在半导体设备运输模拟中对自相一致的施罗丁格-波松方程的收进行数值调查
Junyan Zhu1,2,3, Jiang Cao4, Chen Song5
1Institute of Microelectronics of the Chinese Academy of Sciences, Beijing, 100029, People's Republic of China.
Nanotechnology
|May 20, 2024
概括
这项研究提高了模拟纳米半导体设备的非平衡格林函数 (NEGF) 方法的稳定性. 非线性波桑方程和先进的预解决技术改善了碳纳米管场效应晶体管 (CNTFET) 的融合.
科学领域:
- 在纳米级半导体设备中的量子传输.
- 计算物理和设备模拟.
背景情况:
- 模拟纳米级半导体设备需要解决施罗丁格-波松方程.
- 非平衡格林函数 (NEGF) 方法是标准的,但在计算上昂贵,并面临与波桑方程的融合问题.
研究的目的:
- 调查NEGF方法与Poisson方程的不同形式相结合时的稳定性.
- 在各种兴奋剂条件下评估碳纳米管场效应晶体管 (CNTFET) 的模拟性能.
主要方法:
- 将NEGF方法与线性,分析性非线性和数值非线性Poisson方程结合起来.
- 通过静电兴奋剂和离子植入兴奋剂模拟CNTFETs.
- 运用拉普拉斯方程的解决方案和断片猜测来实施潜在的预解决策略.
主要成果:
- 与线性方程相比,非线性波桑方程公式表现出优越的稳定性和性能.
- 数值非线性波桑方程提供了最好的稳定性,特别是在高偏差和离子植入兴奋剂下.
- 先进的预解决方法显著减少了融合所需的代次数.
结论:
- 非线性Poisson解决器提高了纳米尺度设备模拟的NEGF方法的稳定性.
- 数字非线性方法对于挑战诸如离子植入等兴奋剂场景来说是强大的.
- 优化的潜在预解决加速了趋同,使得NEGF模拟对CNTFET更实用.
相关概念视频
Carrier Transport
430
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:
430
Poisson's And Laplace's Equation
2.8K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
2.8K
Carrier Generation and Recombination
565
Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
565
Metal-Semiconductor Junctions
343
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
343
Fermi Level Dynamics
243
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...
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...
243
Types of Semiconductors
587
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
587


