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On the breakdown of finite-size scaling in high dimensional systems

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Abstract Book of the XXIII IUPAP International Conference on Statistical Physics, Genova, Italy, (9-13 July 2007)

Abstract

Finite-size scaling functions of continuous phase transitions exhibit a scaling anomaly above the upper critical dimension $d_c$. This so-called breakdown of finite-size scaling is well-established on the basis of field theoretical and numerical approaches for system with periodic boundary conditions (BC), both in equilibrium (e.g. the Ising model) and non-equilibrium (e.g. directed percolation 1). Less work was done for geometric phase transitions and for Dirichlet BC. Therefore, we numerically investigate the bond percolation transition in $2 d 10$ dimensions with various boundary conditions. For $d<d_c=6$ the spatial correlation length at criticality, $\xi_c$, is limited by the systems size $L$ for all BCs, whereas it exceeds the systems size as $\xi_c L^d/d_c$ in systems with periodic BC above $d_c$, the hallmark of the breakdown of finite-size scaling. We present, to our knowledge for the first time, a phenomenological and descriptive interpretation of this breakdown of finite-size scaling. Using a generalized distance definition, the correlation length $\xi$ can be directly measured in simulations, even when it exceeds the linear system size $L$. Furthermore, we show that the high-dimensional behavior depends strongly on the boundary conditions. 1) S. Luebeck and H.-K. Janssen, Phys. Rev. E 72, 016119 (2005)

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