The Kahn–Kalai conjecture is a conjecture in combinatorial geometry, specifically related to the understanding of the behavior of random sets and their expected properties. It focuses on a certain type of subset of a finite set and is named after the mathematicians Ben Kahn and Gil Kalai, who introduced this conjecture.
Kaniadakis statistics is a generalization of traditional statistical mechanics that extends the principles of the Boltzmann-Gibbs (BG) statistics to incorporate the effects of non-extensive systems. Developed by the physicist Georgios Kaniadakis, this statistical framework is particularly useful in describing complex systems characterized by long-range interactions, non-Markovian processes, or systems far from equilibrium.
The Kardar–Parisi–Zhang (KPZ) equation is a fundamental equation in statistical physics that describes the dynamics of interface growth and evolution, particularly in the context of stochastic processes. It was introduced by Mehran Kardar, Giorgio Parisi, and Yi-Cheng Zhang in 1986. The KPZ equation is notable for its relevance in various fields, including nonequilibrium statistical mechanics, surface growth phenomena, and even in connection to certain problems in mathematical physics and probability theory.
Kinetic Monte Carlo (KMC) is a stochastic simulation method used to model the time evolution of a system where individual events occur randomly over time. It is particularly useful for studying processes in materials science, chemistry, and biological systems, where the dynamics involve many possible pathways and interactions that can be complex and diverse. ### Key Features of Kinetics Monte Carlo: 1. **Event-Driven**: KMC focuses on discrete events rather than continuous trajectories.
Kinetic exchange models of markets are a type of economic model that use concepts from statistical mechanics and kinetic theory to describe the behavior of markets through the interactions of agents. These models typically focus on how individual agents (such as traders or investors) make decisions about buying and selling based on their local information, interactions with other agents, and the aggregated effects of these interactions over time.
A kinetic scheme refers to a mathematical framework or model used to describe the behavior of a system's particles in terms of their individual trajectories, velocities, and interactions. This concept is often employed in fields like statistical mechanics, fluid dynamics, and kinetic theory. In more detail: 1. **Kinetic Theory of Gases**: In physics, the kinetic theory of gases explains the macroscopic properties of gases in terms of their microscopic constituents (the molecules) and their kinetic energy.
The Kirkwood–Buff solution theory is a theoretical framework used in physical chemistry and statistical mechanics to describe the properties of solutions, especially regarding interactions between molecules in a solvent. It provides a systematic way to understand the behavior of mixtures and solutions by relating macroscopic observable properties (like concentration and thermodynamic functions) to microscopic interactions between individual particles.
The Knudsen paradox refers to a phenomenon in the field of gas dynamics, particularly in the context of kinetic theory of gases. It arises when discussing the behavior of gas molecules in a low-density environment, where the mean free path (the average distance traveled between collisions) is comparable to or larger than the dimensions of the system.
The Kovacs effect describes a phenomenon observed in certain materials, particularly polymers and glasses, during the process of physical aging. When a material is subject to a temperature change, especially in a glassy state, it can exhibit a non-linear response to stress or strain. More specifically, when a sample is suddenly subjected to a step change in temperature (for example, from below to above its glass transition temperature), it can exhibit a characteristic "overshoot" in its mechanical properties.
The Kramers–Moyal expansion is a mathematical framework used in stochastic processes, particularly in the context of describing the dynamics of systems subjected to random influences. It provides a way to derive the Fokker-Planck equation, which governs the time evolution of the probability density function of a stochastic variable. **Key concepts of the Kramers-Moyal expansion:** 1.
Kramers–Wannier duality is a concept from statistical mechanics and condensed matter physics that describes a relationship between two statistical systems, particularly in the context of lattice models. It was originally discovered in the context of the two-dimensional Ising model, but it applies more broadly to other statistical systems as well.
Landau theory, often referred to as Landau's theory of phase transitions, is a framework developed by the Soviet physicist Lev Landau in the early 20th century to describe phase transitions in physical systems. It provides a mathematical formalism for understanding how a system changes from one phase to another, typically as a function of temperature or other external parameters.
Langevin dynamics is a computational and theoretical framework used to simulate the behavior of systems in statistical mechanics, particularly in the context of molecular dynamics. It incorporates both conservative forces (which represent the interactions among particles) and stochastic forces (which model the effect of thermal fluctuations). The Langevin equation is the central mathematical description used in Langevin dynamics.
The Langevin equation is a stochastic differential equation that describes the evolution of a system influenced by both deterministic and random forces. It is commonly used in statistical mechanics, classical mechanics, and various fields like physics and chemistry to model systems that exhibit Brownian motion and other forms of stochastic behavior.
The Laplace principle, also known in the context of large deviations theory, provides a way to understand the asymptotic behavior of probability measures for large samples. It typically focuses on the probability of deviations of random variables from their expected values.
Lattice Density Functional Theory (LDFT) refers to a theoretical framework that extends concepts from traditional density functional theory (DFT) to study systems where lattice structures play a significant role. DFT itself is a computational quantum mechanical method used to investigate the electronic structure of many-body systems, primarily in the context of condensed matter physics and quantum chemistry. It relies on the electron density as the central variable, rather than the many-body wave function, which simplifies the calculations significantly.
The Lieb–Liniger model is a theoretical framework used in condensed matter physics and quantum mechanics to describe a one-dimensional system of interacting particles. Specifically, it focuses on a system of bosons or fermions that interact via a delta-function potential.
The Lifson–Roig model is a theoretical framework used to describe the dynamics of polymer chains, particularly in the context of statistical mechanics and polymer physics. Developed by the physicists I. Lifson and M. Roig in the 1960s, the model provides insights into the behavior of flexible polymers or polypeptides in solution, focusing on aspects such as chain conformation and interactions.
A list of statistical mechanics articles typically includes research papers, review articles, and key contributions to the field that cover a wide range of topics related to statistical mechanics. These topics can include foundational principles, thermodynamics, phase transitions, ensemble theories, and applications in various fields such as physics, chemistry, and biology.
Here is a list of notable textbooks in thermodynamics and statistical mechanics that are widely used in academia: ### Classical Thermodynamics 1. **"Thermodynamics: An Engineering Approach" by Yunus Çengel and Michael Boles** - This book focuses on thermodynamics principles with an engineering application perspective. 2. **"Fundamentals of Thermodynamics" by Richard E. Sonntag, Claus Borgnakke, and Gordon J.