CN107527958A - A kind of superlattices infrared detector surface passivation method - Google Patents
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Abstract
本发明一种超晶格红外探测器表面钝化方法,步骤一:取已完成台面刻蚀而未经钝化的超晶格材料样品,清洗后将样品装入高真空腔室中,真空度高于10‑6Torr;步骤二:利用原子层刻蚀技术在0‑150℃温度下对超晶格台面的表面及侧壁进行清理,以刻蚀并去除表面及侧壁上的氧化层以及前道工艺的残余污染物;步骤三:原子层刻蚀步骤结束后,在同一真空系统中利用原子层沉积技术在0‑280℃温度下逐层沉积生长钝化层,以钝化超晶格台面的表面及侧壁。本发明可有效提高台面侧向电阻率,从而抑制器件侧向漏电,提升探测器性能。
A surface passivation method of a superlattice infrared detector of the present invention, step 1: take the superlattice material sample that has been etched on the table surface without passivation, and put the sample into a high vacuum chamber after cleaning, and the vacuum degree Higher than 10 ‑6 Torr; step 2: use atomic layer etching technology to clean the surface and sidewall of the superlattice mesa at a temperature of 0‑150 ° C, to etch and remove the oxide layer on the surface and sidewall and Residual pollutants from the previous process; Step 3: After the atomic layer etching step, use atomic layer deposition technology in the same vacuum system to deposit and grow a passivation layer layer by layer at a temperature of 0-280°C to passivate the superlattice The surface and side walls of the countertop. The invention can effectively increase the lateral resistivity of the mesa, thereby suppressing the lateral leakage of the device and improving the performance of the detector.
Description
技术领域technical field
本发明属于半导体材料与器件技术领域,具体是一种超晶格红外探测器表面钝化方法,它可被应用于Ⅱ类超晶格红外探测器器件的表面钝化。The invention belongs to the technical field of semiconductor materials and devices, in particular to a method for passivating the surface of a superlattice infrared detector, which can be applied to the surface passivation of class II superlattice infrared detector devices.
背景技术Background technique
基于Ⅲ-Ⅴ族半导体InAs/GaSb的Ⅱ类超晶格材料是一种新型的红外探测器材料,相比于目前市场上的碲镉汞及超晶格探测器,具有1)通过改变超晶格结构可以大范围调节探测波长;2)俄歇复合几率较低,有利于提高工作温度;3)材料的红外吸收系数高,带间跃迁的光电效率高;4)超晶格结构的电子隧穿几率较低,从而降低了暗电流;5)制作大面阵器件的成本和难度较低等诸多优势,因此红外探测器在军用及民用领域的应用范围日益扩展,涵盖了战略预警、战场监视、大气监测、空间通讯、星载探测、安防监控、智能交通和医疗等领域。The class II superlattice material based on III-V semiconductor InAs/GaSb is a new type of infrared detector material. Compared with the mercury cadmium telluride and superlattice detectors currently on the market, it has The lattice structure can adjust the detection wavelength in a large range; 2) the Auger recombination probability is low, which is beneficial to increase the working temperature; 3) the infrared absorption coefficient of the material is high, and the photoelectric efficiency of the interband transition is high; 4) the electron tunneling of the superlattice structure 5) There are many advantages such as low cost and difficulty in making large area array devices, so the application range of infrared detectors in military and civilian fields is expanding day by day, covering strategic early warning, battlefield surveillance , Atmospheric monitoring, space communication, spaceborne detection, security monitoring, intelligent transportation and medical treatment and other fields.
在制作超晶格红外探测器器件时,需要将生长好的超晶格外延片刻蚀成分立的台面,此时台面的侧壁成为了裸露在环境中的新的表面。二类超晶格材料由于有效禁带宽度很小(小于0.3eV,有的甚至小于0.03eV),在材料的表面由于界面的存在能带将会弯曲,能带的弯曲很容易在窄禁带材料表面产生载流子的势阱,从而形成表面导电层;同时,InAs、GaSb两种材料都容易被氧化,并形成单质的半金属As和和金属Sb残留于台面侧面,使表面粗糙,引入表面态,增加表面非辐射复合,增加侧壁漏电,所以表面钝化工艺对Ⅱ类超晶格红外探测器的性能至关重要。另外需要注意的是,InAs/GaSb超晶格材料不能忍受高温的工艺过程,而目前常见的钝化层生长工艺中大于300℃的工艺温度会对超晶格结构造成损伤从而影响其性能,因此非常有必要开发一种低温的表面钝化工艺。When making a superlattice infrared detector device, it is necessary to etch the grown superlattice epitaxial wafer into discrete mesas, and at this time the side walls of the mesas become new surfaces exposed to the environment. Due to the small effective bandgap width of the second type superlattice material (less than 0.3eV, some even less than 0.03eV), the energy band will be bent on the surface of the material due to the existence of the interface, and the bending of the energy band is easy to occur in the narrow bandgap A potential well of carriers is generated on the surface of the material, thereby forming a surface conductive layer; at the same time, both InAs and GaSb are easily oxidized, and form a single semi-metal As and metal Sb remaining on the side of the mesa, making the surface rough and introducing Surface states increase surface non-radiative recombination and sidewall leakage, so the surface passivation process is crucial to the performance of type II superlattice infrared detectors. In addition, it should be noted that InAs/GaSb superlattice materials cannot tolerate high-temperature processes, and the process temperature greater than 300°C in the current common passivation layer growth process will cause damage to the superlattice structure and affect its performance. It is very necessary to develop a low temperature surface passivation process.
发明内容Contents of the invention
本发明的目的是提供一种超晶格红外探测器表面钝化方法,可有效提高台面侧向电阻率,从而抑制器件侧向漏电,提升探测器性能。The purpose of the present invention is to provide a surface passivation method of a superlattice infrared detector, which can effectively increase the lateral resistivity of the mesa, thereby suppressing the lateral leakage of the device and improving the performance of the detector.
本发明通过如下技术方案实现上述目的:The present invention realizes above-mentioned purpose through following technical scheme:
一种超晶格红外探测器表面钝化方法,包括以下步骤:A method for passivating the surface of a superlattice infrared detector, comprising the following steps:
步骤一:取已完成台面刻蚀而未经钝化的超晶格材料样品,清洗后将样品装入高真空腔室中,真空度高于10-6Torr;Step 1: Take a sample of the superlattice material that has been etched on the mesa without passivation, and put the sample into a high vacuum chamber after cleaning, and the vacuum degree is higher than 10 -6 Torr;
步骤二:利用原子层刻蚀技术在0-150℃温度下对超晶格台面的表面及侧壁进行清理,以刻蚀并去除表面及侧壁上的氧化层以及前道工艺的残余污染物;Step 2: Use atomic layer etching technology to clean the surface and sidewall of the superlattice mesa at a temperature of 0-150°C to etch and remove the oxide layer on the surface and sidewall as well as residual pollutants from the previous process ;
步骤三:原子层刻蚀步骤结束后,在同一真空系统中利用原子层沉积技术在0-280℃温度下逐层沉积生长钝化层,以钝化超晶格台面的表面及侧壁。Step 3: After the atomic layer etching step is completed, the atomic layer deposition technology is used in the same vacuum system to deposit and grow a passivation layer layer by layer at a temperature of 0-280° C. to passivate the surface and side walls of the superlattice mesa.
进一步的,所述超晶格材料为锑化物基Ⅱ类超晶格红外探测器材料。Further, the superlattice material is an antimonide-based type II superlattice infrared detector material.
进一步的,所述步骤二中的原子层刻蚀是将样品暴露于含氯等离子体、含氩或含氖等离子体的交替脉冲中,以逐层刻蚀样品的表面和侧壁,交替脉冲的重复周期大于或等于1。Further, the atomic layer etching in the second step is to expose the sample to alternating pulses of chlorine-containing plasma, argon-containing or neon-containing plasma to etch the surface and sidewall of the sample layer by layer, and the alternating pulses The recurrence period is greater than or equal to 1.
进一步的,所述步骤三中的原子层沉积工艺生长的钝化层材料包括氧化铝、氧化硅、氮化硅或Ⅲ-Ⅴ族化合物,所述钝化层由单层、两层或多层所述钝化层材料堆叠而成,Further, the material of the passivation layer grown by the atomic layer deposition process in the step 3 includes aluminum oxide, silicon oxide, silicon nitride or III-V group compounds, and the passivation layer consists of a single layer, two layers or multiple layers The passivation layer materials are stacked,
进一步的,所述钝化层总厚度为2-1000纳米。Further, the total thickness of the passivation layer is 2-1000 nanometers.
与现有技术相比,本发明超晶格红外探测器表面钝化方法的有益效果是:1)工艺全程都在同一个高真空系统中进行,中途不暴露大气,清理过后的材料表面不会再次被氧化或吸附水分;2)台面的表面和侧壁经过原子层刻蚀技术的清理,氧化层和杂质污染物被去除干净,保障了钝化层和超晶格之间的界面质量,可以得到较高的侧向电阻率,抑制器件侧向漏电,提升器件性能;3)原子层沉积技术生长钝化层时,采用的沉积温度较低,因此钝化工艺过程对超晶格结构无损伤;4)原子层沉积技术沉积的钝化层厚度均匀,元素配比精确,电阻率高,可实现大面阵器件的高质量钝化;5)原子层刻蚀和原子层沉积技术都是有自限制性的、各向同性和随形性的工艺过程,可以通过反应周期数来控制工艺厚度,并且刻蚀或生长不受台面形状或高度的影响,因此本钝化工艺易于控制、重复性高,可应用于各波段超晶格红外探测器器件的表面钝化。Compared with the prior art, the beneficial effects of the superlattice infrared detector surface passivation method of the present invention are: 1) the whole process is carried out in the same high-vacuum system, the atmosphere is not exposed midway, and the material surface after cleaning will not 2) The surface and side walls of the mesa are cleaned by atomic layer etching technology, and the oxide layer and impurity pollutants are removed, which ensures the quality of the interface between the passivation layer and the superlattice, which can Obtain higher lateral resistivity, suppress device lateral leakage, and improve device performance; 3) When the atomic layer deposition technology grows the passivation layer, the deposition temperature used is low, so the passivation process has no damage to the superlattice structure ; 4) The thickness of the passivation layer deposited by atomic layer deposition technology is uniform, the ratio of elements is accurate, and the resistivity is high, which can realize high-quality passivation of large area array devices; 5) atomic layer etching and atomic layer deposition technology are both effective Self-limiting, isotropic and conformal process, the process thickness can be controlled by the number of reaction cycles, and etching or growth is not affected by the shape or height of the mesa, so the passivation process is easy to control and repeatable High, it can be applied to the surface passivation of superlattice infrared detector devices in various bands.
附图说明Description of drawings
图1是经过钝化后的超晶格台面示意图。Figure 1 is a schematic diagram of a passivated superlattice mesa.
图2是83K下未钝化与已钝化器件的台面侧向电阻率对比图。Figure 2 is a comparison of the mesa lateral resistivity of unpassivated and passivated devices at 83K.
具体实施方式detailed description
下面结合附图对本发明的技术方案作进一步的说明。The technical scheme of the present invention will be further described below in conjunction with the accompanying drawings.
本实施例展示了一种超晶格红外探测器表面钝化方法,为了表现本发明的钝化效果,本实施例的步骤包括:This embodiment shows a method for passivating the surface of a superlattice infrared detector. In order to show the passivation effect of the present invention, the steps of this embodiment include:
步骤一:取四个已完成台面刻蚀而未经钝化的超晶格材料样品,超晶格材料为锑化物基Ⅱ类超晶格红外探测器材料,包括而不限于InAs/GaSb超晶格、InAs/InAsSb超晶格等,样品是90%截止波长为12.3微米的长波红外探测器材料,台面形状为正方形,台面边长分别为75微米、150微米、270微米和400微米,将样品用丙酮清洗后装入高真空腔室中,真空度高于10-6Torr,优选为5×10-7Torr;Step 1: Take four samples of superlattice materials that have completed mesa etching without passivation. The superlattice materials are antimonide-based Class II superlattice infrared detector materials, including but not limited to InAs/GaSb supercrystals Lattice, InAs/InAsSb superlattice, etc. The sample is a long-wave infrared detector material with a 90% cut-off wavelength of 12.3 microns. After cleaning with acetone, put it into a high vacuum chamber, the vacuum degree is higher than 10 -6 Torr, preferably 5×10 -7 Torr;
步骤二:利用原子层刻蚀(Atomic Layer Etching,ALE)技术在0-150℃,优选为30℃下对超晶格台面的表面及侧壁进行清理,以刻蚀并去除表面及侧壁上的氧化层以及前道工艺的残余污染物,原子层刻蚀采用的是含氯等离子体和含氩等离子体的交替脉冲,交替脉冲的重复周期大于或等于1,优选为重复刻蚀5个周期,刻蚀厚度约为1纳米;Step 2: Use atomic layer etching (Atomic Layer Etching, ALE) technology to clean the surface and sidewall of the superlattice mesa at 0-150°C, preferably 30°C, to etch and remove the surface and sidewall The oxide layer and the residual pollutants of the previous process, the atomic layer etching uses alternating pulses of chlorine-containing plasma and argon-containing plasma, and the repetition period of the alternating pulse is greater than or equal to 1, preferably 5 cycles of repeated etching , the etching thickness is about 1 nanometer;
步骤三:原子层刻蚀步骤结束后,立即在同一真空系统中采用原子层沉积(AtomicLayer Deposition,ALD)技术生长钝化层材料,钝化层材料包括氧化铝、氧化硅、氮化硅或Ⅲ-Ⅴ族化合物,钝化层可以由单一的上述材料组成,也可由两层或多层上述材料堆叠而成,钝化层总厚度为2-1000纳米。钝化层优选为氧化铝钝化层,沉积温度为0-280℃,优选为120℃,采用三甲基铝和水分子的交替脉冲进行沉积,沉积得到的氧化铝钝化层厚度为10纳米。Step 3: Immediately after the atomic layer etching step is completed, the passivation layer material is grown by atomic layer deposition (Atomic Layer Deposition, ALD) technology in the same vacuum system. The passivation layer material includes aluminum oxide, silicon oxide, silicon nitride or III - Group V compounds, the passivation layer can be composed of a single above-mentioned material, or can be formed by stacking two or more layers of the above-mentioned materials, and the total thickness of the passivation layer is 2-1000 nanometers. The passivation layer is preferably an aluminum oxide passivation layer, the deposition temperature is 0-280°C, preferably 120°C, and the deposition is carried out by alternating pulses of trimethylaluminum and water molecules, and the thickness of the deposited aluminum oxide passivation layer is 10 nanometers .
作为对比,同时取另外四个与步骤一中尺寸相同的完成台面刻蚀但未经过表面钝化的超晶格材料样品待测。As a comparison, four other superlattice material samples of the same size as those in step 1 were taken for testing.
图1是经过钝化的超晶格器件示意图,其中P1表示超晶格台面,P2表示钝化层,P3表示超晶格所在的样品基底,P4和P5表示器件的一对电极。Figure 1 is a schematic diagram of a passivated superlattice device, where P1 represents the superlattice mesa, P2 represents the passivation layer, P3 represents the sample substrate where the superlattice is located, and P4 and P5 represent a pair of electrodes of the device.
利用液氮作为冷却源,在83K温度下测得所有未钝化与已钝化样品的R0A值,然后如图2所示,将各样品的周长面积比P/A与R0A值的倒数作线性拟合,使用公式:Using liquid nitrogen as a cooling source, the R 0 A values of all unpassivated and passivated samples were measured at a temperature of 83K, and then as shown in Figure 2, the perimeter area ratio P/A and R 0 A of each sample For a linear fit to the reciprocal of the value, use the formula:
即可得到未钝化与已钝化样品的ρSurface值,即台面侧向电阻率。对比可见,采用本发明钝化方法后,器件的台面侧向电阻率由10.5kΩ·cm提高到了137kΩ·cm,提高了一个数量级,同时超晶格材料的质量未见退化,这表明本发明钝化工艺有效抑制了器件的侧壁漏电,起到了良好的钝化作用。The ρ Surface value of the unpassivated and passivated samples can be obtained, that is, the lateral resistivity of the mesa. It can be seen from the comparison that after adopting the passivation method of the present invention, the lateral resistivity of the mesa of the device is increased from 10.5kΩ cm to 137kΩ cm, which is an order of magnitude improvement, and the quality of the superlattice material is not degraded at the same time, which shows that the passivation method of the present invention The oxidation process effectively suppresses the sidewall leakage of the device and plays a good passivation role.
以上所述的仅是本发明的一种实施方式。对于本领域的普通技术人员来说,在不脱离本发明创造构思的前提下,还可以做出若干变形和改进,这些都属于本发明的保护范围。What has been described above is only one embodiment of the present invention. For those skilled in the art, without departing from the inventive concept of the present invention, several modifications and improvements can be made, and these all belong to the protection scope of the present invention.
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| CN111129223A (en) * | 2019-12-26 | 2020-05-08 | 苏州焜原光电有限公司 | A Novel Fabrication Method of Superlattice Infrared Detectors |
| CN112635581A (en) * | 2020-12-30 | 2021-04-09 | 安徽光智科技有限公司 | Infrared detector and preparation method thereof |
| CN112838143A (en) * | 2020-12-31 | 2021-05-25 | 横店集团东磁股份有限公司 | A kind of deposition method of aluminum oxide film in PERC cell |
| CN114256379A (en) * | 2020-09-11 | 2022-03-29 | 上海丽恒光微电子科技有限公司 | A kind of refrigeration infrared detector and preparation method thereof |
| CN114256378A (en) * | 2020-09-11 | 2022-03-29 | 上海丽恒光微电子科技有限公司 | A kind of refrigeration infrared detector and preparation method thereof |
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| CN111129223A (en) * | 2019-12-26 | 2020-05-08 | 苏州焜原光电有限公司 | A Novel Fabrication Method of Superlattice Infrared Detectors |
| CN111129223B (en) * | 2019-12-26 | 2022-02-08 | 苏州焜原光电有限公司 | A Novel Fabrication Method of Superlattice Infrared Detectors |
| CN114256379A (en) * | 2020-09-11 | 2022-03-29 | 上海丽恒光微电子科技有限公司 | A kind of refrigeration infrared detector and preparation method thereof |
| CN114256378A (en) * | 2020-09-11 | 2022-03-29 | 上海丽恒光微电子科技有限公司 | A kind of refrigeration infrared detector and preparation method thereof |
| CN114256379B (en) * | 2020-09-11 | 2025-08-15 | 浙江珏芯微电子有限公司 | Refrigerating infrared detector and preparation method thereof |
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