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Discontinuous non-equilibrium phase transition in a threshold Schloegl model for autocatalysis: Generic two-phase coexistence and metastability

机译:自动催化的阈Schloegl模型中的不连续非平衡相变:通用两相共存和亚稳定性

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摘要

Threshold versions of Schloegl\u27s model on a lattice, which involve autocatalytic creation and spontaneous annihilation of particles, can provide a simple prototype for discontinuous non-equilibrium phase transitions. These models are equivalent to so-called threshold contact processes. A discontinuous transition between populated and vacuum states can occur selecting a threshold of N ≥ 2 for the minimum number, N, of neighboring particles enabling autocatalytic creation at an empty site. Fundamental open questions remain given the lack of a thermodynamic framework for analysis. For a square lattice with N = 2, we show that phase coexistence occurs not at a unique value but for a finite range of particle annihilation rate (the natural control parameter). This generic two-phase coexistence also persists when perturbing the model to allow spontaneous particle creation. Such behavior contrasts both the Gibbs phase rule for thermodynamic systems and also previous analysis for this model. We find metastability near the transition corresponding to a non-zero effective line tension, also contrasting previously suggested critical behavior. Mean-field type analysis, extended to treat spatially heterogeneous states, further elucidates model behavior.
机译:Schloegl模型的阈值版本涉及晶格的自动催化生成和粒子的自发an灭,可以为不连续的非平衡相变提供简单的原型。这些模型等效于所谓的阈值接触过程。为最小数量的N相邻粒子选择阈值N≥2时,会发生填充状态和真空状态之间的不连续过渡,从而可以在空位自动生成催化。鉴于缺乏热力学分析框架,根本性的悬而未决的问题仍然存在。对于N = 2的方格,我们表明相位共存不是在唯一值处发生,而是在有限范围的粒子an灭率(自然控制参数)下发生。当干扰模型以允许自发创建粒子时,这种通用的两相共存也会继续存在。这种行为既与热力学系统的吉布斯相位定律相反,也与该模型的先前分析相反。我们发现过渡附近的亚稳态对应于非零有效线张力,也与先前建议的临界行为形成对比。扩展为处理空间异构状态的均值场类型分析进一步阐明了模型行为。

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