CN110896114A - PIIN型高In组分InGaAs探测器材料结构和制备方法 - Google Patents
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Abstract
本发明公开了一种PIIN型高In组分InGaAs探测器材料结构和制备方法,所述探测材料结构由下往上依次为InP(001)衬底、n型InxAl1‑xAs缓冲层、i型InyGa1‑yAs吸收层、i型InzAl1‑zAs插入层和p型InzAl1‑zAs帽层。其中,所述的InzAl1‑zAs插入层的厚度为40nm~200nm,其掺杂浓度为2x1014cm‑3~1x1015cm‑3。制备方法为依次分子束外延生长即可。本发明的优势在于,InGaAs探测材料结构中增加的i型插入层能够有效实现对PN结结位置的控制,从而实现器件暗电流的降低。
Description
技术领域
本发明属于半导体光电子器件领域,特别涉及一种PIIN型高In组分InGaAs探测器材料结构和制备方法。
背景技术
与InP衬底晶格匹配的In0.53Ga0.47As三元系材料具有直接带隙和高电子迁移率的特点,其室温下的禁带宽度约0.75eV,对应的波长约1.7微米,恰好可以覆盖光纤通信波段,因此采用In0.53Ga0.47As三元系材料制作的光电探测器在光通信领域获得了普遍应用,并且在遥感、传感和成像等方面也有重要用途。在遥感领域,截止波长大于1.7微米的探测器有着更广泛的用途,能反应更多的信息。比如,2.1微米附近的探测在冰云检测和矿产资源探测方面均有重要价值,所以在气象、环境、资源等航天遥感领域具有重要的应用。通过增加InxGa1-xAs三元系材料中Ⅲ族元素In元素的组分x可以减小InGaAs材料的禁带宽度,从而增加InGaAs探测器的截止波长。比如,x=0.7时,InGaAs探测器的截止波长就能达到约2.2微米。但是,In组分的增加会造成InGaAs材料与InP衬底不再晶格匹配,从而在材料中引入位错,造成材料和器件性能变差。通过在InP衬底和InGaAs吸收层之间插入缓冲层,可以将位错主要限制在缓冲层中,减少InGaAs吸收层中的位错,提高In组分InGaAs探测器的性能,已经获得了一些进展。
为了减少衬底与吸收层之间的晶格失配带来的位错缺陷,目前主要采用在两层间插入组分渐变(或跃变)的缓冲层的方法。采用该技术可以有效抑制位错,改善吸收层的质量,从而使探测器性能得到改善。InAlAs材料与InGaAs材料十分相似,具有增加In的组分值则其晶格常数相应增加并保持直接带隙的特点。InAlAs材料对于所探测的光波长透明,有助于提高量子效率,同时也有利于减小表面复合,改善暗电流特性。因此采用宽禁带InAlAs材料作为帽层。
传统上,高In组分InGaAs探测材料的pn结界面位于InAlAs和InGaAs的异质界面或InGaAs层内。注意到pn结所处的材料禁带宽度越大,相应的探测器产生-复合暗电流越小,而光电流也会相应减小,所以对不同的探测器需要综合考虑,优化设计相应的探测器结构。
发明内容
本发明所要解决的技术问题是提供一种PIIN型高In组分InGaAs探测器材料结构和制备方法,该材料结构能够有效实现对PN结结位置的控制。
本发明的一种多层InGaAs探测器材料结构,所述探测材料结构由下往上依次为InP(001)衬底、n型InxAl1-xAs缓冲层、i型InyGa1-yAs吸收层、i型InzAl1-zAs插入层和p型InzAl1-zAs帽层。
所述的InP(001)衬底为半绝缘的InP(001)单晶衬底或者N型InP(001)单晶衬底。
所述的n型InxAl1-xAs缓冲层为线性渐变组分的掺Si的InxAl1-xAs材料或与吸收层晶格匹配的固定组分的掺Si的InxAl1-xAs材料,其中x的范围为0.52≤x≤1,其掺杂浓度为1x1016cm-3~5x1018cm-3。
所述的i型InyGa1-yAs吸收层,其组分具体为InyGa1-yAs,其中y的范围为0.53≤y≤1。
所述的i型InzAl1-zAs插入层,其组分具体为InzAl1-zAs,其中z的范围为0.52≤z≤1,厚度为40nm~200nm,其掺杂浓度为2x1014cm-3~1x1015cm-3。
所述的p型InzAl1-zAs帽层,其组分具体为InzAl1-zAs,其中z的范围为0.52≤z≤1,厚度为500nm~700nm,其掺杂浓度为1x1016cm-3~5x1018cm-3。
本发明的一种多层InGaAs探测器材料的制备方法,具体包括如下步骤:
(1)在InP(001)衬底上生长n型线性渐变组分的InxAl1-xAs或与吸收层晶格匹配的固定组分的InxAl1-xAs缓冲层;
(2)在n型InxAl1-xAs缓冲层上生长i型的高In组分InyGa1-yAs吸收层;
(3)生长与InyGa1-yAs层晶格匹配的固定组分的i型InzAl1-zAs材料,作为插入层;
(4)继续生长固定组分的p型InzAl1-zAs材料,作为帽层;
(5)完成PIIN型高In组分InGaAs探测器材料的制备。
有益效果
本发明提供一种PIIN型高In组分InGaAs探测器材料结构和制备方法,通过InAlAs插入层的结构设计,实现InGaAs探测器的成结由原来的异质结调整为同质结,有利于器件暗电流特性的优化。
附图说明
图1是本发明的PIIN型高In组分InGaAs探测器材料的结构示意图;
具体实施方式
下面结合具体实施例,进一步阐述本发明。应理解,这些实施例仅用于说明本发明而不用于限制本发明的范围。此外应理解,在阅读了本发明讲授的内容之后,本领域技术人员可以对本发明作各种改动或修改,这些等价形式同样落于本申请所附权利要求书所限定的范围。
实施例1
本实施例1举例说明本发明的PIIN型In0.53Ga0.47As探测器材料的制备方法,具体步骤如下:
(1)在半绝缘InP(001)衬底上生长1μm厚的n型线性渐变组分的InxAl1-xAs和与吸收层晶格匹配的固定组分的In0.52Al0.48As缓冲层,采用Si掺杂,电子浓度为1x1016cm-3;
(2)生长2μm厚的i型的In0.53Ga0.47As吸收层;
(3)生长40nm厚的i型的In0.52Al0.48As材料,作为插入层;
(4)生长500nm厚的p型In0.52Al0.48As材料,采用Be掺杂,空穴浓度为1x1016cm-3;
(5)完成PIIN型In0.53Ga0.47As探测器材料的制备。
实施例2
本实施例2举例说明本发明的PIIN型In0.7Ga0.3As探测器材料的制备方法,具体步骤如下:
(1)在N型InP(001)衬底上生长1μm厚的n型线性渐变组分的InxAl1-xAs和与吸收层晶格匹配的固定组分的In0.69Al0.31As缓冲层,采用Si掺杂,电子浓度为5x1017cm-3;
(2)生长2μm厚的i型的In0.7Ga0.3As吸收层;
(3)生长100nm厚的i型的In0.69Al0.31As材料,作为插入层;
(4)生长600nm厚的p型In0.69Al0.31As材料,采用Be掺杂,空穴浓度为5x1017cm-3;
(5)完成PIIN型In0.7Ga0.3As探测器材料的制备。
实施例3
本实施例3举例说明本发明的PIIN型In0.83Ga0.17As探测器材料的制备方法,具体步骤如下:
(1)在半绝缘InP(001)衬底上生长1μm厚的n型线性渐变组分的InxAl1-xAs和与吸收层晶格匹配的固定组分的In0.82Al0.18As缓冲层,采用Si掺杂,电子浓度为5x1018cm-3;
(2)生长1.5μm厚的i型的In0.83Ga0.17As吸收层;
(3)生长200nm厚的i型的In0.82Al0.18As材料,作为插入层;
(4)生长700nm厚的p型In0.82Al0.18As材料,采用Be掺杂,空穴浓度为5x1018cm-3;
(5)完成PIIN型In0.83Ga0.17As探测器材料的制备。
Claims (7)
1.一种PIIN型高In组分InGaAs探测器材料结构,其特征在于:所述探测材料结构自下往上依次为InP(001)衬底、n型InxAl1-xAs缓冲层、i型InyGa1-yAs吸收层、i型InzAl1-zAs插入层和p型InzAl1-zAs帽层。
2.根据权利要求1所述的一种PIIN型高In组分InGaAs探测器材料结构,其特征在于,所述的InP(001)衬底为半绝缘的InP(001)单晶衬底或者N型InP(001)单晶衬底。
3.根据权利要求1所述的一种PIIN型高In组分InGaAs探测器材料结构,其特征在于,所述的n型InxAl1-xAs缓冲层为线性渐变组分的掺Si的InxAl1-xAs材料或与吸收层晶格匹配的固定组分的掺Si的InxAl1-xAs材料,其中x的范围为0.52≤x≤1,其掺杂浓度为1x1016cm-3~5x1018cm-3。
4.根据权利要求1所述的一种PIIN型高In组分InGaAs探测器材料结构,其特征在于,所述的i型InyGa1-yAs吸收层的组分具体为InyGa1-yAs,其中y的范围为0.53≤y≤1。
5.根据权利要求1所述的一种PIIN型高In组分InGaAs探测器材料结构,其特征在于,所述的i型InzAl1-zAs插入层的组分为InzAl1-zAs,其中z的范围为0.52≤z≤1,厚度为40nm~200nm,其掺杂浓度为2x1014cm-3~1x1015cm-3。
6.根据权利要求1所述的一种PIIN型高In组分InGaAs探测器材料结构,其特征在于,所述的p型InzAl1-zAs帽层的组分为InzAl1-zAs,其中z的范围为0.52≤z≤1,厚度为500nm~700nm,其掺杂浓度为1x1016cm-3~5x1018cm-3。
7.一种制备如权利要求1所述的PIIN型高In组分InGaAs探测器材料结构的方法,其特征在于方法步骤如下:
(1)在InP(001)衬底上生长n型线性渐变组分的InxAl1-xAs或与吸收层晶格匹配的固定组分的InxAl1-xAs缓冲层;
(2)在n型InxAl1-xAs缓冲层上生长i型的高In组分InyGa1-yAs吸收层;
(3)生长与InyGa1-yAs层晶格匹配的固定组分的i型InzAl1-zAs材料,作为插入层;
(4)继续生长固定组分的p型InzAl1-zAs材料,作为帽层;
(5)完成PIIN型高In组分InGaAs探测器材料的制备。
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Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102332456A (zh) * | 2011-10-11 | 2012-01-25 | 清华大学 | 光探测器集成器件及制备方法 |
US20120145996A1 (en) * | 2010-10-22 | 2012-06-14 | California Institute Of Technology | Barrier infrared detector |
CN103367520A (zh) * | 2013-06-27 | 2013-10-23 | 中国科学院上海微系统与信息技术研究所 | InP基截止波长大范围可调的晶格匹配InGaAsBi探测器结构及其制备 |
CN104319307A (zh) * | 2014-09-26 | 2015-01-28 | 中国科学院长春光学精密机械与物理研究所 | PNIN型InGaAs红外探测器 |
CN105185846A (zh) * | 2015-08-26 | 2015-12-23 | 中国科学院长春光学精密机械与物理研究所 | PBN型InGaAs红外探测器 |
-
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Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20120145996A1 (en) * | 2010-10-22 | 2012-06-14 | California Institute Of Technology | Barrier infrared detector |
CN102332456A (zh) * | 2011-10-11 | 2012-01-25 | 清华大学 | 光探测器集成器件及制备方法 |
CN103367520A (zh) * | 2013-06-27 | 2013-10-23 | 中国科学院上海微系统与信息技术研究所 | InP基截止波长大范围可调的晶格匹配InGaAsBi探测器结构及其制备 |
CN104319307A (zh) * | 2014-09-26 | 2015-01-28 | 中国科学院长春光学精密机械与物理研究所 | PNIN型InGaAs红外探测器 |
CN105185846A (zh) * | 2015-08-26 | 2015-12-23 | 中国科学院长春光学精密机械与物理研究所 | PBN型InGaAs红外探测器 |
Non-Patent Citations (1)
Title |
---|
GAO XIN-JIANG 等: "Short wave infrared InGaAs focal plane arrays detector: the performance optimization of photosensitive element", 《PROC. OF SPIE》 * |
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