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相关概念视频

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.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
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¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

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The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
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Quantifying Work02:30

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As a system undergoes a change, its internal energy can change, and energy can be transferred from the system to the surroundings, or from the surroundings to the system. 
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

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Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
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Work-energy Theorem01:42

Work-energy Theorem

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According to Newton’s second law of motion, the sum of all the forces acting on a particle (net force) determines the rate of change in the momentum of the particle (motion). Therefore, we should consider the work done by all forces acting on a particle, or the net work, to see its effect on the particle’s motion.
The work-energy theorem equates work done by all the forces on an object to the change in its kinetic energy. The theorem can be used to calculate work done by a force...
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相关实验视频

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Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
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强储水库合的量子工作统计

Owen Diba1, Harry J D Miller1, Jake Iles-Smith1

  • 1Department of Physics and Astronomy, The University of Manchester, Manchester M13 9PL, United Kingdom.

Physical review letters
|May 28, 2024
PubMed
概括
此摘要是机器生成的。

一个新的极子变换简化了对与水库紧密合的量子系统所做的计算工作. 这种方法与随机热力学一致,并揭示了驱动系统中的环境合效应.

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科学领域:

  • 量子热力学就是量子热力学.
  • 统计力学就是统计力学.
  • 凝聚物质物理学 凝聚物质物理学

背景情况:

  • 在强储备合的量子系统中计算工作统计是复杂的.
  • 现有的方法往往需要完全的系统-水库自身频谱计算.

研究的目的:

  • 开发一种方法来规避量子热力学中的复杂计算.
  • 研究环境合对驱动量子系统的影响.

主要方法:

  • 利用极子变换将系统映射到一个弱合框架中.
  • 在转换的框架中应用弱合理论.
  • 分析Jarzynski波动定理的一致性.

主要成果:

  • 波拉龙方法成功地复制了Jarzynski波动定理.
  • 在Landau-Zener过渡的劳动分配中发现了环境合的明确标志.
  • 该方法允许分析超越马科维安和弱合制度.

结论:

  • 极子变换为非马科夫系统的量子热力学提供了一种可处理的方法.
  • 这种形式主义为环境与系统合的作用提供了新的见解.
  • 该方法适用于驱动量子系统,包括那些接近临界过渡的量子系统.