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相关概念视频

Angular Momentum: Single Particle01:10

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Angular momentum is directed perpendicular to the plane of the rotation, and its magnitude depends on the choice of the origin. The perpendicular vector joining the linear momentum vector of an object to the origin is called the “lever arm.” If the lever arm and linear momentum are collinear, then the magnitude of the angular momentum is zero. Therefore, in this case, the object rotates about the origin such that it lies on the rim of the circumference defined by the lever arm...
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Angular momentum characterizes an object's rotational motion and is defined as the moment of its linear momentum about a specified point O. When a particle moves along a curved path in the x-y plane, the scalar formulation calculates the magnitude of its angular momentum, utilizing the moment arm (d), representing the perpendicular distance from point O to the line of action of the linear momentum. Despite being scalar in formulation, angular momentum is inherently a vector quantity. Its...
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A system's total angular momentum remains constant if the net external torque acting on the system is zero. Examples of such systems include a freely spinning bicycle tire that slows over time due to torque arising from friction, or the slowing of Earth's rotation over millions of years due to frictional forces exerted on tidal deformations. However in the absence of a net external torque, the angular momentum remains conserved. The conservation of angular momentum principle requires a...
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A system's total angular momentum remains constant if the net external torque acting on the system is zero. Considering a system that consists of n tiny particles, the angular momentum of any tiny particle may change, but the system's total angular momentum would remain constant. The principle of conservation of angular momentum only considers the net external torque acting on the system. While there are internal forces exerted by different particles within the system that also produce...
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Imagine a rigid body with a mass denoted as 'm', which has its center of mass at point G and is rotating around an inertial reference frame. The angular momentum at an arbitrary point P can be calculated by taking the cross product of the position vector and linear momentum vector for each individual mass element.
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轨道角动量微激光器

Pei Miao1, Zhifeng Zhang1, Jingbo Sun1

  • 1Department of Electrical Engineering, The State University of New York at Buffalo, Buffalo, NY 14260, USA.

Science (New York, N.Y.)
|July 30, 2016
PubMed
概括
此摘要是机器生成的。

研究人员创建了一个微环激光器,可以产生轨道角动量 (OAM) . 在非赫密斯光子学中的这一突破精确地控制了OAM拓电荷和极化,用于先进的光通信.

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科学领域:

  • 光学和光学
  • 非赫尔密斯物理学
  • 微型激光器

背景情况:

  • 结构光,包括轨道角动量 (OAM),在光学方面提供了先进的功能.
  • 在微和纳米尺度上生成OAM激光对于增加信息能力至关重要.
  • 非赫尔密斯光子学和特殊点为光学设备提供了新的设计范式.

研究的目的:

  • 展示一个微环激光器能够产生单模OAM.
  • 精确控制OAM模式的拓电荷.
  • 为了实现对辐射偏振辐射的偏振操作.

主要方法:

  • 在特殊情况下利用非赫米特式光子设计原理.
  • 开发用于OAM生成的微环激光结构.
  • 在微激光器内集成偏振控制机制.

主要成果:

  • 成功演示了产生单模OAM旋激光的微环激光.
  • 精确控制生成的OAM模式的拓电荷.
  • 实现对偏振的按需操纵,从而产生辐射偏振.

结论:

  • 开发的OAM微激光器有效地产生和控制OAM波束.
  • 这项技术利用非赫尔密斯光子来实现先进的光学功能.
  • 潜在的应用包括用于量子和经典光通信的下一代集成光电子设备.