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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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The de Broglie Wavelength02:32

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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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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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Equilibrium Conditions for a Particle01:23

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When an object is in equilibrium, it is either at rest or moving with a constant velocity. There are two types of equilibrium: static and dynamic. Static equilibrium occurs when an object is at rest, while dynamic equilibrium occurs when an object is moving with a constant velocity. In both cases, there must be a balance of forces acting on the object.
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Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as the...
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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Gradient Echo Quantum Memory in Warm Atomic Vapor
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在驱动的Rydberg原子阵列中控制量子多体动力学

D Bluvstein1, A Omran1,2, H Levine1

  • 1Department of Physics, Harvard University, Cambridge, MA 02138, USA.

Science (New York, N.Y.)
|February 26, 2021
PubMed
概括
此摘要是机器生成的。

研究人员使用周期性驱动稳定了量子多体痕. 这种方法控制了复杂的量子动力学,并显示了量子信息科学应用的潜力.

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科学领域:

  • 量子物理学
  • 多体系统
  • 量子动力学

背景情况:

  • 在多体系统中控制不平衡的量子动力学是很困难的.
  • 量子系统中的相互作用往往导致希尔伯特空间的混乱扩散.

研究的目的:

  • 在强烈相互作用的量子比特系统中研究快速灭后的不平衡动态.
  • 探索稳定量子多体痕的方法.

主要方法:

  • 使用Rydberg原子阵列的可编程量子模拟器.
  • 在3到200个量子位的多体系统中应用周期性驱动.
  • 在一个和两个空间维度中研究系统.

主要成果:

  • 证明了连贯复苏与量子多体痕的稳定性.
  • 观察到一个强大的亚响应类似于离散的时间晶体顺序.
  • 绘制了希尔伯特空间动态,几何,相图和系统大小依赖.

结论:

  • 周期性驾驶提供了一种新的方式来控制多体系统中的复杂动力学.
  • 这种量子动态的控制在量子信息科学中具有潜在的应用.