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相关概念视频

Zeroth Law of Thermodynamics01:14

Zeroth Law of Thermodynamics

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Experimentally, if object A is in equilibrium with object B, and object B is in equilibrium with object C, then object A is in equilibrium with object C. That statement of transitivity is called the "zeroth law of thermodynamics." For example, a cold metal block and a hot metal block are both placed on a metal plate at room temperature. Eventually, the cold block and the plate will be in thermal equilibrium. In addition, the hot block and the plate will be in thermal equilibrium.
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Entropy and the Second Law of Thermodynamics01:20

Entropy and the Second Law of Thermodynamics

2.6K
The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
The relation  between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
2.6K
Third Law of Thermodynamics02:38

Third Law of Thermodynamics

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A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
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Thermodynamic Systems01:06

Thermodynamic Systems

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A thermodynamic system is a set of objects whose thermodynamic properties are of interest. The system is considered to be embedded in its surroundings or the environment. The system and its environment can exchange heat and do work on each other through a boundary that separates them. However, the immediate surroundings of the system interact with it directly and therefore have a much stronger influence on its behavior and properties.
Consider an example of  tea boiling in a kettle. The...
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

885
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.
885
Second Law of Thermodynamics02:49

Second Law of Thermodynamics

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In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Processes that involve an increase in entropy of the system (ΔS > 0) are very often spontaneous; however, examples to the contrary are plentiful. By expanding consideration of entropy changes to include the surroundings, a significant conclusion regarding the relation between this property and spontaneity may be reached. In thermodynamic...
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相关实验视频

Updated: May 7, 2025

Gradient Echo Quantum Memory in Warm Atomic Vapor
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Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

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在热力学上微不足道的系统中,在零度以外的温度下进行量子记忆.

Yifan Hong1, Jinkang Guo1, Andrew Lucas2

  • 1Department of Physics and Center for Theory of Quantum Matter, University of Colorado, Boulder, CO, USA.

Nature communications
|January 2, 2025
PubMed
概括

一些经典和量子代码提供了无热力学相位转换的被动错误校正. 在临界温度以下,吉布斯采样变得缓慢,使有限电路的容错量子错误校正成为可能.

科学领域:

  • 量子信息科学 量子信息科学
  • 统计力学 统计力学
  • 错误纠正代码 错误纠正代码

背景情况:

  • 被动错误纠正利用本地信息进行信息保护.
  • 经典和量子模型通常依赖于热力学相位过渡来纠错.
  • 低密度平价检查 (LDPC) 代码在经典和量子信息理论中至关重要.

研究的目的:

  • 研究古典和量子低密度平价性检查代码中的被动错误校正.
  • 探索这些代码中没有热力学相变的缺失.
  • 确定实现被动量子错误纠正的替代机制.

主要方法:

  • 分析经典和量子低密度平价性检查代码.
  • 调查当地的吉布斯采样动态.
  • 研究突破ergodicity的动态转换和混合时间.
  • 探索有限深度电路的实现.

主要成果:

  • 某些LDPC代码在零度以外的温度下缺乏热力学相变.
  • 这些代码表现出Gibbs采样时间偏离于临界温度以下的动态过渡.
  • 缓慢的吉布斯采样可以实现容错的被动量子错误校正.

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Gradient Echo Quantum Memory in Warm Atomic Vapor
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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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  • 拟议的策略适用于无测量量子误差校正.
  • 结论:

    • 被动量子误差校正可以在没有热力学相位过渡的情况下实现.
    • 破坏ergodicity的动态转换为错误保护提供了一条新的路线.
    • 这种方法比传统的积极反方法提供了潜在的实验优势.