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Power Dissipated in a Circuit: Problem Solving01:15

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The equivalent resistance of a combination of resistors depends on their values and how they are connected.
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In an atom, the negatively charged electrons are attracted to the positively charged nucleus. In a multielectron atom, electron-electron repulsions are also observed. The attractive and repulsive forces are dependent on the distance between the particles, as well as the sign and magnitude of the charges on the individual particles. When the charges on the particles are opposite, they attract each other. If both particles have the same charge, they repel each other.
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Atoms — and the protons, neutrons, and electrons that compose them — are extremely small. For example, a carbon atom weighs less than 2 × 10−23 g. When describing the properties of tiny objects such as atoms, we use appropriately small units of measure, such as the atomic mass unit (amu). The amu was originally defined based on hydrogen, the lightest element, then later in terms of oxygen. Since 1961, it has been defined with regard to the most abundant isotope of carbon, atoms of which...
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An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.
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The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
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相互作用的赖德伯格原子的集体消散工程.

Tao Chen1,2,3, Chenxi Huang1,2, Jacob P Covey1

  • 1University of Illinois at Urbana-Champaign, Department of Physics, Urbana, Illinois 61801-3080, USA.

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概括
此摘要是机器生成的。

工程消散提供了新的量子控制. 研究人员开发了激光诱导的原子损失来操纵量子状态,揭示了相互作用效应,并使量子系统的新准备方法成为可能.

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科学领域:

  • 量子物理学 量子物理学 是一种量子物理学.
  • 原子物理 原子物理
  • 量子光学是一种量子光学.

背景情况:

  • 工程消散是一种用于量子状态控制的新方法.
  • 它使得高保真度的准备,转移,稳定和访问新的量子相位过渡成为可能.
  • 控制开放的量子系统对于量子技术至关重要.

研究的目的:

  • 实现一个可调节的,状态解析的激光诱导损失通道,用于单个Rydberg原子.
  • 在非相互作用和强烈相关的环境中探索工程消散的影响.
  • 展示相关量子状态的散射制备的新方法.

主要方法:

  • 使用Rydberg原子创建一个可调节的,状态解析的激光诱导损失通道.
  • 研究单个原子和强烈相关的设置.
  • 具有工程消散的多体链的理论建模.

主要成果:

  • 揭示了量子泽诺和反泽诺政权之间的异常点的相互作用驱动的转移.
  • 证明了相互作用增强的衰变.
  • 观察到一种选择性配置的双体Zeno效应,可以结目标自旋状态.
  • 理论上显示了多体链中不需要的旋转配置的消耗性蒸.

结论:

  • 为探索强烈相互作用,开放的量子自旋系统建立了通用方法.
  • 在里德伯格原子数组中开启了对相关量子态的消散性准备的新程序.
  • 突出了工程消散对于量子状态控制和新型相位过渡的潜力.