-p-i-n核辐射探测器的同等电路
Ahmet Saymbetov1, Ramizulla Muminov2, Zhang Jing1
1Al-Farabi Kazakh National University, Almaty, Kazakhstan.
Scientific reports
|August 2, 2023
概括
这项研究引入了-p-i-n核辐射探测器的同等电路,使得精确的α-衰变频谱模拟成为可能. 模型 模型的模型
科学领域:
- 核物理学 核物理 核物理
- 半导体设备物理学 半导体设备物理
背景情况:
- p-i-n探测器对于核辐射研究和X射线光谱学至关重要.
- 它们在正常条件下的运行增加了对它们发展的兴趣.
研究的目的:
- 为-p-i-n核辐射探测器提出一个同等的电路.
- 用实验数据模拟和验证探测器的性能.
主要方法:
- 使用肖克利和电报方程开发了一个相当的电路.
- 通过多重回归分析确定电路参数.
- 在 MATLAB Simulink 中模拟的振幅频率和相频率特征.
- 使用蒙特卡洛方法进行α衰变频谱分析.
主要成果:
- 获得了拟议探测器模型的振幅频率和相频率特征.
- 产生了,和美洲同位素的α-衰变光谱.
- 与现有实验数据对比验证的模拟结果.
结论:
- 拟议的同等电路准确地模拟了-p-i-n核辐射探测器.
- 模拟方法提供可靠的α-衰变光谱,与实验发现保持一致.
更多相关视频
14:19A Basic Positron Emission Tomography System Constructed to Locate a Radioactive Source in a Bi-dimensional Space
Published on: February 1, 2016
8.6K
06:28Visualization of Low-Level Gamma Radiation Sources Using a Low-Cost, High-Sensitivity, Omnidirectional Compton Camera
Published on: January 30, 2020
12.6K
相关概念视频
P-N junction
578
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...
578
Biasing of P-N Junction
602
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
602
Biological Effects of Radiation
15.5K
All radioactive nuclides emit high-energy particles or electromagnetic waves. When this radiation encounters living cells, it can cause heating, break chemical bonds, or ionize molecules. The most serious biological damage results when these radioactive emissions fragment or ionize molecules. For example, α and β particles emitted from nuclear decay reactions possess much higher energies than ordinary chemical bond energies. When these particles strike and penetrate matter, they...
15.5K
Norton Equivalent Circuits
415
Norton's theorem is a fundamental concept in the field of electrical engineering that allows for the simplification of complex AC circuits. The theorem states that any two-terminal linear network can be replaced with an equivalent circuit that consists of an impedance, which is parallel with a constant current source. Figure 1 shows the AC circuit portioned into two parts: Circuit A and Circuit B, while Figure 2 depicts the circuit obtained by replacing Circuit A by its Norton equivalent...
415
Diode: Forward bias
1.1K
In semiconductor devices, diodes play a crucial role in directing current flow, and its operation is primarily categorized into forward bias and reverse bias. A diode is said to be forward-biased when its p-type region is connected to the positive terminal of a battery and its n-type region is linked to the negative terminal. This configuration reduces the potential barrier within the diode, allowing current to flow easily from the p to the n-type region.
The behavior of a diode in forward bias...
The behavior of a diode in forward bias...
1.1K
Gas Chromatography: Types of Detectors-II
418
In gas chromatography, different detectors are employed to meet specific analytical needs. These detectors are often categorized based on their detection mechanisms and the types of compounds they are best suited to analyze. Thermal Conductivity Detectors (TCD), Flame Ionization Detectors (FID), and Electron Capture Detectors (ECD) represent common categories, each with unique operating principles and applications. However, beyond these, several other detectors are designed for more specialized...
418
