非线性波浪传播由一个分数导数控制
Van Thuy Hoang1,2, Justin Widjaja3,4,5, Y Long Qiang3,4
1Institute of Photonics and Optical Science (IPOS), School of Physics A28, The University of Sydney, Sydney, New South Wales, Australia. vanthuy.hoang@sydney.edu.au.
Nature communications
|July 2, 2025
概括
研究人员报告了第一个由分数非线性波方程控制的时间单元的实验观测. 这些单子表现出非指数尾,突出了它们的非局部性质和一个小的时间带宽产物.
科学领域:
- 非线性物理学 非线性物理学
- 波浪现象是一种波浪现象.
- 分数微积分的微积分计算.
背景情况:
- 分数导数在物理学中具有悠久的历史和应用,特别是在具有非局部相互作用的系统中.
- 分数系统的实验研究是罕见的,因为实施的挑战.
研究的目的:
- 通过实验观察和描述由分数非线性波形方程控制的时间单子.
- 为了研究这些单子的独特特性,例如它们的尾巴行为和时间带宽乘积.
主要方法:
- 时间单体的观察和描述.
- 使用分数非线性波方程来描述单体的行为.
主要成果:
- 成功观察并完全描述了一种状单体的家族.
- 证明这些单体具有非指数尾巴,表明它们的非局部特征.
- 测量了一个非常小的时间带宽乘积观察到的单子.
结论:
- 分数单子的实验实现为物理学中研究非局部现象开辟了新的途径.
- 观察到的非指数尾巴和小时间带宽的产物为分数系统的行为提供了独特的见解.
相关概念视频
Linear Approximation in Frequency Domain
137
Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
137
Velocity and Acceleration of a Wave
4.2K
A wave propagates through a medium with a constant speed, known as a wave velocity. It is different from the speed of the particles of the medium, which is not constant. In addition, the velocity of the medium is perpendicular to the velocity of the wave. The variable speed of the particles of the medium implies that there must be acceleration associated with it.
The velocity of the particles can be obtained by taking the partial derivative of the position equation with respect to time....
The velocity of the particles can be obtained by taking the partial derivative of the position equation with respect to time....
4.2K
Propagation of Waves
2.4K
When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
2.4K
Linear Approximation in Time Domain
129
Nonlinear systems often require sophisticated approaches for accurate modeling and analysis, with state-space representation being particularly effective. This method is especially useful for systems where variables and parameters vary with time or operating conditions, such as in a simple pendulum or a translational mechanical system with nonlinear springs.
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
129
Graphing the Wave Function
2.1K
Consider the wave equation for a sinusoidal wave moving in the positive x-direction. The wave equation is a function of both position and time. From the wave equation, two different graphs can be plotted.
2.1K
Traveling Waves: Lossless Lines
203
The provided content explores the behavior of traveling waves on single-phase lossless transmission lines. It begins with a single-phase two-wire lossless transmission line of length Δx, characterized by a loop inductance LH/m and a line-to-line capacitance C F/m. These parameters result in a series inductance LΔx and a shunt capacitance CΔx.
203


