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相关概念视频

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...
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Induced Electric Dipoles01:28

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A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
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Molecular Orbital Theory II03:51

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Molecular Orbital Energy Diagrams
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Electric Dipoles and Dipole Moment01:30

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Consider two charges of equal magnitude but opposite signs. If they cannot be separated by an external electric field, the system is called a permanent dipole. For example, the water molecule is a dipole, making it a good solvent.
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Structure of Benzene: Molecular Orbital Model01:18

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According to the molecular orbital (MO) model, benzene has a planar structure with a regular hexagon of six sp2 hybridized carbons. As shown in Figure 1, each carbon is bonded to three other atoms with C–C–C and H–C–C bond angles of 120°. The C–H bond length is 109 pm, and the C–C bond length is 139 pm which is midway between the single bond length of sp3 hybridized carbons (154 pm) and sp2 hybridized carbons (133 pm).
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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
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相关实验视频

Updated: Aug 28, 2025

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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用双极激子扩展的斯-哈巴德模型

C Lagoin1, U Bhattacharya2, T Grass2

  • 1Institut des Nanosciences de Paris, CNRS and Sorbonne Université, Paris, France.

Nature
|September 14, 2022
PubMed
概括
此摘要是机器生成的。

研究人员使用二极激子在2D网格中实现了扩展波斯-哈密尔顿式. 这使得在斯-哈巴德模型系统中可以观察象棋盘的顺序.

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相关实验视频

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科学领域:

  • 凝聚物质物理学
  • 量子模拟
  • 人工格子

背景情况:

  • 哈伯德模型是理解强相关量子系统的关键.
  • 实验实现长距离相互作用的扩展波斯-哈巴德模型是具有挑战性的.
  • 扩展的Bose-Hubbard模型预测了小部分填充的新秩序阶段.

研究的目的:

  • 在实验中实现波斯 - 哈密尔顿扩展式.
  • 在一个新的量子系统中研究隔离有序相.
  • 探索二极激子在量子模拟中的潜力.

主要方法:

  • 限制半导体双极激子在一个二维的人造正方形格子.
  • 使用强大的双极排斥来进行近邻相互作用.
  • 实现一个具有可编程几何形状和100多个站点的网格.

主要成果:

  • 在半填充时稳定绝缘状态.
  • 观察与棋盘空间顺序一致的签名.
  • 用外站互动对玻色子类阵列的控制实施的演示.

结论:

  • 双极激子为实现扩展的斯-哈伯德物理学提供了一个平台.
  • 这项工作开辟了模拟可调节相互作用的复杂量子相的途径.
  • 该系统允许可编程格子几何和大规模量子模拟.