Paoluzzi Matteo, Levis Demian, Crisanti Andrea, Pagonabarraga Ignacio
<a href="https://ror.org/00ygy3d85">Istituto per le Applicazioni del Calcolo del Consiglio Nazionale delle Ricerche</a>, Via Pietro Castellino 111, 80131 Naples, Italy.
Dipartimento di Fisica, <a href="https://ror.org/02be6w209">Sapienza Università di Roma Piazzale A. Moro 2</a>, I-00185 Rome, Italy.
Phys Rev Lett. 2024 Sep 13;133(11):118301. doi: 10.1103/PhysRevLett.133.118301.
Within the Landau-Ginzburg picture of phase transitions, scalar field theories develop phase separation because of a spontaneous symmetry-breaking mechanism. This picture works in thermodynamics but also in the dynamics of phase separation. Here we show that scalar nonequilibrium field theories undergo phase separation just because of nonequilibrium fluctuations driven by a persistent noise. The mechanism is similar to what happens in motility-induced phase separation where persistent motion introduces an effective attractive force. We observe that noise-induced phase separation occurs in a region of the phase diagram where disordered field configurations would otherwise be stable at equilibrium. Measuring the local entropy production rate to quantify the time-reversal symmetry breaking, we find that such breaking is concentrated on the boundary between the two phases.
在朗道 - 金兹堡相变图景中,标量场理论由于自发对称性破缺机制而发生相分离。这一图景不仅适用于热力学,也适用于相分离动力学。在此我们表明,标量非平衡场理论发生相分离仅仅是由于由持续噪声驱动的非平衡涨落。该机制类似于在运动诱导相分离中发生的情况,其中持续运动引入了有效的吸引力。我们观察到,噪声诱导的相分离发生在相图的一个区域,在该区域中无序场构型在平衡时原本是稳定的。通过测量局部熵产生率来量化时间反演对称性破缺,我们发现这种破缺集中在两相之间的边界上。