Magnetic-glassy multicritical behavior of the three-dimensional +- J Ising model
| dc.creator | Hasenbusch, M. | |
| dc.creator | Toldin, F. Parisen | |
| dc.creator | Pelissetto, A. | |
| dc.creator | Vicari, E. | |
| dc.date | 2007-07-19 | |
| dc.date.accessioned | 2026-07-07T08:42:10Z | |
| dc.date.available | 2026-07-07T08:42:10Z | |
| dc.description | We consider the three-dimensional $\pm J$ model defined on a simple cubic lattice and study its behavior close to the multicritical Nishimori point where the paramagnetic-ferromagnetic, the paramagnetic-glassy, and the ferromagnetic-glassy transition lines meet in the T-p phase diagram (p characterizes the disorder distribution and gives the fraction of ferromagnetic bonds). For this purpose we perform Monte Carlo simulations on cubic lattices of size $L\le 32$ and a finite-size scaling analysis of the numerical results. The magnetic-glassy multicritical point is found at $p^*=0.76820(4)$, along the Nishimori line given by $2p-1={\rm Tanh}(J/T)$. We determine the renormalization-group dimensions of the operators that control the renormalization-group flow close to the multicritical point, $y_1 = 1.02(5)$, $y_2 = 0.61(2)$, and the susceptibility exponent $η= -0.114(3)$. The temperature and crossover exponents are $ν=1/y_2=1.64(5)$ and $ϕ=y_1/y_2 = 1.67(10)$, respectively. We also investigate the model-A dynamics, obtaining the dynamic critical exponent $z = 5.0(5)$. | |
| dc.description | 17 pages | |
| dc.identifier | https://arxiv.org/abs/0707.2866 | |
| dc.identifier | http://arxiv.org/abs/0707.2866 | |
| dc.identifier | Phys. Rev. B 76 (2007), 184202 | |
| dc.identifier | doi:10.1103/PhysRevB.76.184202 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/141871 | |
| dc.subject | Disordered Systems and Neural Networks | |
| dc.title | Magnetic-glassy multicritical behavior of the three-dimensional +- J Ising model | |
| dc.type | text |