在两个非 ergodic 可逆细胞自动机上,一个是古典的,另一个是量子的
1Faculty of Mathematics and Physics, University of Ljubljana, Jadranska 19, SI-1000 Ljubljana, Slovenia.
Entropy (Basel, Switzerland)
|May 27, 2023
概括
我们介绍了两种具有独特性质的简单运动粒子模型. 一个模型揭示了非ergodic行为和潜在的可整合性,而另一个模型则生成无限保留的运算符,称为滑翔机运算符.
科学领域:
- 统计力学 统计力学
- 凝聚物质物理学 凝聚物质物理学
- 计算物理 计算物理
背景情况:
- 蜂自动机为复杂的物理系统提供了简化的模型.
- 动力粒子模型对于理解新兴现象至关重要.
- 格子气体模型为流体动力学和统计性质提供了洞察力.
研究的目的:
- 提出和分析两个新的1+1维动力粒子模型.
- 探索决定性,可逆自动机及其保存量的特性.
- 为了研究一个带电的硬点格子气体及其保守运算符的量子变形.
主要方法:
- 开发了两个具有不同粒子类型和相互作用的细胞自动机模型.
- 分析连续性方程以确定保存的电荷和电流.
- 对-巴克斯特方程和量子变形的相关同一性的研究.
主要成果:
- 第一个模型展示了三个保存电荷,其中一个电荷和电流是九个站点的支持,表明非ergodicity和潜在的可集成性.
- 第二个模型,量子变形,满足-巴克斯特相关的身份,导致无限的滑翔机操作员.
- 这两种模型都显示出有趣的特性,适合进一步的研究和应用.
结论:
- 拟议的动力粒子模型为研究复杂系统提供了简单但强大的框架.
- 发现非ergodic行为和无限保存运算符突出显示了新应用的潜力.
- 这些模型需要进一步研究它们的数学结构和物理含义.
相关概念视频
Entropy Change in Reversible Processes
2.6K
In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
2.6K
Woodward–Hoffmann Selection Rules and Microscopic Reversibility
3.2K
Electrocyclic reactions, cycloadditions, and sigmatropic rearrangements are concerted pericyclic reactions that proceed via a cyclic transition state. These reactions are stereospecific and regioselective. The stereochemistry of the products depends on the symmetry characteristics of the interacting orbitals and the reaction conditions. Accordingly, pericyclic reactions are classified as either symmetry-allowed or symmetry-forbidden. Woodward and Hoffmann presented the selection criteria for...
3.2K
Non-equilibrium in the Cell
4.5K
An important concept in studying metabolism and energy is that of chemical equilibrium. Most chemical reactions are reversible. They can proceed in both directions, releasing energy into their environment in one direction, and absorbing it from the environment in the other direction. The same is true for the chemical reactions involved in cell metabolism, such as the breaking down and building up of proteins into and from individual amino acids, respectively. Reactants within a closed system...
4.5K
The Quantum-Mechanical Model of an Atom
42.6K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
42.6K
Reversible and Irreversible Processes
4.3K
The thermodynamic processes can be classified into reversible and irreversible processes. The processes that can be restored to their initial state are called reversible processes. It is only possible if the process is in quasi-static equilibrium, i.e., it takes place in infinitesimally small steps, and the system remains at equilibrium However, these are ideal processes and do not occur naturally. An ideal system undergoing a reversible process is always in thermodynamic equilibrium within...
4.3K
Reaction Quotient
48.7K
The status of a reversible reaction is conveniently assessed by evaluating its reaction quotient (Q). For a reversible reaction described by m A + n B ⇌ x C + y D, the reaction quotient is derived directly from the stoichiometry of the balanced equation as
48.7K


