we further formulate a variant of the clock FMet algorithm, with the limiting case of a single box reducing to the standard Metropolis method. A theoretical analysis shows that an overall acceleration of O(N κ ) (0 ≤ κ ≤ 1) can be achieved compared to the Metropolis method, where N is the system size and the κ value depends on the nature of the energy extensivity. As a systematic test, we simulate long-range O(n) spin models in a wide parameter regime: for n = 1, 2, 3, with disordered algebraically decaying or oscillatory Ruderman-Kittel-Kasuya-Yoshida-type interactions and with and without external fields, and in spatial dimensions from d = 1, 2, 3 to mean-field. The O(1) computational complexity is demonstrated, and the expected acceleration is confirmed. Its flexibility and its independence from the interaction range guarantee that the clock method would find decisive applications in systems with many interaction terms.
We study the thermodynamics and phase structures of the asymptotically flat
dilatonic black holes in 4 dimensions, placed in a cavity {\it a la} York, in
string theory for an arbitrary dilaton coupling. We consider these charged
black systems in canonical ensemble for which the temperature at the wall of
and the charge inside the cavity are fixed. We find that the dilaton coupling
plays the key role in the underlying phase structures. The connection of these
black holes to higher dimensional brane systems via diagonal (double) and/or
direct dimensional reductions indicates that the phase structures of the former
may exhaust all possible ones of the latter, which are more difficult to study,
under conditions of similar settings. Our study also shows that a diagonal
(double) dimensional reduction preserves the underlying phase structure while a
direct dimensional reduction has the potential to change it.Comment: 32 pages, 4 figures, 2 tables, a footnote on bubble phase adde
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