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相关概念视频

Fault Types01:18

Fault Types

63
When analyzing a single line-to-ground fault from phase A to ground at a three-phase bus, it is important to consider the fault impedance. This impedance is zero for a bolted fault, equal to the arc impedance for an arcing fault, and represents the total fault impedance for a transmission-line insulator flashover. To derive sequence and phase currents, fault conditions are translated from the phase domain to the sequence domain.
For line-to-line faults occurring between phases B and C, the...
63
Phase Transitions02:31

Phase Transitions

18.7K
Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to...
18.7K
Electrostatic Boundary Conditions in Dielectrics01:27

Electrostatic Boundary Conditions in Dielectrics

1.1K
When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's...
1.1K
Fermi Level Dynamics01:12

Fermi Level Dynamics

216
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.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
216

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缺陷诱导了石墨烯从动态到静态波纹的相位过渡.

Fabian L Thiemann1,2, Camille Scalliet3, Erich A Müller4

  • 1IBM Research Europe, Daresbury WA4 4AD, United Kingdom.

Proceedings of the National Academy of Sciences of the United States of America
|February 28, 2025
PubMed
概括

在二维 (2D) 材料中的缺陷可以将波纹从动态转变为静态,在临界度以上. 这种由缺陷相互作用驱动的过渡使得量身定制的二维材料特性和应用成为可能.

关键词:
缺陷 缺陷 缺陷 缺陷 缺陷石墨烯是一种石墨烯.机器学习潜在的机器学习潜力两个维的材料是二维材料.

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科学领域:

  • 材料科学 材料科学 材料科学
  • 凝聚物质物理学 凝聚物质物理学
  • 计算纳米科学 计算纳米科学

背景情况:

  • 二维 (2D) 材料表现出纳米级的动态波纹,影响其物理和化学特性.
  • 水晶格子缺陷对于定制二维材料的形态和行为至关重要.
  • 在二维材料中,缺陷与波纹动态之间的关系需要进行更深入的研究.

研究的目的:

  • 综合调查缺陷对二维材料波纹动态的影响.
  • 在有缺陷的二维材料中阐明从动态到静态波纹的过渡机制.
  • 建立设计具有可控波纹特性的二维材料的原则.

主要方法:

  • 利用机器学习驱动的分子动力学模拟来进行原子分辨率分析.
  • 研究了具有不同缺陷度的独立石墨烯板.
  • 分析了缺陷之间的弹性相互作用作为波纹动态的驱动力.

主要成果:

  • 确定了一个关键缺陷度,触发了石墨烯从动态到静态的过渡.
  • 揭示了缺陷之间的弹性相互作用支配了这种动态到静态的过渡.
  • 证明相互作用强度因缺陷类型而异,提供了统一的原则.

结论:

  • 缺陷度和类型批判性地控制2D材料中的波纹动态.
  • 这些发现合理化了在有缺陷的二维材料中的实验观测.
  • 开辟了设计具有可调节性质的新型基于混乱的催化和接口二维材料的途径.