CN115172171A - Method for improving reverse breakdown voltage of gallium oxide diode based on neutron radiation - Google Patents
Method for improving reverse breakdown voltage of gallium oxide diode based on neutron radiation Download PDFInfo
- Publication number
- CN115172171A CN115172171A CN202210873436.6A CN202210873436A CN115172171A CN 115172171 A CN115172171 A CN 115172171A CN 202210873436 A CN202210873436 A CN 202210873436A CN 115172171 A CN115172171 A CN 115172171A
- Authority
- CN
- China
- Prior art keywords
- neutron
- neutron source
- dose
- breakdown voltage
- radiation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000015556 catabolic process Effects 0.000 title claims abstract description 32
- 230000005855 radiation Effects 0.000 title claims abstract description 25
- AJNVQOSZGJRYEI-UHFFFAOYSA-N digallium;oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[Ga+3].[Ga+3] AJNVQOSZGJRYEI-UHFFFAOYSA-N 0.000 title claims abstract description 22
- 229910001195 gallium oxide Inorganic materials 0.000 title claims abstract description 22
- 238000000034 method Methods 0.000 title claims abstract description 16
- 229910005191 Ga 2 O 3 Inorganic materials 0.000 claims abstract description 24
- 239000000463 material Substances 0.000 claims abstract description 8
- 239000002356 single layer Substances 0.000 claims description 6
- 238000004364 calculation method Methods 0.000 claims description 5
- 239000010410 layer Substances 0.000 claims description 5
- 238000000342 Monte Carlo simulation Methods 0.000 claims description 2
- 239000011148 porous material Substances 0.000 abstract 1
- 238000012360 testing method Methods 0.000 description 17
- 239000004065 semiconductor Substances 0.000 description 9
- 238000006731 degradation reaction Methods 0.000 description 5
- 125000004429 atom Chemical group 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000011156 evaluation Methods 0.000 description 3
- JJWKPURADFRFRB-UHFFFAOYSA-N carbonyl sulfide Chemical compound O=C=S JJWKPURADFRFRB-UHFFFAOYSA-N 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000007547 defect Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000002245 particle Substances 0.000 description 2
- 230000000149 penetrating effect Effects 0.000 description 2
- 238000002360 preparation method Methods 0.000 description 2
- 238000011160 research Methods 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- 241000282412 Homo Species 0.000 description 1
- 241000282414 Homo sapiens Species 0.000 description 1
- 206010028980 Neoplasm Diseases 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000033228 biological regulation Effects 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 230000007812 deficiency Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 239000003814 drug Substances 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 230000004992 fission Effects 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 125000004433 nitrogen atom Chemical group N* 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 238000001959 radiotherapy Methods 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
- 238000002560 therapeutic procedure Methods 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/34—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies not provided for in groups H01L21/18, H10D48/04 and H10D48/07, with or without impurities, e.g. doping materials
- H01L21/42—Bombardment with radiation
- H01L21/423—Bombardment with radiation with high-energy radiation
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D8/00—Diodes
- H10D8/60—Schottky-barrier diodes
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D99/00—Subject matter not provided for in other groups of this subclass
Landscapes
- Engineering & Computer Science (AREA)
- Health & Medical Sciences (AREA)
- Toxicology (AREA)
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Manufacturing & Machinery (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Thyristors (AREA)
Abstract
Description
技术领域technical field
本发明属于宽禁带半导体领域,具体涉及一种二极管反向击穿电压的提升方法,可用于高耐压大功率电力电子领域。The invention belongs to the field of wide band gap semiconductors, in particular to a method for increasing the reverse breakdown voltage of a diode, which can be used in the field of high withstand voltage and high power power electronics.
背景技术Background technique
氧化镓Ga2O3材料具有~4.9eV的宽禁带宽度,基于该材料研制的半导体器件具有较高的击穿电压,在高工作电压的电力电子器件方面具有巨大的应用优势。Ga2O3功率半导体器件作为一种非常有潜力的半导体元件,在电路中起到整流、放大、开关的作用,未来可以用做各种设备的电源、驱动负载以及电子设备的脉冲功率调节系统,在新能源、轨道交通、航空航天等领域具有重要的潜在应用价值。The gallium oxide Ga 2 O 3 material has a wide band gap of ~4.9eV, and the semiconductor devices developed based on this material have a high breakdown voltage, and have great application advantages in power electronic devices with high operating voltages. Ga 2 O 3 power semiconductor device, as a very potential semiconductor component, plays the role of rectification, amplification and switching in the circuit, and can be used as power supply for various equipment, driving load and pulse power regulation system for electronic equipment in the future. It has important potential application value in new energy, rail transit, aerospace and other fields.
随着空间电推进及电能管理领域的不断发展,对高性能电力电子器件提出了巨大的需求,Ga2O3功率器件正是满足这一需求的重要选择。二极管是Ga2O3功率器件的主要研究内容之一,二极管反向击穿电压的高低直接影响着器件在实际中的应用。目前,大多数研究主要通过改变二极管器件的结构来提高反向击穿电压。With the continuous development of space electric propulsion and power management, there is a huge demand for high-performance power electronic devices, and Ga 2 O 3 power devices are an important choice to meet this demand. Diode is one of the main research contents of Ga 2 O 3 power devices. The level of diode reverse breakdown voltage directly affects the application of the device in practice. At present, most researches mainly improve the reverse breakdown voltage by changing the structure of the diode device.
马晓华等人在申请号为202111069074.7专利文献中提出用具有P型特性的薄层NiO层与β-Ga2O3漂移层形成异质PN结结构,以降低器件边缘处的峰值电场,改善阳极金属与氧化镓界面特性,降低反向泄漏电流,提升氧化镓二极管的击穿电压。Ma Xiaohua et al. proposed in the patent document No. 202111069074.7 to form a hetero-PN junction structure with a thin NiO layer with P-type characteristics and a β-Ga 2 O 3 drift layer to reduce the peak electric field at the edge of the device and improve the anode metal The interface with gallium oxide reduces the reverse leakage current and improves the breakdown voltage of the gallium oxide diode.
冯倩等人在申请号为201710057175.X专利文献中提出在有机铁电介质层的边缘处沉积带有场板结构的肖特基二极管,以减小边缘处的电场强度,提高氧化镓肖特基二极管的反向击穿电压。Feng Qian et al. proposed in the patent document No. 201710057175.X to deposit a Schottky diode with a field plate structure at the edge of the organic ferrodielectric layer to reduce the electric field strength at the edge and improve the gallium oxide Schottky The reverse breakdown voltage of the diode.
上述两种方法虽说可提高器件反向击穿电压,但在提高器件反向击穿电压的同时,也带来了器件正向电流密度的严重降低;此外,这些方法由于都需要增加工艺步骤,技术难度较大,成品率低,制造成本高。Although the above two methods can improve the reverse breakdown voltage of the device, while increasing the reverse breakdown voltage of the device, it also brings a serious reduction in the forward current density of the device; in addition, these methods need to increase the process steps, The technical difficulty is relatively high, the yield is low, and the manufacturing cost is high.
发明内容:Invention content:
本发明的目的是针对上述已有技术的不足,提供一种基于中子辐射的氧化镓二极管反向击穿电压提升方法,以在提高反向击穿电压的同时保证正向电流密度和开启电压退化较小,提高器件成品率,降低制造成本。The purpose of the present invention is to provide a method for increasing the reverse breakdown voltage of a gallium oxide diode based on neutron radiation, aiming at the deficiencies of the above-mentioned prior art, so as to ensure the forward current density and the turn-on voltage while increasing the reverse breakdown voltage. Degradation is small, device yield is improved, and manufacturing cost is reduced.
本发明的技术方案是这样实现的:The technical scheme of the present invention is realized as follows:
一,技术原理1. Technical principle
中子广泛分布于太空和地球大气层中,太空中的中子主要来源于宇宙射线与行星表面或大气层中的原子碰撞;地球大气层中的中子主要来源于银河宇宙射线重离子与空气中的氧和氮原子发生的核反应。此外,人类进行的各种核试验也会产生大量的中子。目前,人类已经可以较成熟的通过核反应堆、加速器、自发裂变这些不同的方式产生出不同能量的中子,并逐渐应用于各个领域。Neutrons are widely distributed in space and the earth's atmosphere. Neutrons in space mainly come from the collision of cosmic rays with atoms on the surface of planets or in the atmosphere; neutrons in the earth's atmosphere mainly come from galactic cosmic ray heavy ions and oxygen in the air. nuclear reaction with nitrogen atoms. In addition, various nuclear tests conducted by humans also produce large amounts of neutrons. At present, human beings have been able to generate neutrons of different energies through different methods such as nuclear reactors, accelerators, and spontaneous fission, which are gradually applied in various fields.
中子作为各种辐射粒子中穿透性最强的粒子,对极大多数物质都具有很强的穿透性,且中子本身不带电,主要通过与被辐射物质的原子或分子发生核反应产生效应。在医疗上常用作肿瘤的放射治疗,如硼中子俘获治疗法;在工业上也常用于材料改性,如中子掺杂。As the most penetrating particle among all kinds of radiation particles, neutrons have strong penetrability to most substances, and neutrons themselves are not charged, and are mainly produced by nuclear reactions with atoms or molecules of irradiated substances. effect. It is commonly used in radiation therapy of tumors in medicine, such as boron neutron capture therapy; it is also commonly used in material modification in industry, such as neutron doping.
本发明正是基于中子的不带电和强穿透性的物理特性,利用中子辐射对氧化镓材料进行改性,以提高氧化镓二极管的反向击穿电压。其通过设置中子源设备所出射中子的能量和剂量参数对氧化镓二极管器件进行照射,使照射到氧化镓二极管器件上的中子与氧化镓晶格中的原子发生核反应而产生空位缺陷,这些空位缺陷以杂质补偿陷阱的形式存在,可降低氧化镓材料的掺杂浓度,导致掺杂浓度下器件的耗尽区宽度变大,器件边缘处的峰值电场减小,从而实现反向击穿电压的增大。The invention is based on the non-charged and strong penetrating physical properties of neutrons, and uses neutron radiation to modify the gallium oxide material to improve the reverse breakdown voltage of the gallium oxide diode. It irradiates the gallium oxide diode device by setting the energy and dose parameters of the neutrons emitted by the neutron source device, so that the neutrons irradiated on the gallium oxide diode device react with atoms in the gallium oxide lattice to generate vacancy defects, These vacancy defects exist in the form of impurity compensation traps, which can reduce the doping concentration of the gallium oxide material, resulting in an increase in the width of the depletion region of the device under the doping concentration, and a decrease in the peak electric field at the edge of the device, thereby achieving reverse breakdown. increase in voltage.
二,技术方案Second, technical solutions
根据上述原理,本发明基于中子辐射的氧化镓二极管反向击穿电压提升方法,其特征在于,包括如下步骤:According to the above principle, the method for boosting the reverse breakdown voltage of a gallium oxide diode based on neutron radiation of the present invention is characterized in that it includes the following steps:
选用中子源设备,根据氧化镓材料对中子辐射的耐受程度,设置该设备的中子能量为0.1MeV-20MeV,剂量为1×1013-1×1016n/cm2;Neutron source equipment is selected, and according to the tolerance of gallium oxide material to neutron radiation, the neutron energy of the equipment is set to 0.1MeV-20MeV, and the dose is 1×10 13 -1×10 16 n/cm 2 ;
将多只Ga2O3二极管水平均匀贴在PCB板上,再将该贴有器件的PCB板垂直放在中子源辐射设备的孔道位置;A plurality of Ga 2 O 3 diodes are evenly attached to the PCB board horizontally, and then the PCB board with the devices is placed vertically in the hole position of the neutron source radiation device;
检查中子源设备的各项设置参数无误后,打开电源对所贴器件进行中子辐照,直到中子源出射的中子剂量到达预设值后关闭电源,取出Ga2O3二极管,实现对其反向击穿电压的提升。After checking that the setting parameters of the neutron source equipment are correct, turn on the power to irradiate the attached device with neutrons until the neutron dose emitted by the neutron source reaches the preset value, then turn off the power, and take out the Ga 2 O 3 diode to achieve increase its reverse breakdown voltage.
进一步,所述多只Ga2O3二极管水平均匀贴在PCB板上,是将多只Ga2O3二极管器件按照与中子源设备的辐射孔道大小相同的圆周单层平铺或多层堆叠固定在PCB板上,保证中子源设备出射的中子能垂直于电极入射到器件中。Further, the plurality of Ga 2 O 3 diodes are evenly and horizontally attached to the PCB board, and the plurality of Ga 2 O 3 diode devices are tiled in a single layer or stacked in multiple layers according to the same size as the radiation channel of the neutron source device. It is fixed on the PCB board to ensure that the neutrons emitted by the neutron source device can be incident into the device perpendicular to the electrodes.
进一步,所述中子源设备的中子参数设置,是通过蒙特卡洛仿真结果确定,即在软件中将器件的结构进行建模后,把中子的能量和剂量值输入上述仿真软件,通过软件的计算结果评估出该能量和剂量下的中子辐射对器件的损伤情况,选取导致器件的正向电流密度退化幅度在5%-50%的中子参数,以此确定中子源出射的中子能量为0.1MeV-20MeV,剂量为1×1013-1×1016n/cm2。Further, the neutron parameter setting of the neutron source device is determined by the results of Monte Carlo simulation, that is, after modeling the structure of the device in the software, the energy and dose values of neutrons are input into the above simulation software, The calculation results of the software evaluate the damage of the neutron radiation to the device under the energy and dose, and select the neutron parameters that cause the degradation of the forward current density of the device to be 5%-50%, so as to determine the neutron source output. The neutron energy is 0.1MeV-20MeV, and the dose is 1×10 13 -1×10 16 n/cm 2 .
本发明由于不需要增加工艺步骤,技术难度较小,成品率高,制造成本低。Since the present invention does not need to increase the process steps, the technical difficulty is small, the yield is high, and the manufacturing cost is low.
测试结果表明,本发明在显著提高器件反向击穿电压的同时,器件的正向电流密度下降幅度小于20%,且开启电压仅增加0.05V±0.01V。The test results show that the present invention significantly improves the reverse breakdown voltage of the device, while the forward current density of the device decreases by less than 20%, and the turn-on voltage only increases by 0.05V±0.01V.
附图说明Description of drawings
图1为本发明是实现流程图;Fig. 1 is the realization flow chart for the present invention;
图2为采用本发明中子辐照前后的Ga2O3二极管反向击穿电压对比变化图;Fig. 2 is the contrast change diagram of the reverse breakdown voltage of Ga 2 O 3 diode before and after the neutron irradiation of the present invention;
图3为采用本发明中子辐照前后的Ga2O3二极管在低电压下的I-V测试对比图。FIG. 3 is a comparison diagram of IV test under low voltage of Ga 2 O 3 diodes before and after neutron irradiation using the present invention.
具体实施方式Detailed ways
下面结合附图对本发明的具体实例和效果做进一步详细的描述,但本发明的实施方式不限于此。Specific examples and effects of the present invention will be described in further detail below with reference to the accompanying drawings, but the embodiments of the present invention are not limited thereto.
参照图1,本发明给出如下三种实施例。1, the present invention provides the following three embodiments.
实施例1,设置氧化镓肖特基二极管器件的排列方式为单层平铺,中子源出射中子能量为1MeV,剂量为1×1014n/cm2。In Example 1, the arrangement of the gallium oxide Schottky diode devices is set as a single-layer tile, the neutron energy emitted by the neutron source is 1MeV, and the dose is 1×10 14 n/cm 2 .
步骤1,设置中子源设备的中子能量和剂量。
在蒙特卡洛软件中对氧化镓肖特基二极管的结构进行建模后,将中子能量和剂量值输入仿真软件,通过软件的计算结果评估出能量为1MeV,剂量为1×1014n/cm2的中子辐射对器件的损伤情况,评估结果表明,该条件下导致器件的正向电流密度退化幅度约为17%,以此确定选用中子源出射的能量为1MeV,剂量为1×1014n/cm2。After modeling the structure of the gallium oxide Schottky diode in Monte Carlo software, the neutron energy and dose values were input into the simulation software, and the calculation results of the software estimated that the energy was 1MeV and the dose was 1×10 14 n/ cm 2 neutron radiation damage to the device, the evaluation results show that the forward current density of the device is degraded by about 17% under this condition, so the energy of the selected neutron source is 1MeV, and the dose is 1× 10 14 n/cm 2 .
步骤2,设置器件的排列方式为单层平铺。
中子源设备的辐射孔道为固定大小的圆周,仅在该圆周范围内为有效中子辐照区域。为了较大限度的利用该区域,本实验将150只TO257封装的长方形Ga2O3肖特基二极管器件,按照器件之间长边与长边紧挨对齐,宽边与宽边紧挨对齐的方式,单层平铺排列在与中子源设备的辐射孔道大小相同的圆周范围内并固定在PCB板上,再将该贴有器件的PCB板垂直放在中子源辐射设备的孔道位置,以保证中子源设备出射的中子能垂直于电极入射到器件中。The radiation channel of the neutron source device is a circle with a fixed size, and only within the circle is the effective neutron irradiation area. In order to maximize the use of this area, in this experiment, 150 rectangular Ga 2 O 3 Schottky diode devices packaged in TO257 are aligned according to the long side and the long side of the devices, and the wide side and the wide side are closely aligned. The single-layer tile is arranged in the same circumferential range as the radiation channel of the neutron source device and fixed on the PCB board, and then the PCB board with the device is placed vertically on the channel position of the neutron source radiation device. In order to ensure that the neutrons emitted by the neutron source device can be incident into the device perpendicular to the electrodes.
步骤3,打开中子源设备,对器件进行辐照。Step 3, turn on the neutron source equipment and irradiate the device.
检查中子源设备的出射中子能量、剂量以及设备在正常工作下的各设置参数无误后打开总电源,对所贴器件进行中子辐照,直到中子源出射的中子剂量到达1×1014n/cm2后关闭电源,取出Ga2O3二极管,实现对其反向击穿电压的提升。After checking the neutron energy and dose of the neutron source equipment and the setting parameters of the equipment under normal operation, turn on the main power supply and irradiate the attached device with neutrons until the neutron dose emitted by the neutron source reaches 1× After 10 14 n/cm 2 , the power was turned off, and the Ga 2 O 3 diode was taken out to improve its reverse breakdown voltage.
实施例2,设置氧化镓肖特基二极管器件的排列方式为多层堆叠,中子源出射中子能量为1MeV,剂量为3×1014n/cm2。In Example 2, the arrangement of the gallium oxide Schottky diode devices is set to be multi-layer stacking, the neutron energy emitted by the neutron source is 1MeV, and the dose is 3×10 14 n/cm 2 .
步骤一,设置中子源设备的中子能量和剂量。Step 1: Set the neutron energy and dose of the neutron source equipment.
在蒙特卡洛软件中对氧化镓肖特基二极管的结构进行建模后,将中子能量和剂量值输入仿真软件,通过软件的计算结果评估出能量为1MeV,剂量为3×1014n/cm2的中子辐射对器件的损伤情况,评估结果表明,该条件下导致器件的正向电流密度退化幅度约为49%,以此确定选用中子源出射的能量为1MeV,剂量为3×1014n/cm2。After modeling the structure of the gallium oxide Schottky diode in Monte Carlo software, the neutron energy and dose values were input into the simulation software, and the calculation results of the software estimated that the energy was 1MeV and the dose was 3×10 14 n/ cm 2 neutron radiation damage to the device, the evaluation results show that the degradation of the forward current density of the device is about 49% under this condition, so the energy of the selected neutron source is 1MeV, and the dose is 3× 10 14 n/cm 2 .
步骤二,设置器件的排列方式为多层堆叠。In
2.1)将150只TO257封装的长方形Ga2O3肖特基二极管器件,先按照器件之间长边与长边紧挨对齐,宽边与宽边紧挨对齐的方式,单层平铺排列在与中子源设备的辐射孔道大小相同的圆周范围内并固定在PCB板上;2.1) Arrange 150 rectangular Ga 2 O 3 Schottky diode devices in a TO257 package, and arrange them in a single-layer tile according to the method that the long side and the long side of the devices are closely aligned, and the wide side and the wide side are closely aligned. Within the same circumference as the radiation channel of the neutron source device and fixed on the PCB;
2.2)重复2.1)的排列方式将器件分别排列并固定在n块PCB板上,n<50;2.2) Repeat the arrangement of 2.1) to arrange and fix the devices on n PCB boards respectively, n<50;
2.3)将分别贴有150只器件的n块PCB板按照2cm的间距垂直放在中子源辐射设备的孔道位置,以保证中子源设备出射的中子能垂直于电极入射到器件中。2.3) Place n PCB boards with 150 devices respectively placed in the hole position of the neutron source radiation device at a distance of 2cm to ensure that the neutrons emitted by the neutron source device can be incident into the device perpendicular to the electrodes.
步骤三,打开中子源设备,对器件进行辐照。Step 3, turn on the neutron source equipment, and irradiate the device.
检查中子源设备的出射中子能量、剂量以及设备在正常工作下的各设置参数无误后打开总电源,对所贴器件进行中子辐照,直到中子源出射的中子剂量到达3×1014n/cm2后关闭电源,取出Ga2O3二极管,实现对其反向击穿电压的提升。After checking the neutron energy and dose of the neutron source equipment and the setting parameters of the equipment under normal operation, turn on the main power supply and irradiate the attached device with neutrons until the neutron dose emitted by the neutron source reaches 3× After 10 14 n/cm 2 , the power was turned off, and the Ga 2 O 3 diode was taken out to improve its reverse breakdown voltage.
实施例3,设置氧化镓肖特基二极管器件的排列方式为多层堆叠,中子源出射中子能量为1MeV,剂量为3×1013n/cm2。In Example 3, the arrangement of the gallium oxide Schottky diode devices is set to be multi-layer stacking, the neutron energy emitted by the neutron source is 1MeV, and the dose is 3×10 13 n/cm 2 .
步骤A,设置中子源设备的中子能量和剂量。Step A, setting the neutron energy and dose of the neutron source device.
在蒙特卡洛软件中对氧化镓肖特基二极管的结构进行建模后,将中子能量和剂量值输入仿真软件,通过软件的计算结果评估出能量为1MeV,剂量为3×1013n/cm2的中子辐射对器件的损伤情况,评估结果表明,该条件下导致器件的正向电流密度退化幅度约为5%,以此确定选用中子源出射的能量为1MeV,剂量为3×1013n/cm2。After modeling the structure of the gallium oxide Schottky diode in Monte Carlo software, the neutron energy and dose values were input into the simulation software, and the calculation results of the software estimated that the energy was 1MeV and the dose was 3×10 13 n/ cm 2 neutron radiation damage to the device, the evaluation results show that the degradation of the forward current density of the device is about 5% under this condition, so the energy of the selected neutron source is 1MeV, and the dose is 3× 10 13 n/cm 2 .
步骤B,设置器件的排列方式为多层堆叠。In step B, the arrangement of the devices is set as a multi-layer stack.
本步骤的具体实现与实施例2的步骤二相同。The specific implementation of this step is the same as the second step in
步骤C,打开中子源设备,对器件进行辐照。In step C, the neutron source device is turned on, and the device is irradiated.
检查中子源设备的出射中子能量、剂量以及设备在正常工作下的各设置参数无误后打开总电源,对所贴器件进行中子辐照,直到中子源出射的中子剂量到达3×1013n/cm2后关闭电源,取出Ga2O3二极管,实现对其反向击穿电压的提升。After checking the neutron energy and dose of the neutron source equipment and the setting parameters of the equipment under normal operation, turn on the main power supply and irradiate the attached device with neutrons until the neutron dose emitted by the neutron source reaches 3× After 10 13 n/cm 2 , the power was turned off, and the Ga 2 O 3 diode was taken out to improve its reverse breakdown voltage.
以上描述仅是本发明的三个具体实例,并未构成对本发明的任何限制。对于本发明所属技术领域的普通技术人员来说,在不脱离本发明构思的前提下,还可以做出若干简单推理或者替换,都应当视为属于本发明的保护范围。The above descriptions are only three specific examples of the present invention, and do not constitute any limitation to the present invention. For those of ordinary skill in the technical field to which the present invention pertains, without departing from the concept of the present invention, some simple inferences or substitutions can be made, which should be regarded as belonging to the protection scope of the present invention.
本发明的效果可通过以下实测数据进一步说明:The effect of the present invention can be further illustrated by the following measured data:
一、测试条件1. Test conditions
选用半导体分析仪设备,设置I-V测试的测试电压为0—2V,测试精度为0.01V;设置测试器件反向击穿电压的电压为-1000—0V,测试精度为1V,限制电流设定为0.1mASelect semiconductor analyzer equipment, set the test voltage of the I-V test to 0-2V, and the test accuracy to 0.01V; set the voltage of the reverse breakdown voltage of the test device to -1000-0V, the test accuracy to 1V, and set the limit current to 0.1 mA
二.测试内容2. Test content
测试1,准备二十只同一制备工艺的Ga2O3肖特基二极管,选取其中的十只器件,依次将这些器件的正负两极连接到半导体分析仪设备上,在上述条件下,测试照射前器件的I-V曲线;再对该测试中选取的十只器件采用本发明方法进行照射后,依次将这些器件的正负两极连接到半导体分析仪设备上,在上述条件下,测试其照射后器件的I-V曲线,结果如图2。
从图3可看出中子辐照后器件的开启电压仅退化了0.05V,正向电流密度仅退化了17%,表明用本发明方法对器件的开启电压和正向电流密度造成的退化较小。It can be seen from Fig. 3 that the turn-on voltage of the device after neutron irradiation is only degraded by 0.05V, and the forward current density is only degraded by 17%, indicating that the degradation of the turn-on voltage and forward current density of the device is small by the method of the present invention .
测试2,准备同一制备工艺的另外二十只Ga2O3肖特基二极管,选取其中的十只器件,依次将这些器件的正负两极连接到半导体分析仪设备上,在上述条件下,测试其照射前的反向击穿电压;再对该测试中未选取的另外十只器件采用本发明方法进行照射后,依次将这些器件的正负两极连接到半导体分析仪设备上,在上述条件下,测试其照射后器件的反向击穿电压,结果如图3。
从图2可看出中子辐照前器件的反向击穿电压为540V,中子辐照后器件的反向击穿电压为925V。表明用本发明方法可使得器件的反向击穿电压提高近400V。It can be seen from Figure 2 that the reverse breakdown voltage of the device before neutron irradiation is 540V, and the reverse breakdown voltage of the device after neutron irradiation is 925V. It is shown that the reverse breakdown voltage of the device can be increased by nearly 400V by the method of the present invention.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202210873436.6A CN115172171A (en) | 2022-07-21 | 2022-07-21 | Method for improving reverse breakdown voltage of gallium oxide diode based on neutron radiation |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202210873436.6A CN115172171A (en) | 2022-07-21 | 2022-07-21 | Method for improving reverse breakdown voltage of gallium oxide diode based on neutron radiation |
Publications (1)
Publication Number | Publication Date |
---|---|
CN115172171A true CN115172171A (en) | 2022-10-11 |
Family
ID=83496447
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN202210873436.6A Pending CN115172171A (en) | 2022-07-21 | 2022-07-21 | Method for improving reverse breakdown voltage of gallium oxide diode based on neutron radiation |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN115172171A (en) |
Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
BE880836A (en) * | 1978-12-22 | 1980-06-23 | Westinghouse Electric Corp | METHOD FOR MANUFACTURING SEMICONDUCTOR DEVICES REDUCING THEIR SWITCHING TIME THROUGH NEUTRON IRRADIATION |
US5028556A (en) * | 1990-02-16 | 1991-07-02 | Hughes Aircraft Company | Process for fabricating radiation hard high voltage devices |
RU2006881C1 (en) * | 1991-04-19 | 1994-01-30 | Войсковая часть 51105 | Method for determining fluency rate of neutrons |
WO2000051187A1 (en) * | 1999-02-22 | 2000-08-31 | Infineon Technologies Ag | Method for regulating the breakdown voltage of a thyristor |
DE10207339A1 (en) * | 2002-02-21 | 2003-09-11 | Infineon Technologies Ag | Process for reducing mobility of free charge carriers in a semiconductor body uses high energy radiation followed by thermal processing |
US20160211330A1 (en) * | 2015-01-21 | 2016-07-21 | National Chiao Tung University | High electron mobility transistor |
CN112885890A (en) * | 2021-01-29 | 2021-06-01 | 中国电子科技集团公司第五十五研究所 | Structure for improving breakdown voltage of depletion type gallium nitride HEMT power device and preparation method thereof |
CN113871454A (en) * | 2021-09-28 | 2021-12-31 | 西安电子科技大学芜湖研究院 | Gallium oxide Schottky barrier diode based on silicon dioxide edge termination and preparation method thereof |
CN113964041A (en) * | 2021-09-13 | 2022-01-21 | 西安电子科技大学 | A high breakdown voltage gallium oxide power diode and preparation method thereof |
-
2022
- 2022-07-21 CN CN202210873436.6A patent/CN115172171A/en active Pending
Patent Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
BE880836A (en) * | 1978-12-22 | 1980-06-23 | Westinghouse Electric Corp | METHOD FOR MANUFACTURING SEMICONDUCTOR DEVICES REDUCING THEIR SWITCHING TIME THROUGH NEUTRON IRRADIATION |
US5028556A (en) * | 1990-02-16 | 1991-07-02 | Hughes Aircraft Company | Process for fabricating radiation hard high voltage devices |
RU2006881C1 (en) * | 1991-04-19 | 1994-01-30 | Войсковая часть 51105 | Method for determining fluency rate of neutrons |
WO2000051187A1 (en) * | 1999-02-22 | 2000-08-31 | Infineon Technologies Ag | Method for regulating the breakdown voltage of a thyristor |
DE10207339A1 (en) * | 2002-02-21 | 2003-09-11 | Infineon Technologies Ag | Process for reducing mobility of free charge carriers in a semiconductor body uses high energy radiation followed by thermal processing |
US20160211330A1 (en) * | 2015-01-21 | 2016-07-21 | National Chiao Tung University | High electron mobility transistor |
CN112885890A (en) * | 2021-01-29 | 2021-06-01 | 中国电子科技集团公司第五十五研究所 | Structure for improving breakdown voltage of depletion type gallium nitride HEMT power device and preparation method thereof |
CN113964041A (en) * | 2021-09-13 | 2022-01-21 | 西安电子科技大学 | A high breakdown voltage gallium oxide power diode and preparation method thereof |
CN113871454A (en) * | 2021-09-28 | 2021-12-31 | 西安电子科技大学芜湖研究院 | Gallium oxide Schottky barrier diode based on silicon dioxide edge termination and preparation method thereof |
Non-Patent Citations (2)
Title |
---|
袁晓利;吴凤美;施毅;郑有炓;: "脉冲中子辐照在硅中引起缺陷的研究", 固体电子学研究与进展, no. 03, 30 September 2001 (2001-09-30), pages 350 - 353 * |
邱彦章;张林;: "Ti/4H-SiC SBD中子辐照效应的研究", 微电子学, no. 05, 20 October 2013 (2013-10-20), pages 723 - 726 * |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Paternò et al. | Perovskite solar cell resilience to fast neutrons | |
Holmes et al. | A 4.5 μm PIN diamond diode for detecting slow neutrons | |
US20220349934A1 (en) | Detection Method for Sensitive Parts of Ionization Damage in Bipolar Transistor | |
Qiu et al. | Effects of neutron and gamma radiation on lithium-ion batteries | |
CN108254668A (en) | It is a kind of to analyze the method for interface state defects being accelerated to be formed during electronic component ionization radiation injury mechanism | |
Mackenzie et al. | A diamond gammavoltaic cell utilizing surface conductivity and its response to different photon interaction mechanisms | |
CN115172171A (en) | Method for improving reverse breakdown voltage of gallium oxide diode based on neutron radiation | |
RU2011141984A (en) | METHOD FOR TESTING CMOS / KND SEMICONDUCTOR BIS ON THE RESISTANCE TO EFFECTS OF SINGLE FAILURES FROM EXPOSURE TO HEAVY CHARGED SPACE PARTICLES | |
Chen et al. | Effects of total-ionizing-dose irradiation on single-event burnout for commercial enhancement-mode AlGaN/GaN high-electron mobility transistors | |
Sun et al. | Investigation of the performance degradation of 4H-SiC neutron detectors using MCNP and TCAD | |
Yue et al. | Investigation on the radiation induced conductivity of space-applied polyimide under cyclic electron irradiation | |
CN108362965B (en) | Method for inhibiting formation of oxide trapped charges based on displacement damage | |
Bilinski et al. | Proton-neutron damage equivalence in Si and Ge semiconductors | |
Bisello et al. | Neutron irradiation effects on standard and oxygenated silicon diodes | |
Zhang et al. | Radiation characterization of SiPMs for HERD PSD | |
Wanga et al. | Effect of C ion irradiation on AlGaAs/InGaAs HEMT | |
Consentino et al. | Dangerous Effects Induced on Power MOSFETs by Terrestrial Neutrons | |
Hashizume et al. | Direct energy conversion from gamma ray to electricity using silicon semiconductor cells | |
Shan et al. | Simulation of Ionization/Displacement Synergistic Effect on Bipolar Transistors under Different Processes conditions | |
Sharma et al. | Neutron induced oxide degradation in MOSFET structures | |
Yahya et al. | for Harsh Environment Applications | |
Matsumura et al. | Radiation damage to MPPCs by irradiation with protons | |
RU2304824C1 (en) | Method for increasing radiation resistance of devices based on gallium arsenide | |
Powell et al. | Photovoltaic Response of Thin-Film CdTe Solar Cells under Accelerated Neutron Radiation in a TRIGA Reactor | |
RU179476U1 (en) | DEVICE FOR TRANSFORMING ENERGY OF BETA RADIATION IN ELECTRICITY |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination |