Antoniazzi Andrea, Fanelli Duccio, Ruffo Stefano, Yamaguchi Yoshiyuki Y
Dipartimento di Energetica and CSDC, Università di Firenze, and INFN, via S. Marta, 3, 50139 Firenze, Italy.
Phys Rev Lett. 2007 Jul 27;99(4):040601. doi: 10.1103/PhysRevLett.99.040601. Epub 2007 Jul 24.
Systems with long-range interactions display a short-time relaxation towards quasistationary states whose lifetime increases with system size. With reference to the Hamiltonian mean field model, we here show that a maximum entropy principle, based on Lynden-Bell's pioneering idea of "violent relaxation," predicts the presence of out-of-equilibrium phase transitions separating the relaxation towards homogeneous (zero magnetization) or inhomogeneous (nonzero magnetization) quasistationary states. When varying the initial condition within a family of "water bags" with different initial magnetization and energy, first- and second-order phase transition lines are found that merge at an out-of-equilibrium tricritical point. Metastability is theoretically predicted and numerically checked around the first-order phase transition line.
具有长程相互作用的系统会朝着准稳态进行短时间弛豫,其寿命随系统规模增大而增加。参照哈密顿平均场模型,我们在此表明,基于林登 - 贝尔“剧烈弛豫”这一开创性理念的最大熵原理,预测存在非平衡相变,该相变将朝着均匀(零磁化)或非均匀(非零磁化)准稳态的弛豫区分开来。当在具有不同初始磁化强度和能量的一族“水袋”内改变初始条件时,会发现一阶和二阶相变线在一个非平衡三临界点处合并。理论上预测了亚稳性,并在一阶相变线附近进行了数值检验。