非线性福克-普朗克方程与非辐射漂移力和异性潜力
V T F de Luca1, R S Wedemann1,2, A R Plastino3
1Instituto de Matemática e Estatística, Universidade do Estado do Rio de Janeiro (UERJ), Rua São Francisco Xavier, 524, Rio de Janeiro 20550-900, RJ, Brazil.
Chaos (Woodbury, N.Y.)
|September 5, 2025
概括
这项研究探讨了非线性福克-普朗克方程与不对称潜力和非渐变力. 它揭示了依赖时间的q-Gaussian解决方案,这些解决方案演变为静止状态,适用于具有不对称相互作用的复杂系统.
科学领域:
- 统计物理
- 复杂系统理论
- 非线性动力学
背景情况:
- 非线性福克-普朗克方程通常以梯度漂移力模型系统.
- 对于更广泛的应用来说,研究具有非渐变力和不对称潜力的系统至关重要.
研究的目的:
- 分析非线性福克-普朗克方程的梯度 (不对称的潜力) 和非梯度力.
- 确定静止的q指数解的条件,并分析时间依赖的q高斯解.
主要方法:
- 非线性福克-普朗克方程的数学分析.
- 从不断变化的概率密度中推导和数值研究粒子轨迹.
- 探索与非辐射项相结合的异型波潜力.
主要成果:
- 有时间依赖的q-高斯式解决方案演变为静止状态.
- 确定允许使用q指数式静止溶液的条件.
- 与这些溶液相关的粒子轨迹的数值研究.
结论:
- 开发的理论框架扩展了基于Sq的非线性福克-普朗克方程的适用性.
- 能够建模具有不对称相互作用的复杂系统,例如神经网络.
- 提供了超越传统潜力驱动模型的系统动态见解.
相关概念视频
Poisson's And Laplace's Equation
3.4K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
3.4K
Navier–Stokes Equations
730
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
730
Force and Potential Energy in One Dimension
5.5K
Force can be calculated from the expression for potential energy, which is a function of position. The component of a conservative force, in a particular direction, equals the negative of the derivative of the corresponding potential energy with respect to the displacement in that direction. For regions where potential energy changes rapidly with displacement, the work done and force is maximum. Also, when force is applied along the positive coordinate axis, the potential energy decreases with...
5.5K
Differential Form of Maxwell's Equations
634
James Clerk Maxwell (1831–1879) was one of the significant contributors to physics in the nineteenth century. He is probably best known for having combined existing knowledge of the laws of electricity and the laws of magnetism with his insights to form a complete overarching electromagnetic theory, represented by Maxwell's equations. The four basic laws of electricity and magnetism were discovered experimentally through the work of physicists such as Oersted, Coulomb, Gauss, and...
634
Force and Potential Energy in Three Dimensions
5.0K
Consider a particle moving under the action of a conservative force that has components along each coordinate axis. Each component of force is a function of the coordinates. The potential energy function U is also a function of all three spatial coordinates. Force in one dimension can be written as the negative ratio of potential energy change to the displacement along that coordinate. For minimal displacement, the ratios become derivatives. If a function has many variables, the derivative only...
5.0K
Carrier Transport
561
The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
561


