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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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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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Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He...
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Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If...
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Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
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量子通道中的量子古典对应.

Bidhi Vijaywargia1, Arul Lakshminarayan1

  • 1Indian Institute of Technology Madras, Department of Physics, & Center for Quantum Information, Computation and Communication, Chennai 600036, India.

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此摘要是机器生成的。

本研究介绍了古典库普曼通道作为量子通道的类比,使量子和古典动力学的比较分析成为可能. 结果显示,量子通道行为受到经典相位空间稳定性和混乱的影响.

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科学领域:

  • 量子力学就是量子力学.
  • 经典机械学 经典机械学
  • 动态系统理论 动态系统理论

背景情况:

  • 量子通道模型开放系统演变.
  • 古典库普曼运算子理论分析了相空间中的函数演变.

研究的目的:

  • 建立古典库普曼通道作为量子通道的类比.
  • 在通道层面探索量子-经典对应.
  • 为了比较量子和经典通道的光谱特性.

主要方法:

  • 确定四个古典的库普曼通道,类似于量子通道.
  • 将通道解释为杂的单粒子系统.
  • 使用合的旋转机模型进行比较光谱分析.

主要成果:

  • 经典库普曼通道为研究量子-经典对应提供了一个框架.
  • 量子通道模式受到稳定的经典相位空间区域的显著影响.
  • 混乱的动态导致环状的光谱密度,由随机矩阵理论描述.
  • 经典的极限方法导致光谱环缩小,幸存模式显示痕.

结论:

  • 古典库普曼通道为量子和古典限制理论提供了新的见解.
  • 该研究强调了经典相位空间结构和量子光谱特性之间的相互作用.
  • 在幸存的量子模式中观察到不稳定的多元体和周期轨道的痕效应.