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相关概念视频

The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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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

The de Broglie Wavelength

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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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The Bohr Model02:18

The Bohr Model

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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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Electronic Structure of Atoms02:28

Electronic Structure of Atoms

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An atom comprises protons and neutrons, which are contained inside the dense, central core called the nucleus, with electrons present around the nucleus. Taking into account the wave–particle duality of electrons and the uncertainty in position around the nucleus, quantum mechanics provides a more accurate model for the atomic structure. It describes atomic orbitals as the regions around the nucleus where electrons of discrete energy exist, characterized by four quantum...
28.0K
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

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Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
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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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High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
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在大原子数的迪克型模型中真正的量子效应.

Kai Müller1, Walter T Strunz1

  • 1TUD Dresden University of Technology, Institute of Theoretical Physics, 01062, Dresden, Germany.

Physical review letters
|October 5, 2025
PubMed
概括
此摘要是机器生成的。

真正的量子效应仍然存在于具有中观原子数的不平衡开放的迪克模型中. 这与这些效应随着原子数的增加而消失的平衡模型形成鲜明对比,在量子多体系统中揭示了非通行极限.

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科学领域:

  • 量子物理学的量子物理学
  • 量子多体系统是一个量子多体系统.
  • 开放的量子系统是开放的.

背景情况:

  • 狄克模型描述了许多原子的系统中的集体量子现象.
  • 平均场理论经常预测热力学极限 (N→∞) 中的系统行为.
  • 最近的实验实现了在光学空洞中使用超冷气体的驱动和消散量子多体系统.

研究的目的:

  • 在开放的迪克模型中研究超出平均场预测的量子效应.
  • 探索原子数 (N) 对这些量子效应的影响.
  • 为了确定真正的量子现象在很大,有限的N.生存的条件.

主要方法:

  • 对平衡和不平衡的开放迪克模型进行数值研究.
  • 应用一种新的开放系统动力学方法来获得精确的量子动力学结果.
  • 对原子数高达中等距离的系统进行分析 N≈1000.

主要成果:

  • 在平衡的迪克模型中,超出平均场效应随着N的增加而迅速减少.
  • 在不平衡的迪克模型中,确定了量子效应持续存在的中观 N. 的参数模式.
  • 观察到的量子效应包括强烈的稳定状态挤压和在平均场描述中缺少的修改相图.

结论:

  • 对于这些系统,稳定状态极限和热力学极限不会通勤.
  • 真正的量子效应可以在不平衡的迪克模型中在特定条件下在介面镜系统中存活.
  • 平均场描述不足以捕捉大型,有限的开放量子系统中的所有量子现象.