- 必威体育下载

姓名
邮箱
手机号码
标题
留言内容
验证码

Abstract

This paper aims to analyze the failure mechanism of the two-stage PIN limiter after having been injected by a microwave pulse. A two-stage PIN limiter model with high computational efficiency and accuracy is built by using the method of field-circuit collaborative simulation. Using this model, the temperature change of the PIN diodes during the injection of microwave pulse is simulated. The melting temperature of the PIN diode is selected as the failure criterion of the PIN limiter. The time and energy required for the failure of the PIN limiter under injection of microwave pulses with different frequencies and amplitudes are simulated. Furthermore, the mechanisms that trigger off these effects are analyzed. The relationship between the microwave pulse parameters and the PIN limiter failure time is summarized by using an empirical formula. According to the simulation results, the temperature change of the second-stage PIN diode is relatively small compared with that of the first-stage. During the injection of the microwave pulse, the failure time and energy consumption of limiter show a certain regularity with the variation of microwave pulse amplitude and frequency, and this work discusses this regularity from the following three aspects. Firstly, the failure time and energy consumption decrease in a similar trend with frequency increasing. And with the increase in signal amplitude, the failure time and energy consumption tend to stabilize. Secondly, the increase in the signal amplitude leads failure time to decrease, which is similar to the relationship between failure time and the signal frequency mentioned before. But as the signal’s amplitude increases, the energy consumption first increases and then decreases slightly when the amplitude reaches about 900 V. Based on the theoretical analysis and the physical image of the two-stage PIN limiter, the reasons for these effects can be explained as the changes in the I-region's impedance and heat distribution change caused by electric field changes. Thirdly, the failure time and energy consumption show different sensitivities to different parameters of the microwave pulse. The signal frequency change has greater influence on the energy consumption than the signal amplitude change, while the amplitude change can exert a greater influence on the failure time than the frequency change.

Keywords:

Authors and contacts

Corresponding author:Zhang Yang,16103271g@connect.polyu.hk

Funds:Project supported by the Natural Science Foundation of Hunan Province, China (Grant No. 2023JJ40675), the Science and Technology Innovation Plan of Hunan Province, China (Grant No. 2021RC2065), and the Scientific Research Plan of National University of Defense Technology, China (Grant No. ZK22-42).

FullText HTML: translate this paragraph

References

[1]
[2]
[3]
[4]
[5]
[6]
[7]
[8]
[9]
[10]
[11]
[12]
[13]
[14]
[15]
[16]
[17]
[18]
[19]
[20]
[21]
[22]
[23]
[24]
[25]

Cited By

DownLoad: Full-Size Img PowerPoint

参数	电子(P)	空穴(B)
${\mu _{\max }}$/(${\text{c}}{{\text{m}}^{2}} {\cdot} {{\text{V}}^{{{ - 1}}}} {\cdot} {{\text{s}}^{{{ - 1}}}}$)	1441	470.5
$c$	–0.11	0
$\gamma $	2.45	2.16
${\mu _{0 d}}$/(${\text{c}}{{\text{m}}^{2}} {\cdot} {{\text{V}}^{{{ - 1}}}} {\cdot} {{\text{s}}^{{{ - 1}}}}$)	62.2${T_n}^{{{ - }}{\gamma _{{0}d}}}$	90.0$ {T_n}^{{{ - }}{\gamma _{{0}d}}} $
${\gamma _{0 d}}$	0.7	1.3
${\mu _{1 d}}$/(${\text{c}}{{\text{m}}^{2}} {\cdot} {{\text{V}}^{{{ - 1}}}} {\cdot} {{\text{s}}^{{{ - 1}}}}$)	48.6${T_n}^{{{ - }}{\gamma _{{1}d}}}$	28.2${T_n}^{{{ - }}{\gamma _{{1}d}}}$
${\gamma _{1 d}}$	0.7	2.0
${\mu _{1 a}}$/(${\text{c}}{{\text{m}}^{2}} {\cdot} {{\text{V}}^{{{ - 1}}}} {\cdot} {{\text{s}}^{{{ - 1}}}}$)	73.5${T_n}^{{{ - }}{\gamma _{{1}a}}}$	28.2${T_n}^{{{ - }}{\gamma _{{1}a}}}$
${\gamma _{1 a}}$	1.25	0.8
${C_{r1}}$/cm^–3	$8.5 \times {10^{16}} {T_n}^{{\gamma _{r1}}}$	$1.3 \times {10^{18}} {T_n}^{{\gamma _{r{1}}}}$
${\gamma _{r1}}$	3.65	2.2
${C_{r2}}$/cm^–3	$1.22 \times {10^{17}} {T_n}^{{\gamma _{r2}}}$	$2.45 \times {10^{17}} {T_n}^{{\gamma _{r{2}}}}$
${\gamma _{r2}}$	2.65	3.1
${C_{s1}}$/cm^–3	$4.0 \times {10^{20}} {T_n}^{{\gamma _{s{1}}}}$	$1.1 \times {10^{18}} {T_n}^{{\gamma _{s{1}}}}$
${\gamma _{s1}}$	0	6.2
${C_{s2}}$/(10²⁰cm^–3)	$7.0$	$6.1$
$\alpha $	0.68	0.77
$\beta $	0.72	0.719
${\mu _{0 a}}$/(${\text{c}}{{\text{m}}^{2}} {\cdot} {{\text{V}}^{{{ - 1}}}} {\cdot} {{\text{s}}^{{{ - 1}}}}$)	132.0${T_n}^{{{ - }}{\gamma _{{0}a}}}$	44.0${T_n}^{{{ - }}{\gamma _{{0}a}}}$
${\gamma _{0 a}}$	1.3	0.7

DownLoad: CSV

参数	值
$D$/(cm^–1·V^–1·s^–1)	$1.04 \times {10^{21}}$
$F$/cm^–2	$7.452 \times {10^{13}}$

DownLoad: CSV

参数	电子	空穴
${v_{{\text{sat, 0}}}}$/(10⁷cm·s^–1)	$1.07$	$0.837$
$ {v_{{\text{sat}}, \exp }} $	0.87	0.52

DownLoad: CSV

参数	电子	空穴
${\beta _0}$	1.109	1.213
${\beta _{\exp }}$	0.66	0.17

DownLoad: CSV

参数	电子	空穴
${\tau _{\min }}$/s	0	0
${\tau _{\max }}$/μs	$10$	$3$
${\tau _0}$/μs	$10$	$3$
${N_{{\text{ref}}}}$/(10¹⁶cm^–3)	$1$	$1$
$\gamma $	1	1
${T_{\text{α }}}$	–1.5	–1.5
${E_{{\text{trap}}}}$/eV	0	0

DownLoad: CSV

参数	电子	空穴
${A_{\text{A}}}$/(10^–32cm⁶·s^–1)	$6.7$	$7.2$
${B_{\text{A}}}$/(10^–33cm⁶·s^–1)	$245$	$4.5$
${C_{\text{A}}}$/(10^–33cm⁶·s^–1)	$ - 2.2$	$2.63$
$H$	3.46667	8.25688
${N_0}$/(10¹⁸cm^–3)	$1$	$1$

DownLoad: CSV

参数	电子	空穴
${a_0}$/V	4.65403	2.26018
${a_1}$/mV	$ - 8.76031$	13.4001
${a_2}$/μV	$13.4037$	$ - 5.87724$
${a_3}$/nV	$ - 2.75108$	$ - 1.14021$
${b_0}$/V	–0.128302	0.058547
${b_1}$/(10^–4V)	$44.5552$	$ - 1.95755$
${b_2}$/(10^–7V)	$ - 108.66$	$2.44357$
${b_3}$/(10^–10V)	$92.3119$	$ - 1.33202$
${b_4}$/(10^–14V)	$ - 182.482$	$2.68082$
${b_5}$/V	$ - 4.82689 \times {10^{ - 15}}$	0
${b_6}$/V	$1.09402 \times {10^{ - 17}}$	0
${b_7}$/V	$ - 1.24961 \times {10^{ - 20}}$	0
${b_8}$/V	$7.55584 \times {10^{ - 24}}$	0
${b_9}$/V	$ - 2.28615 \times {10^{ - 27}}$	0
${b_{10}}$/V	$2.73344 \times {10^{ - 31}}$	0
${c_0}$/(10³V·cm^–1)	$7.76221$	$19.5399$
${c_1}$/(V·cm^–1)	25.18888	–104.441
${c_2}$/(V·cm^–1)	$ - 1.37417 \times {10^{ - 3}}$	0.498768
${c_3}$/(V·cm^–1)	$1.59525 \times {10^{ - 4}}$	0
${d_0}$/(10⁵V·cm^–1)	$7.10481$	$20.7712$
${d_1}$/(10³V·cm^–1)	$3.98594$	0.993153
${d_2}$/(V·cm^–1)	–7.19956	7.77769
${d_3}$/(V·cm^–1)	$6.96431 \times {10^{ - 3}}$	0

DownLoad: CSV

[1]
[2]
[3]
[4]
[5]
[6]
[7]
[8]
[9]
[10]
[11]
[12]
[13]
[14]
[15]
[16]
[17]
[18]
[19]
[20]
[21]
[22]
[23]
[24]
[25]

[1]	He Yu, Chen Wei-Bin, Hong Bin, Huang Wen-Tao, Zhang Kun, Chen Lei, Feng Xue-Qiang, Li Bo, Liu Guo, Sun Xiao-Han, Zhao Meng, Zhang Yue.Significant role of thermal effects in current-induced exchange bias field switching at antiferromagnet/ferromagnet interface. Acta Physica Sinica, 2024, 73(2): 027501.doi:10.7498/aps.73.20231374
[2]	Lian Tian-Hong, Dou Yi-Qun, Zhou Lei, Liu Yun, Kou Ke, Jiao Ming-Xing.Modal structure of high power thin-disk vortex laser under thermal effect. Acta Physica Sinica, 2024, 73(16): 164206.doi:10.7498/aps.73.20240757
[3]	Zhang Mei-Mei, Wu Yi-Yun, Yu Jie, Tu Juan, Zhang Dong.Effect of pulse duty ratio on temperature rise induced by focused ultrasound combined with magnetic microbubbles. Acta Physica Sinica, 2023, 72(8): 084301.doi:10.7498/aps.72.20230068
[4]	.Biological effects of terahertz waves. Acta Physica Sinica, 2022, (): .doi:10.7498/aps.71.20211996
[5]	Peng Xiao-Yu, Zhou Huan.Biological effects of terahertz waves. Acta Physica Sinica, 2021, 70(24): 240701.doi:10.7498/aps.70.20211996
[6]	Xia Qing-Gan, Xiao Wen-Bo, Li Jun-Hua, Jin Xin, Ye Guo-Ming, Wu Hua-Ming, Ma Guo-Hong.Optimization of thermal performance of cladding power stripper in fiber laser. Acta Physica Sinica, 2020, 69(1): 014204.doi:10.7498/aps.69.20191093
[7]	Zhou Zi-Chao, Wang Xiao-Lin, Tao Ru-Mao, Zhang Han-Wei, Su Rong-Tao, Zhou Pu, Xu Xiao-Jun.Theoretical study of the temperature distribution in high power gain fiber of gradient doping. Acta Physica Sinica, 2016, 65(10): 104204.doi:10.7498/aps.65.104204
[8]	Chen Gui-Bo, Zhang Jia-Jia, Wang Chao-Qun, Bi Juan.A parameter inversion method of film based on thermal effects induced by laser irradiation. Acta Physica Sinica, 2016, 65(12): 124401.doi:10.7498/aps.65.124401
[9]	Huang Wen-Fa, Li Xue-Chun, Wang Jiang-Feng, Lu Xing-Hua, Zhang Yu-Qi, Fan Wei, Lin Zun-Qi.Theoretical and experimental investigations on wavefront distortion and thermal-stress induced birefringence in a laser diode pumped helium gas-cooled multislab Nd:glass laser amplifier. Acta Physica Sinica, 2015, 64(8): 087801.doi:10.7498/aps.64.087801
[10]	Tao Ru-Mao, Zhou Pu, Wang Xiao-Lin, Si Lei, Liu Ze-Jin.Experimental study on mode instability in high power all-fiber master oscillator power amplifer fiber lasers. Acta Physica Sinica, 2014, 63(8): 085202.doi:10.7498/aps.63.085202
[11]	Zhou Ying, Dai Yu, Yao Shu-Na, Liu Jun, Chen Jia-Bin, Chen Shu-Fen, Xin Jian-Guo.Three-dimensional thermal effects of the diode-pumped Nd:YVO4 slab. Acta Physica Sinica, 2013, 62(2): 024210.doi:10.7498/aps.62.024210
[12]	Hu Miao, Zhang Hui, Zhang Fei, Liu Chen-Xi, Xu Guo-Rui, Deng Jing, Huang Qian-Feng.Thermally induced frequency difference characteristics of dual-frequency microchip laser used optical generation millimeter-wave. Acta Physica Sinica, 2013, 62(20): 204205.doi:10.7498/aps.62.204205
[13]	Liu Hai-Qiang, Guo Zhen, Wang Shi-Yu, Lin Lin, Guo Long-Cheng, Li Bing-Bin, Cai De-Fang.Research on thermal contact conductance between crystal rod and heat sink in LD end-pumped solid-state laser. Acta Physica Sinica, 2011, 60(1): 014212.doi:10.7498/aps.60.014212
[14]	Liu Quan-Xi, Zhong Ming.Analysis on thermal effect of laser-diode array end-pumped composite rod laser by finite element method. Acta Physica Sinica, 2010, 59(12): 8535-8541.doi:10.7498/aps.59.8535
[15]	Wang Jian, Li Ying-Hong, Cheng Bang-Qin, Su Chang-Bing, Song Hui-Min, Wu Yun.The mechanism investigation on shock wave controlled by plasma aerodynamic actuation. Acta Physica Sinica, 2009, 58(8): 5513-5519.doi:10.7498/aps.58.5513
[16]	Dong Hao, Ren Min, Zhang Lei, Deng Ning, Chen Pei-Yi.Thermal effect in current induced magnetic switching. Acta Physica Sinica, 2009, 58(10): 7176-7182.doi:10.7498/aps.58.7176
[17]	Song Xiao-Lu, Guo Zhen, Li Bing-Bin, Wang Shi-Yu, Cai De-Fang, Wen Jian-Guo.Time-varying thermal effect of laser crystal in pulsed diode laser side-pumped Nd∶YAG laser. Acta Physica Sinica, 2009, 58(3): 1700-1708.doi:10.7498/aps.58.1700
[18]	Wang Li-Shi, Pan Chun-Xu, Cai Qi-Zhou, Wei Bo-Kang.Study of the heat effect of single steady-state microdischarge during plasma electrolytic oxidation. Acta Physica Sinica, 2007, 56(9): 5341-5346.doi:10.7498/aps.56.5341
[19]	Wu Jian.Analytical thermal model and characterization of lateral thermal effects in AlInGaAs vertical-cavity top-emitting lasers. Acta Physica Sinica, 2006, 55(11): 5848-5854.doi:10.7498/aps.55.5848
[20]	Ji Xiao-Ling, Tao Xiang-Yang, Lü Bai-Da.The influence of thermal effects in a beam control system and spherical aberration on the laser beam quality. Acta Physica Sinica, 2004, 53(3): 952-960.doi:10.7498/aps.53.952

Catalog

Vol. 73, Issue 6 - 2024-03-20

Metrics

Abstract views:1212
PDF Downloads:36
Cited By:0

Search

Article