Binder parameter

The Binder parameter or Binder cumulant^[1][2] in statistical physics, also known as the fourth-order cumulant ${\displaystyle U_{L}=1-{\frac {{\langle s^{4}\rangle }_{L}}{3{\langle s^{2}\rangle }_{L}^{2}}}}$ is defined as the kurtosis (more precisely, minus one third times the excess kurtosis) of the order parameter, s, introduced by Austrian theoretical physicist Kurt Binder. It is frequently used to determine accurately phase transition points in numerical simulations of various models.^[3]

The phase transition point is usually identified comparing the behavior of ${\displaystyle U}$ as a function of the temperature for different values of the system size ${\displaystyle L}$. The transition temperature is the unique point where the different curves cross in the thermodynamic limit. This behavior is based on the fact that in the critical region, ${\displaystyle T\approx T_{c}}$, the Binder parameter behaves as ${\displaystyle U(T,L)=b(\epsilon L^{1/\nu })}$, where ${\displaystyle \epsilon ={\frac {T-T_{c}}{T}}}$.

Accordingly, the cumulant may also be used to identify the universality class of the transition by determining the value of the critical exponent ${\displaystyle \nu }$ of the correlation length.^[1]

In the thermodynamic limit, at the critical point, the value of the Binder parameter depends on boundary conditions, the shape of the system, and anisotropy of correlations. ^[1][4][5][6]

A generalization called the geometric Binder cumulant (GBC) also exists.^[7] Unlike the conventional Binder cumulant, which is based on expectation values of operators representing physical quantities, the GBC implements the Binder cumulant scheme in cases in which the relevant physical quantity is a geometric phase, which happens in many systems which are inherently quantum mechanical. For example, bulk dielectric polarization in crystalline insulators can only be described as a geometric phase, the associated Binder cumulant is a GBC. In this case the GBC can be used as a gauge of the metal-insulator transition, which is an example of a quantum phase transition.

1. ^ ^{a b c} Binder, K. (1981). "Finite size scaling analysis of ising model block distribution functions". Zeitschrift für Physik B: Condensed Matter. 43 (2): 119–140. Bibcode:1981ZPhyB..43..119B. doi:10.1007/bf01293604. ISSN 0340-224X. S2CID 121873477.
2. ^ Binder, K. (1981-08-31). "Critical Properties from Monte Carlo Coarse Graining and Renormalization". Physical Review Letters. 47 (9): 693–696. Bibcode:1981PhRvL..47..693B. doi:10.1103/physrevlett.47.693. ISSN 0031-9007.
3. ^ K. Binder, D. W. Heermann, Monte Carlo Simulation in Statistical Physics: An Introduction (2010) Springer
4. ^ Kamieniarz, G; Blote, H W J (1993-01-21). "Universal ratio of magnetization moments in two-dimensional Ising models". Journal of Physics A: Mathematical and General. 26 (2): 201–212. Bibcode:1993JPhA...26..201K. doi:10.1088/0305-4470/26/2/009. ISSN 0305-4470.
5. ^ Chen, X. S.; Dohm, V. (2004-11-30). "Nonuniversal finite-size scaling in anisotropic systems". Physical Review E. 70 (5) 056136. arXiv:cond-mat/0408511. Bibcode:2004PhRvE..70e6136C. doi:10.1103/physreve.70.056136. ISSN 1539-3755. PMID 15600721. S2CID 44785145.
6. ^ Selke, W; Shchur, L N (2005-10-19). "Critical Binder cumulant in two-dimensional anisotropic Ising models". Journal of Physics A: Mathematical and General. 38 (44): L739 – L744. arXiv:cond-mat/0509369. doi:10.1088/0305-4470/38/44/l03. ISSN 0305-4470. S2CID 14774533.
7. ^ Hetényi, B.; Cengiz, S. "Geometric cumulants associated with adiabatic cycles crossing degeneracy points: Application to finite size scaling of metal-insulator transitions in crystalline electronic systems". Physical Review B. 106: 195101. doi:10.1103/PhysRevB.106.195151.

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