半导体探测器中的电荷扩散和排斥
Manuel Ballester1, Jaromir Kaspar2, Francesc Massanés2
1Department of Computer Sciences, Northwestern University, Evanston, IL 60208, USA.
Sensors (Basel, Switzerland)
|November 27, 2024
概括
这项研究引入了一种新的蒙特卡洛方法来模拟半导体探测器,通过包括电荷扩散和库伦排斥来提高准确性. 这增强了数字双胞胎模型,用于更好的高能传感应用.
科学领域:
- 物理 物理学 物理
- 材料科学 材料科学 材料科学
- 工程 工程师 工程师 工程师
背景情况:
- 半导体探测器对于高能传感 (X/γ射线) 在天文学,医学成像和安全等各个领域至关重要.
- 精确的探测器表征对于通过数字双胞胎优化成像系统设计和性能至关重要.
- 现有的模拟通常由于复杂性而省略电荷扩散和库伦反射,限制了保真度.
研究的目的:
- 评估现有的模拟半导体探测器中电荷扩散和库伦反射的方法.
- 提出和验证一种新的蒙特卡洛技术,用于高保真探测器模拟.
- 为了实现更现实的性能预测,用于先进的传感应用.
主要方法:
- 已经确定的模拟方法的评估 (加蒂,1987;贝诺伊特和哈梅尔,2009).
- 开发一种新的蒙特卡洛模拟技术.
- 在模拟模型中包括电荷扩散和库伦反推现象.
主要成果:
- 新的蒙特卡洛方法与现有方法相比,提供了更高的准确性.
- 拟议的技术考虑了电荷扩散和库伦反射效应.
- 新方法在实际计算约束范围内实现了现实的性能预测.
结论:
- 准确模拟半导体探测器需要结合电荷扩散和库伦反射.
- 新的蒙特卡洛技术为探测器表征提供了更精确的方法.
- 这一进步支持了用于高能传感系统的改进数字双胞胎的开发.
相关概念视频
Carrier Transport
405
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:
405
Metal-Semiconductor Junctions
300
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...
300
P-N junction
468
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
468
Biasing of Metal-Semiconductor Junctions
215
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
215
Carrier Generation and Recombination
521
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...
521
Schottky Barrier Diode
297
Schottky barrier diodes are specialized semiconductor devices characterized by their unique construction. This construction involves combining a metal layer with a moderately doped n-type semiconductor material. This combination leads to the formation of a Schottky barrier, a pivotal element that defines the diode's operational characteristics. The core functionality of Schottky barrier diodes is their capacity to allow current to flow in only one direction due to their distinctive...
297


