CN108039391A - 一种氧化镓x射线探测器及其制备方法 - Google Patents

一种氧化镓x射线探测器及其制备方法 Download PDF

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CN108039391A
CN108039391A CN201711286493.XA CN201711286493A CN108039391A CN 108039391 A CN108039391 A CN 108039391A CN 201711286493 A CN201711286493 A CN 201711286493A CN 108039391 A CN108039391 A CN 108039391A
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矫淑杰
李少方
张峻华
高世勇
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Harbin Institute of Technology
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Abstract

本发明公开了一种氧化镓X射线探测器及其制备方法,属于半导体器件制造领域。本发明要解决以硅、锗、CdTe和CdZnTe等半导体作为x射线探测器,由于材料带隙较小,对环境温度敏感、抗辐射特性弱,限制了在太空领域的应用的技术问题。本发明探测器以氧化镓单晶为基体,所述氧化镓单晶的上表面设置有接触电极和Pt/Au工作电极,下表面设置有ITO/Ti/Au工作电极,Pt/Au工作电极的顶部和ITO/Pt/Au工作电极的底部与外接电路通过连接引线连接;通过沉积制备。本发明的氧化镓x射线探测器可在室温工作,也可耐受高压,并在严苛环境下工作。

Description

一种氧化镓X射线探测器及其制备方法
技术领域
本发明属于半导体器件制造领域;具体涉及一种氧化镓X射线探测器及其制备方法。
背景技术
X射线探测器主要应用于外太空、核电站等苛刻环境中,探测器需要高灵敏度、小型化、抗辐射能力强等特性。传统气体探测器是通过气体离化产生探测信号所需能量约为30eV,对弱信号的检测灵敏度低。气体探测器密度小,体积大,不利于器件的小型化,也不利于集成为大规模阵列器件,并且不能室温工作,无法满足日益增长的应用需求。半导体x射线探测器由于带隙能量小于10eV,因此产生电子空穴对的辐射能量也小于10eV,相对气体探测器而言对弱信号检测灵敏度高,半导体单晶材料厚度在几个毫米范围内,在器件小型化方面具有优势;半导体探测器还可制成探测阵列。
发展较早的硅、锗、CdTe和CdZnTe等半导体作为x射线探测器,由于材料带隙较小,对环境温度敏感、抗辐射特性弱,限制了在太空领域的应用。
发明内容
本发明要解决以硅、锗作为x射线探测器,由于材料带隙较小,对环境温度敏感、抗辐射特性弱,限制了在太空领域的应用的技术问题;而提供了一种氧化镓X射线探测器及其制备方法。
为解决上述技术问题,本发明的一种氧化镓X射线探测器以氧化镓单晶为基体,所述氧化镓单晶的上表面设置有接触电极和Pt/Au工作电极,下表面设置有ITO/Ti/Au工作电极,Pt/Au工作电极的顶部和ITO/Ti/Au工作电极的底部与外接电路通过连接引线连接,接触电极接地;
所述接触电极和Pt/Au工作电极的横截面呈“回”字形,且Pt/Au工作电极设置在接触电极内,从下至上,接触电极和Pt/Au工作电极是由沉积在氧化镓单晶上表面的铂层和金层构成;
从上至下,ITO/Ti/Au工作电极是由依次沉积在氧化镓单晶的下表面的ITO薄膜、钛层和金层构成。
进一步地限定,所述氧化镓单晶体基体横截面为边长为2-5mm的正方形,氧化镓单晶的厚度为300~1000μm。
进一步地限定,所述Pt/Au工作电极中铂层的厚度为20~100nm,金层的厚度为200~500nm。
进一步地限定,所述ITO/Ti/Au工作电极中ITO薄膜的厚度为10~100nm,钛层的厚度为20~100nm,金层的厚度为200~500nm。
本发明中上述氧化镓X射线探测器的制备方法是按下述步骤进行的:
步骤一、在氧气气氛下,将氧化镓单晶退火,依次在丙酮、乙醇中超声处理后用去离子水冲洗,用氮气吹干;
步骤二、然后在氧化镓单晶的一侧依次沉积ITO薄膜(氧化铟锡导电薄膜),再在真空状态下退火;
步骤三、然后在氧化镓单晶上,与ITO薄膜相对的一侧用掩膜版覆盖,再依次沉积铂层和金层,形成接触电极和Pt/Au工作电极;
步骤四、然后在ITO薄膜之上沉积钛层和金层,形成ITO/Ti/Au工作电极;
步骤五、然后在氮气保护下退火;
步骤六、将接触电极接地,将Pt/Au工作电极和ITO/Ti/Au工作电极与外接电路通过连接引线连接,即获得氧化镓X射线探测器。
进一步地限定,步骤一退火温度为700℃~1000℃,退火时间为1h~10h。
进一步地限定,步骤二退火温度为700℃~1000℃,退火时间为1h~5h。
进一步地限定,步骤二退火温度为350℃~400℃,退火时间为0.5h~2h。
本发明设置的接触电极有效地减少表面缺陷引起的漏电流。
本发明探测器的宽带隙半导体带隙更宽,热效应不明显,抗辐射特性更强,击穿电场强,其中禁带宽度达到4.9eV,击穿电场高至8MV/cm,约是SiC或GaN的2至3倍,介电常数高至10,以及电子迁移率高至300cm2/Vs,平均原子序数为17.2,较之ZnO和GaN的原子序数更大,本发明的氧化镓x射线探测器具有显著优势。
本发明制作工艺简单实用。
本发明的氧化镓x射线探测器可在室温工作,也可耐受高压,并在严苛环境下工作。
附图说明
图1是本发明所述探测器的结构示意图,图2是掩膜版的结构示意图;
图中1——Pt/Au工作电极的金层,2——铂层,3——氧化镓单晶,4——ITO薄膜,5——钛层,6——ITO/Ti/Au工作电极的金层,7——外接电路,8——外侧的方形环,9——中间正方形。
具体实施方式
具体实施方式一:结合图1进行说明,本实施方式氧化镓X射线探测器以边长为2mm的正方形,厚度为500μm的氧化镓单晶3为基体,所述氧化镓单晶3的上表面设置有接触电极和Pt/Au工作电极,下表面设置有ITO/Ti/Au工作电极,Pt/Au工作电极的顶部和ITO/Ti/Au工作电极的底部与外接电路通过连接引线连接,接触电极接地;
所述接触电极和Pt/Au工作电极的横截面呈“回”字形,且Pt/Au工作电极设置在接触电极内,从下至上,接触电极和Pt/Au工作电极是由沉积在氧化镓单晶上表面的铂层2和金层1构成;
从上至下,ITO/Ti/Au工作电极是由依次沉积在氧化镓单晶3的下表面的ITO薄膜4、钛层5和金层6构成;具体制备方法按下述步骤进行的:
步骤一、在氧气气氛、反应温度为1000℃条件下,将氧化镓单晶退火5h,先在丙酮中超声处理5min,再在乙醇中超声处理5min,尔后用去离子水冲洗,之后用氮气吹干;
步骤二、然后在氧化镓单晶的一侧依次沉积厚度为50nm的ITO薄膜4(氧化铟锡导电薄膜),再在真空状态、反应温度为1000℃条件下退火2h;
步骤三、然后在氧化镓单晶上,与ITO薄膜相对的一侧用掩膜版覆盖,再依次沉积厚度为20nm的铂层2和厚度为200nm金层1,形成接触电极和Pt/Au工作电极;
步骤三所述Pt/Au工作电极形状为正方形,尺寸为500×500μm2
接触电极的形状为方形环,外边长为2×2cm2,内边长为1×1cm2
步骤四、然后在ITO薄膜4之上沉积厚度为20nm的钛层5和厚度为500nm的金层6,形成ITO/Ti/Au工作电极;
步骤五、然后在氮气保护、反应温度为400℃条件下退火2h;
步骤六、将接触电极接地,将Pt/Au工作电极和ITO/Pt/Au工作电极与外接电路7通过连接引线连接,即获得氧化镓X射线探测器。
其中,步骤三使用的所述掩膜版如图2所示,中间正方形9尺寸为500×500μm2;外侧的方形环8的外边长为2×2cm2,内边长为1×1cm2
本实施在Pt/Au工作电极外侧设置的接触电极有效地减少表面缺陷引起的漏电流。

Claims (8)

1.一种氧化镓X射线探测器,其特征在于所述探测器以氧化镓单晶为基体,所述氧化镓单晶的上表面设置有接触电极和Pt/Au工作电极,下表面设置有ITO/Ti/Au工作电极,Pt/Au工作电极的顶部和ITO/Ti/Au工作电极的底部与外接电路通过连接引线连接,接触电极接地;
所述接触电极和Pt/Au工作电极的横截面呈“回”字形,且Pt/Au工作电极设置在接触电极内,从下至上,接触电极和Pt/Au工作电极是由沉积在氧化镓单晶上表面的铂层和金层构成;
从上至下,ITO/Ti/Au工作电极是由依次沉积在氧化镓单晶的下表面的ITO薄膜、钛层和金层构成。
2.根据权利要求1所述的一种氧化镓X射线探测器,其特征在于所述氧化镓单晶体基体横截面为边长为2-5mm的正方形,氧化镓单晶的厚度为300~1000μm。
3.根据权利要求2所述的一种氧化镓X射线探测器,其特征在于所述Pt/Au工作电极中铂层的厚度为20~100nm,金层的厚度为200~500nm。
4.根据权利要求3所述的一种氧化镓X射线探测器,其特征在于所述ITO/Ti/Au工作电极中ITO薄膜的厚度为10~100nm,钛层的厚度为20~100nm,金层的厚度为200~500nm。
5.如权利要求1-4任意一项权利要求所述的一种氧化镓X射线探测器的制备方法,其特征在于所述制备方法是按下述步骤进行的:
步骤一、在氧气气氛下,将氧化镓单晶退火,依次在丙酮、乙醇中超声处理后用去离子水冲洗,用氮气吹干;
步骤二、然后在氧化镓单晶的一侧依次沉积ITO薄膜(氧化铟锡导电薄膜),再在真空状态下退火;
步骤三、然后在氧化镓单晶上,与ITO薄膜相对的一侧用掩膜版覆盖,再依次沉积铂层和金层,形成接触电极和Pt/Au工作电极;
步骤四、然后在ITO薄膜之上沉积钛层和金层,形成ITO/Ti/Au工作电极;
步骤五、然后在氮气保护下退火;
步骤六、将接触电极接地,将Pt/Au工作电极和ITO/Ti/Au工作电极与外接电路通过连接引线连接,即获得氧化镓X射线探测器。
6.根据权利要5所述的一种氧化镓X射线探测器的制备方法,其特征在于步骤一退火温度为700℃~1000℃,退火时间为1h~10h。
7.根据权利要5所述的一种氧化镓X射线探测器的制备方法,其特征在于步骤二退火温度为700℃~1000℃,退火时间为1h~5h。
8.根据权利要5所述的一种氧化镓X射线探测器的制备方法,其特征在于步骤五退火温度为350℃~400℃,退火时间为0.5h~2h。
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