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相关概念视频

The Quantum-Mechanical Model of an Atom02:45

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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Atomic Nuclei: Nuclear Spin State Overview01:03

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NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
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Mathematically, the motion of a wave can be studied using a wavefunction. Consider a string oscillating up and down in simple harmonic motion, having a period T. The wave on the string is sinusoidal and is translated in the positive x-direction as time progresses. Sine is a function of the angle θ, oscillating between +A and −A and repeating every 2π radians. To construct a wave model, the ratio of the angle θ and the position x is considered.
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In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
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Updated: Jun 29, 2025

Generation and Coherent Control of Pulsed Quantum Frequency Combs
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对于交互的量子旋转厅阶段的变量张力波函数.

Yixin Ma1, Shenghan Jiang1, Chao Xu1

  • 1Kavli Institute for Theoretical Sciences, University of Chinese Academy of Sciences, Beijing 100190, China.

Physical review letters
|April 5, 2024
PubMed
概括
此摘要是机器生成的。

我们介绍了一种新的张量网络方法来模拟复杂材料中的量子自旋霍尔 (QSH) 阶段. 这种方法模拟了拓绝缘体及其边缘状态,推进了对相关系统的研究.

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科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 量子力学就是量子力学.
  • 材料科学 材料科学 材料科学

背景情况:

  • 量子自旋霍尔 (QSH) 阶段是一个二维拓绝缘体,由于时间逆向对称性,具有受保护的螺旋边缘模式.
  • 这一阶段可以发生在超出传统带理论范围的强相关系系统中.

研究的目的:

  • 在现实的相关模型中开发一个新的框架来模拟QSH阶段.
  • 克服目前对拓绝缘体的模拟技术的局限性.

主要方法:

  • 利用费米子张量网络状态来构建固定点波函数的张量表示.
  • 从一个确切的可解决模型中推导出张量方程来描述对称性转换.
  • 通过解决这些张量方程,获得了QSH阶段的变量替代品.

主要成果:

  • 开发了一种方法来推导描述QSH阶段的异常边缘理论.
  • 成功获得了QSH阶段的变异替代品.
  • 通过数值计算验证了QSH阶段的拓性质.

结论:

  • 拟议的张量网络方法是模拟强相关系系统中的QSH阶段的可行第一步.
  • 这项工作为使用张量算法研究复杂材料中的拓现象开辟了新的途径.