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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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Quantum Numbers02:43

Quantum Numbers

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It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
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Graphing the Wave Function01:13

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Consider the wave equation for a sinusoidal wave moving in the positive x-direction. The wave equation is a function of both position and time. From the wave equation, two different graphs can be plotted.
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Fermi Level Dynamics01:12

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The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
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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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Impulse-Momentum Theorem00:49

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The total change in the motion of an object is proportional to the total force vector acting on it and the time over which it acts. This product is called impulse, a vector quantity with the same direction as the total force acting on the object.
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相关实验视频

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Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
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虚时间格林函数的量子算法

Diksha Dhawan1,2, Dominika Zgid1,3, Mario Motta4

  • 1Department of Chemistry, University of Michigan, Ann Arbor, Michigan 48109, United States.

Journal of chemical theory and computation
|May 18, 2024
PubMed
概括
此摘要是机器生成的。

本研究介绍了一种混合量子-经典算法,用于计算单粒子格林函数,这是模拟分子和材料的关键性质. 这种新方法显示出更准确的量子模拟的前景.

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科学领域:

  • 量子计算是一种量子计算.
  • 计算化学计算化学
  • 材料科学 材料科学 材料科学

背景情况:

  • 格林的函数方法允许精确,可改进的分子和材料的初始模拟.
  • 计算精确的单粒子格林函数对于经典计算机来说是计算密集型的,将模拟限制在小系统上.
  • 状态的光谱函数和密度是通过格林函数方法可访问的实验可观测的属性.

研究的目的:

  • 开发一种混合量子-经典算法,用于计算虚时单粒子格林函数.
  • 为了克服古典计算机在更大的系统中计算格林函数时的局限性.
  • 为分子和材料属性提供一个系统可改进的模拟方法.

主要方法:

  • 一种混合量子-经典方法,结合了变量量子自溶解器 (VQE) 和量子子空间扩张 (QSE).
  • 在雷曼的表示中计算绿色的函数.
  • 在量子模拟器和IBM的量子设备上实施和测试.

主要成果:

  • 成功演示了用于计算虚时单粒子格林函数的混合算法.
  • 通过对H2和H4系统的模拟来验证方法.
  • 该方法在当前量子硬件上的可行性.

结论:

  • 拟议的混合量子-经典算法是计算单粒子格林函数的可行方法.
  • 这种方法为分子和材料的更准确和更可扩展的量子模拟提供了一条途径.
  • 该方法提供了访问诸如光谱函数之类的基本属性,推进了计算化学和材料科学.