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相关概念视频

Space-Time Curvature and the General Theory of Relativity01:17

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In 1905, Albert Einstein published his special theory of relativity. According to this theory, no matter in the universe can attain a speed greater than the speed of light in a vacuum, which thus serves as the speed limit of the universe.
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Gauss's Law: Spherical Symmetry01:26

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A charge distribution has spherical symmetry if the density of charge depends only on the distance from a point in space and not on the direction. In other words, if the system is rotated, it doesn't look different. For instance, if a sphere of radius R is uniformly charged with charge density ρ0, then the distribution has spherical symmetry. On the other hand, if a sphere of radius R is charged so that the top half of the sphere has a uniform charge density ρ1 and the bottom half has...
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Gauss's Law: Cylindrical Symmetry01:20

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A charge distribution has cylindrical symmetry if the charge density depends only upon the distance from the axis of the cylinder and does not vary along the axis or with the direction about the axis. In other words, if a system varies if it is rotated around the axis or shifted along the axis, it does not have cylindrical symmetry. In real systems, we do not have infinite cylinders; however, if the cylindrical object is considerably longer than the radius from it that we are interested in,...
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Gauss's Law: Planar Symmetry01:27

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A planar symmetry of charge density is obtained when charges are uniformly spread over a large flat surface. In planar symmetry, all points in a plane parallel to the plane of charge are identical with respect to the charges. Suppose the plane of the charge distribution is the xy-plane, and the electric field at a space point P with coordinates (x, y, z) is to be determined. Since the charge density is the same at all (x, y) - coordinates in the z = 0 plane, by symmetry, the electric field at P...
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Symmetry in Maxwell's Equations01:28

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Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
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Conservation of Mass in Fixed, Nondeforming Control Volume01:07

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The principle of conservation of mass is fundamental in fluid dynamics and is crucial for analyzing flow within fixed control volumes, such as pipes or ducts. This principle states that the total mass within a control volume remains constant unless altered by the inflow or outflow of mass through the control surfaces. This results in a vital relationship for steady, incompressible flow where the mass entering a system equals the mass leaving it.
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相关实验视频

Updated: May 7, 2026

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
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全维几何相空间光元调节全维几何相空间光元调节

Jinwei Zeng1,2, Jinrun Zhang1,2, Yajuan Dong1,2

  • 1Wuhan National Laboratory for Optoelectronics and School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, 430074 Hubei, China.

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|July 1, 2024
PubMed
概括
此摘要是机器生成的。

研究人员开发了用于全维空间光调制的并行任务元表面. 这一突破使得人们能够独立控制光线.

关键词:
这是一个完整的维度.几何相的几何阶段metasurface 地表的表面是什么平行执行任务并行执行任务.空间光调制的空间光调制

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科学领域:

  • 光学和光子学 在光学和光子学.
  • 超材料是指一种超材料.
  • 轻光调制光的调制方法

背景情况:

  • 全维空间光调制需要同时控制相位,振幅和极化.
  • 实现这些光属性的独立操纵对于先进的光学应用是必不可少的.
  • 当前的元调节技术在管理多个独立的控制因素方面面临挑战.

研究的目的:

  • 提出和演示一种全新的超表面设计,用于全维空间光元调节.
  • 为了实现对光的空间相,振幅和极化进行任意和独立的控制.
  • 克服现有的元调节方法的局限性.

主要方法:

  • 使用几何相概念开发并行任务的超表面.
  • 将元原子划分为子相,用于独立控制.
  • 通过几何相,干扰和直角极化叠加来操纵光特性.

主要成果:

  • 演示了宽带全维空间光元调节.
  • 成功生成了各种类型的结构光.
  • 验证了对光的相位,振幅和偏振的独立控制.

结论:

  • 平行任务的超表面为全维空间光调制提供了可行的解决方案.
  • 拟议的基于几何相位的方法能够对光特性进行前所未有的控制.
  • 这项技术具有显著的潜力,用于各种应用在光操纵.