The energy deposition and electrothermal behavior of SiC metal-oxide-semiconductor field-effect transistor(MOSFET)under heavy ion radiation are investigated based on Monte Carlo method and TCAD numerical simulation.Th...The energy deposition and electrothermal behavior of SiC metal-oxide-semiconductor field-effect transistor(MOSFET)under heavy ion radiation are investigated based on Monte Carlo method and TCAD numerical simulation.The Monte Carlo simulation results show that the density of heavy ion-induced energy deposition is the largest in the center of the heavy ion track.The time for energy deposition in SiC is on the order of picoseconds.The TCAD is used to simulate the single event burnout(SEB)sensitivity of SiC MOSFET at four representative incident positions and four incident depths.When heavy ions strike vertically from SiC MOSFET source electrode,the SiC MOSFET has the shortest SEB time and the lowest SEB voltage with respect to direct strike from the epitaxial layer,strike from the channel,and strike from the body diode region.High current and strong electric field simultaneously appear in the local area of SiC MOSFET,resulting in excessive power dissipation,further leading to excessive high lattice temperature.The gate-source junction area and the substrate-epitaxial layer junction area are both the regions where the SiC lattice temperature first reaches the SEB critical temperature.In the SEB simulation of SiC MOSFET at different incident depths,when the incident depth does not exceed the device's epitaxial layer,the heavy-ion-induced charge deposition is not enough to make lattice temperature reach the SEB critical temperature.展开更多
Experiments and simulation studies on 283 MeV I ion induced single event effects of silicon carbide(SiC) metal–oxide–semiconductor field-effect transistors(MOSFETs) were carried out. When the cumulative irradiation ...Experiments and simulation studies on 283 MeV I ion induced single event effects of silicon carbide(SiC) metal–oxide–semiconductor field-effect transistors(MOSFETs) were carried out. When the cumulative irradiation fluence of the SiC MOSFET reached 5×10^(6)ion·cm^(-2), the drain–gate channel current increased under 200 V drain voltage, the drain–gate channel current and the drain–source channel current increased under 350 V drain voltage. The device occurred single event burnout under 800 V drain voltage, resulting in a complete loss of breakdown voltage. Combined with emission microscope, scanning electron microscope and focused ion beam analysis, the device with increased drain–gate channel current and drain–source channel current was found to have drain–gate channel current leakage point and local source metal melt, and the device with single event burnout was found to have local melting of its gate, source, epitaxial layer and substrate. Combining with Monte Carlo simulation and TCAD electrothermal simulation, it was found that the initial area of single event burnout might occur at the source–gate corner or the substrate–epitaxial interface, electric field and current density both affected the lattice temperature peak. The excessive lattice temperature during the irradiation process appeared at the local source contact, which led to the drain–source channel damage. And the excessive electric field appeared in the gate oxide layer, resulting in drain–gate channel damage.展开更多
The addition of a buffer layer can improve the device＇s secondary breakdown voltage, thus, improving the single event burnout （SEB） threshold voltage. In this paper, an N type linear doping buffer layer is proposed...The addition of a buffer layer can improve the device＇s secondary breakdown voltage, thus, improving the single event burnout （SEB） threshold voltage. In this paper, an N type linear doping buffer layer is proposed. According to quasi-stationary avalanche simulation and heavy ion beam simulation, the results show that an op- timized linear doping buffer layer is critical. As SEB is induced by heavy ions impacting, the electric field of an optimized linear doping buffer device is much lower than that with an optimized constant doping buffer layer at a given buffer layer thickness and the same biasing voltages. Secondary breakdown voltage and the parasitic bipolar turn-on current are much higher than those with the optimized constant doping buffer ~ayer. So the linear buffer layer is more advantageous to improving the device＇s SEB performance.展开更多
提出了一种漂移区具有Nbuffer结构的N型横向扩散金属氧化物半导体(NLDMOS)结构,以提高器件抗单粒子烧毁(single-event burnout,SEB)能力。通过TCAD仿真验证了该结构的电学和抗单粒子特征。在不改变器件性能的前提下,18 V NLDMOS SEB触...提出了一种漂移区具有Nbuffer结构的N型横向扩散金属氧化物半导体(NLDMOS)结构,以提高器件抗单粒子烧毁(single-event burnout,SEB)能力。通过TCAD仿真验证了该结构的电学和抗单粒子特征。在不改变器件性能的前提下,18 V NLDMOS SEB触发电压由22 V提高到32 V,达到理论最大值,即器件雪崩击穿电压。具有Nbuffer结构的NLDMOS器件可以抑制单粒子入射使得器件寄生三极管开启时的峰值电场转移,避免器件雪崩击穿而导致SEB。此外,对于18~60 V NLDMOS器件的SEB加固,Nbuffer结构依然适用。展开更多
The experimental results of single event burnout induced by heavy ions and 252Cf fission fragments in power MOSFET devices have been investigated. It is concluded that the characteristics of single event burnout induc...The experimental results of single event burnout induced by heavy ions and 252Cf fission fragments in power MOSFET devices have been investigated. It is concluded that the characteristics of single event burnout induced by 252Cf fission fragments is consistent to that in heavy ions. The power MOSFET in the ＂turn-off＂ state is more susceptible to single event burnout than it is in the ＂turn-on＂ state. The thresholds of the drain-source voltage for single event burnout induced by 173 MeV bromine ions and ^252Cf fission fragments are close to each other, and the burnout cross section is sensitive to variation of the drain-source voltage above the threshold of single event burnout. In addition, the current waveforms of single event burnouts induced by different sources are similar. Different power MOSFET devices may have different probabilities for the occurrence of single event burnout.展开更多
We present a single-event burnout（SEB） hardened planar power MOSFET with partially widened trench sources by three-dimensional（3 D） numerical simulation. The advantage of the proposed structure is that the work of...We present a single-event burnout（SEB） hardened planar power MOSFET with partially widened trench sources by three-dimensional（3 D） numerical simulation. The advantage of the proposed structure is that the work of the parasitic bipolar transistor inherited in the power MOSFET is suppressed effectively due to the elimination of the most sensitive region（P-well region below the N＋ source）. The simulation result shows that the proposed structure can enhance the SEB survivability significantly. The critical value of linear energy transfer（LET）,which indicates the maximum deposited energy on the device without SEB behavior, increases from 0.06 to0.7 p C/μm. The SEB threshold voltage increases to 120 V, which is 80% of the rated breakdown voltage. Meanwhile, the main parameter characteristics of the proposed structure remain similar with those of the conventional planar structure. Therefore, this structure offers a potential optimization path to planar power MOSFET with high SEB survivability for space and atmospheric applications.展开更多
随着空间技术和核技术的快速发展,越来越多的先进半导体器件应用于军事和航天电子系统。利用TCAD模拟仿真软件,设计一种抗辐射加固30 V N型LDMOS器件结构,开展LDMOS器件的单粒子烧毁效应(SEB)研究。诱发单粒子烧毁效应源于N型MOSFET器...随着空间技术和核技术的快速发展,越来越多的先进半导体器件应用于军事和航天电子系统。利用TCAD模拟仿真软件,设计一种抗辐射加固30 V N型LDMOS器件结构,开展LDMOS器件的单粒子烧毁效应(SEB)研究。诱发单粒子烧毁效应源于N型MOSFET器件中的寄生NPN三极管在光电流作用下开启并维持工作。从版图设计和工艺设计角度考虑提高器件的抗单粒子烧毁能力的因素,包括LDD浓度、LDD长度、P型埋层结构、工作电压和LET能量等。通过抗辐射设计和工艺加固,获得击穿电压34.6 V、导通电阻只有10.04 mΩ·mm^2的LDMOS器件,同时在工作电压30 V时,器件的抗单粒子烧毁能力达到100 MeV·cm^2/mg。展开更多
针对空间应用,开展SiC MOSFET单粒子效应试验研究。在加速器上用重离子辐照1200 V SiC MOSFET,离子线性能量传输(LET)在0.26~118 MeV·cm^(2)/mg之间,辐照中被试器件加50~600 V静态漏源偏置电压、栅源短接,实时测量电特性,进行辐照...针对空间应用,开展SiC MOSFET单粒子效应试验研究。在加速器上用重离子辐照1200 V SiC MOSFET,离子线性能量传输(LET)在0.26~118 MeV·cm^(2)/mg之间,辐照中被试器件加50~600 V静态漏源偏置电压、栅源短接,实时测量电特性,进行辐照后栅应力(PIGS)测试。试验结果发现,50~100 V偏置电压下,离子引起瞬态电流,PIGS测试栅失效。分析认为离子引起栅氧化物潜在损伤,PIGS测试过程中,潜在损伤进一步退化导致栅失效。氧化物潜在损伤不仅与辐照偏置电压有关,还与入射离子LET和注量有关。PIGS测试需要的栅应力时间与潜在损伤程度有关,可超过300 s。并给出了电荷累积损伤模型。模型进行SiC MOSFET单粒子效应评估时,应考虑离子引起栅氧化物潜在损伤的影响,需根据轨道和任务周期确定试验离子注量,根据应用情况确定辐照偏置电压,并评估确定PIGS测试栅应力时间。展开更多
基金the National Natural Science Foundation of China(Grant Nos.11875229 and 12075065).
文摘The energy deposition and electrothermal behavior of SiC metal-oxide-semiconductor field-effect transistor(MOSFET)under heavy ion radiation are investigated based on Monte Carlo method and TCAD numerical simulation.The Monte Carlo simulation results show that the density of heavy ion-induced energy deposition is the largest in the center of the heavy ion track.The time for energy deposition in SiC is on the order of picoseconds.The TCAD is used to simulate the single event burnout(SEB)sensitivity of SiC MOSFET at four representative incident positions and four incident depths.When heavy ions strike vertically from SiC MOSFET source electrode,the SiC MOSFET has the shortest SEB time and the lowest SEB voltage with respect to direct strike from the epitaxial layer,strike from the channel,and strike from the body diode region.High current and strong electric field simultaneously appear in the local area of SiC MOSFET,resulting in excessive power dissipation,further leading to excessive high lattice temperature.The gate-source junction area and the substrate-epitaxial layer junction area are both the regions where the SiC lattice temperature first reaches the SEB critical temperature.In the SEB simulation of SiC MOSFET at different incident depths,when the incident depth does not exceed the device's epitaxial layer,the heavy-ion-induced charge deposition is not enough to make lattice temperature reach the SEB critical temperature.
基金supported by the National Natural Science Foundation of China (Grant No. 12075065)。
文摘Experiments and simulation studies on 283 MeV I ion induced single event effects of silicon carbide(SiC) metal–oxide–semiconductor field-effect transistors(MOSFETs) were carried out. When the cumulative irradiation fluence of the SiC MOSFET reached 5×10^(6)ion·cm^(-2), the drain–gate channel current increased under 200 V drain voltage, the drain–gate channel current and the drain–source channel current increased under 350 V drain voltage. The device occurred single event burnout under 800 V drain voltage, resulting in a complete loss of breakdown voltage. Combined with emission microscope, scanning electron microscope and focused ion beam analysis, the device with increased drain–gate channel current and drain–source channel current was found to have drain–gate channel current leakage point and local source metal melt, and the device with single event burnout was found to have local melting of its gate, source, epitaxial layer and substrate. Combining with Monte Carlo simulation and TCAD electrothermal simulation, it was found that the initial area of single event burnout might occur at the source–gate corner or the substrate–epitaxial interface, electric field and current density both affected the lattice temperature peak. The excessive lattice temperature during the irradiation process appeared at the local source contact, which led to the drain–source channel damage. And the excessive electric field appeared in the gate oxide layer, resulting in drain–gate channel damage.
基金supported by the National Natural Science Foundation of China(No.61176071)the Doctoral Fund of Ministry of Education of China(No.20111103120016)the Science and Technology Program of State Grid Corporation of China(No.SGRI-WD-71-13-006)
文摘The addition of a buffer layer can improve the device＇s secondary breakdown voltage, thus, improving the single event burnout （SEB） threshold voltage. In this paper, an N type linear doping buffer layer is proposed. According to quasi-stationary avalanche simulation and heavy ion beam simulation, the results show that an op- timized linear doping buffer layer is critical. As SEB is induced by heavy ions impacting, the electric field of an optimized linear doping buffer device is much lower than that with an optimized constant doping buffer layer at a given buffer layer thickness and the same biasing voltages. Secondary breakdown voltage and the parasitic bipolar turn-on current are much higher than those with the optimized constant doping buffer ~ayer. So the linear buffer layer is more advantageous to improving the device＇s SEB performance.
文摘提出了一种漂移区具有Nbuffer结构的N型横向扩散金属氧化物半导体(NLDMOS)结构,以提高器件抗单粒子烧毁(single-event burnout,SEB)能力。通过TCAD仿真验证了该结构的电学和抗单粒子特征。在不改变器件性能的前提下,18 V NLDMOS SEB触发电压由22 V提高到32 V,达到理论最大值,即器件雪崩击穿电压。具有Nbuffer结构的NLDMOS器件可以抑制单粒子入射使得器件寄生三极管开启时的峰值电场转移,避免器件雪崩击穿而导致SEB。此外,对于18~60 V NLDMOS器件的SEB加固,Nbuffer结构依然适用。
文摘The experimental results of single event burnout induced by heavy ions and 252Cf fission fragments in power MOSFET devices have been investigated. It is concluded that the characteristics of single event burnout induced by 252Cf fission fragments is consistent to that in heavy ions. The power MOSFET in the ＂turn-off＂ state is more susceptible to single event burnout than it is in the ＂turn-on＂ state. The thresholds of the drain-source voltage for single event burnout induced by 173 MeV bromine ions and ^252Cf fission fragments are close to each other, and the burnout cross section is sensitive to variation of the drain-source voltage above the threshold of single event burnout. In addition, the current waveforms of single event burnouts induced by different sources are similar. Different power MOSFET devices may have different probabilities for the occurrence of single event burnout.
基金Project supported by the National Natural Science Foundation of China(Nos.61404161,61404068,61404169)
文摘We present a single-event burnout（SEB） hardened planar power MOSFET with partially widened trench sources by three-dimensional（3 D） numerical simulation. The advantage of the proposed structure is that the work of the parasitic bipolar transistor inherited in the power MOSFET is suppressed effectively due to the elimination of the most sensitive region（P-well region below the N＋ source）. The simulation result shows that the proposed structure can enhance the SEB survivability significantly. The critical value of linear energy transfer（LET）,which indicates the maximum deposited energy on the device without SEB behavior, increases from 0.06 to0.7 p C/μm. The SEB threshold voltage increases to 120 V, which is 80% of the rated breakdown voltage. Meanwhile, the main parameter characteristics of the proposed structure remain similar with those of the conventional planar structure. Therefore, this structure offers a potential optimization path to planar power MOSFET with high SEB survivability for space and atmospheric applications.
文摘针对空间应用,开展SiC MOSFET单粒子效应试验研究。在加速器上用重离子辐照1200 V SiC MOSFET,离子线性能量传输(LET)在0.26~118 MeV·cm^(2)/mg之间,辐照中被试器件加50~600 V静态漏源偏置电压、栅源短接,实时测量电特性,进行辐照后栅应力(PIGS)测试。试验结果发现,50~100 V偏置电压下,离子引起瞬态电流,PIGS测试栅失效。分析认为离子引起栅氧化物潜在损伤,PIGS测试过程中,潜在损伤进一步退化导致栅失效。氧化物潜在损伤不仅与辐照偏置电压有关,还与入射离子LET和注量有关。PIGS测试需要的栅应力时间与潜在损伤程度有关,可超过300 s。并给出了电荷累积损伤模型。模型进行SiC MOSFET单粒子效应评估时,应考虑离子引起栅氧化物潜在损伤的影响,需根据轨道和任务周期确定试验离子注量,根据应用情况确定辐照偏置电压,并评估确定PIGS测试栅应力时间。
