宏观大厅电流响应在无限扩展的间隙费米子系统中的近线性
Marius Wesle1, Giovann Marcelli2, Tadahiro Miyao3
1Fachbereich Mathematik, Eberhard Karls Universität Tübingen, Auf der Morgenstelle 10, 72076 Tübingen, Germany.
概括
这项研究表明,拓绝缘体是优秀的绝缘体,纵向电流随着电场强度的增加而呈指数级消失. 然而,霍尔导电性仍然强大且可测量,提供了一种精确的方法来表征这些材料.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 拓学物质是一个拓学物质.
- 量子运输现象 量子运输现象
背景情况:
- 拓绝缘体是具有独特电子特性的材料,在散装中起到绝缘体的作用,但在表面是导电的.
- 了解它们对外部电场的反应对于应用和基本物理学至关重要.
- 以前的研究往往侧重于电压下降,而不是宏观系统上的恒定电场.
研究的目的:
- 为了研究空隙拓绝缘体对恒定的外部电场的电流响应.
- 为了确定这些系统中的纵向和霍尔电流密度.
- 在相互作用的费米子系统中推导霍尔导电性的公式.
主要方法:
- 利用非平衡几乎静止状态的方法.
- 在一个具有短距离相互作用的晶格上分析了一个宏观的,无限扩展的费米子系统.
- 考虑的系统有间隙基本状态和磁转换不变.
主要成果:
- 由恒定的电场引起的纵向电流密度是微小的 (O(ε^∞)).
- 霍尔电流密度在电场强度 (ε) 中是线性的,直至指数级小的校正.
- 在交互系统中推导霍尔导电性的一般化双通换器公式.
结论:
- 该系统在纵向电流方面表现为理想的绝缘体.
- 霍尔导电性 (σ_H) 在间隙相内是恒定的,并且对相互作用具有强度.
- 对于2D系统,霍尔导电性精确地测量了s_H,随着实验方差的消失.
相关概念视频
The Hall Effect
2.7K
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
2.7K
Linear Circuits
486
A linear circuit is characterized by its output having a direct proportionality to its input, adhering to the linearity property, which encompasses the principles of homogeneity (scaling) and additivity. Homogeneity dictates that when the input, also referred to as the excitation, is multiplied by a constant factor, the output, known as the response, is correspondingly scaled by the same constant factor. For instance, if the current is multiplied by a constant 'k,' the voltage likewise...
486
Carrier Transport
571
The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
571
Linear Approximation in Frequency Domain
136
Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
136
Small-Signal Analysis of MOSFET Amplifiers
746
In small-signal analysis, a MOSFET transistor amplifier acts as a linear amplifier when operating in its saturation region. The gate-to-source voltage (VGS) of the MOSFET is the sum of the DC biasing voltage and the small time-varying input signal. This combination sets up the operating point and modulates the drain current (ID) that flows from the drain to the source. When a small AC signal is superimposed on the DC bias voltage at the gate, the instantaneous drain current comprises three...
746
Fermi Level
828
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
828


