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Atomic Nuclei: Nuclear Relaxation Processes01:23

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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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Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If...
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Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
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The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
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The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
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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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雪崩中的多体共振 多体定位的不稳定性

Hyunsoo Ha1, Alan Morningstar1,2, David A Huse1

  • 1Department of Physics, Princeton University, Princeton, New Jersey 08544, USA.

Physical review letters
|July 7, 2023
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概括
此摘要是机器生成的。

多体局部系统避免了热平衡. 由多体共振驱动的雪崩可以通过这些系统传播热化,揭示了一个关键的连接.

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科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 量子多体系统是一个量子多体系统.

背景情况:

  • 多体局部化 (MBL) 系统表现出独特的非平衡动态.
  • 这些系统,尽管有相互作用,但由于局部化而抵抗热化.
  • 一个"雪崩"的不稳定性可以触发MBL系统中的热化.

研究的目的:

  • 调查MBL系统中雪崩传播的机制.
  • 探索多体共振在MBL热化中的作用.
  • 为了确定共振与雪崩现象之间的联系.

主要方法:

  • 一维MBL系统的数值模拟.
  • 模拟雪崩通过合到无限温度浴来扩散.
  • 对多体共振和近共振固有状态的分析.

主要成果:

  • 雪崩的传播主要是由强大的多体共振介导的.
  • 这些共振发生在封闭系统的罕见,接近共振的固有状态之间.
  • 确定了多体共振与雪崩动态之间的直接联系.

结论:

  • 多体共振对于MBL系统中热化的传播至关重要.
  • 了解共振可以了解局部化的崩.
  • 这项研究阐明了管理MBL系统行为的基本机制.