CN109103283B - Transverse germanium detector structure and preparation method - Google Patents

Transverse germanium detector structure and preparation method Download PDF

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CN109103283B
CN109103283B CN201810956083.XA CN201810956083A CN109103283B CN 109103283 B CN109103283 B CN 109103283B CN 201810956083 A CN201810956083 A CN 201810956083A CN 109103283 B CN109103283 B CN 109103283B
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CN109103283A (en
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陈昌华
魏江镔
仇超
柏艳飞
甘甫烷
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Siluxtek Technologies Co ltd
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Abstract

The invention comprises a transverse germanium detector structure and a preparation method thereof, wherein the transverse germanium detector structure is a transverse photodiode and comprises a silicon substrate; a silicon oxide layer is deposited on the upper surface of the silicon substrate; the silicon oxide layer includes a top layer silicon; the germanium layer is formed on the upper surface of the top silicon and comprises a germanium layer main body, a first extending part and a second extending part, wherein the first extending part and the second extending part extend from the germanium layer main body to two sides respectively; and the silicon nitride waveguide is formed above the germanium layer and is of a conical structure. Has the advantages that: through reforming transform germanium layer structure, effectively strengthen the coupling efficiency that silicon nitride waveguide couples to the germanium detector, can realize the effective integration of optical multiplexer and optical demultiplexer and germanium detector, can also be applied to the photoelectric detection field of high optical power and high bandwidth.

Description

一种横向锗探测器结构及制备方法A kind of lateral germanium detector structure and preparation method

技术领域technical field

本发明涉及光学器件技术领域,尤其涉及一种横向锗探测器结构及制备方法。The invention relates to the technical field of optical devices, in particular to a lateral germanium detector structure and a preparation method.

背景技术Background technique

光复用器(mux)和光解复用器(demux)是目前光电子芯片中非常重要的光学器件之一,考虑到光复用器或者光解复用器工作的稳定性,比如受温度影响,受工艺条件而导致光复用器和光解复用器中心波长发生偏移及光谱曲线发生形变,我们需要选取合适的材料来制备光复用器和光解复用器。由于氮化硅(SiN)和氮氧化硅(SiON)的折射率随着温度变化的影响要远小于硅(Si)材料,因此光复用器和光解复用器选用SiN或者SiON作为材料,在实际应用中,光复用器和光解复用器的末端都会与探测器(PD)相连接实现光电转换,普通的光模块产品中,光复用器、光解复用器及探测器是在分立的两个芯片上通过光纤(fiber)来实现连接,进一步提高了产品的尺寸面积及增加后段对光工艺复杂度,同时在传统CMOS(互补金属氧化物半导体,英文全称Complementary Metal Oxide Semiconductor)工艺中的锗(Ge)探测器,光是由Si波导耦合到Ge探测器中,Ge探测器结构通常为垂直PIN结构,而此探测器结构并不适用于此专利的应用场景,其次对于传统CMOS工艺的Ge探测器,其饱和光电流都比较小,因此无法适用于高光功率的探测。Optical multiplexer (mux) and optical demultiplexer (demux) are one of the very important optical devices in optoelectronic chips at present. Considering the stability of optical multiplexer or optical demultiplexer, for example, it is affected by temperature and process. The optical multiplexer and the optical demultiplexer are caused by the shift of the center wavelength and the deformation of the spectral curve due to the conditions. We need to select suitable materials to prepare the optical multiplexer and the optical demultiplexer. Since the influence of the refractive index of silicon nitride (SiN) and silicon oxynitride (SiON) with temperature changes is much smaller than that of silicon (Si) materials, SiN or SiON are selected as materials for optical multiplexers and optical demultiplexers. In the application, the end of the optical multiplexer and the optical demultiplexer will be connected with the detector (PD) to realize photoelectric conversion. In ordinary optical module products, the optical multiplexer, the optical demultiplexer and the detector are in separate two The connection is realized by optical fiber (fiber) on each chip, which further increases the size and area of the product and increases the complexity of the back-end optical process. Germanium (Ge) detector, the light is coupled into the Ge detector by the Si waveguide, the Ge detector structure is usually a vertical PIN structure, and this detector structure is not suitable for the application scenario of this patent, followed by the traditional CMOS process. Ge detectors have relatively small saturation photocurrents, so they cannot be used for high optical power detection.

发明内容SUMMARY OF THE INVENTION

针对现有技术中存在的上述问题,现提供一种横向锗探测器结构及制备方法。In view of the above problems existing in the prior art, a lateral germanium detector structure and a preparation method are now provided.

具体技术方案如下:The specific technical solutions are as follows:

一种横向锗探测器结构,其中,所述横向锗探测器结构为横向光电二极管,具体包括:A lateral germanium detector structure, wherein the lateral germanium detector structure is a lateral photodiode, specifically comprising:

一硅衬底;a silicon substrate;

一硅氧化层,沉积于所述硅衬底的上表面;所述硅氧化层上包括:A silicon oxide layer is deposited on the upper surface of the silicon substrate; the silicon oxide layer includes:

一顶层硅;a top layer of silicon;

一锗层,形成于所述顶层硅的上表面,所述锗层包括锗层主体,以及由所述锗层主体分别向两侧延伸的第一延伸部与第二延伸部,于所述第一延伸部与所述第二延伸部分别形成一第一掺杂区域与一第二掺杂区域,于所述第一掺杂区域与所述第二掺杂区域的上表面分别形成一第一电极与一第二电极,所述第一电极与所述第二电极分别向上延伸出所述硅氧化层;A germanium layer is formed on the upper surface of the top layer silicon, the germanium layer includes a germanium layer main body, and a first extension portion and a second extension portion extending from the germanium layer main body to two sides respectively. An extension portion and the second extension portion respectively form a first doped region and a second doped region, and a first doped region is respectively formed on the upper surface of the first doped region and the second doped region an electrode and a second electrode, the first electrode and the second electrode respectively extend upward from the silicon oxide layer;

一氮化硅波导,形成于所述锗层的上方,所述氮化硅波导为锥形结构,所述氮化硅波导具有一第一端与一第二端,所述第一端小于所述第二端,所述氮化硅波导用于接收光信号,并将所述光信号耦合至所述锗层,所述锗层用以接收所述光信号,并将所述光信号转换为电信号。A silicon nitride waveguide is formed above the germanium layer, the silicon nitride waveguide has a tapered structure, the silicon nitride waveguide has a first end and a second end, and the first end is smaller than the At the second end, the silicon nitride waveguide is used for receiving an optical signal and coupling the optical signal to the germanium layer, and the germanium layer is used for receiving the optical signal and converting the optical signal into electric signal.

优选的,所述锗层主体、所述第一延伸部以及所述第二延伸部形成一体成型的T型结构的所述锗层。Preferably, the germanium layer body, the first extension portion and the second extension portion form the germanium layer of an integrally formed T-shaped structure.

优选的,所述锗层主体、所述第一延伸部以及所述第二延伸部,全面覆盖所述顶层硅。Preferably, the germanium layer body, the first extension part and the second extension part fully cover the top layer silicon.

优选的,于所述第一掺杂区域掺杂N+离子,以形成一N+第一注入区域;Preferably, N+ ions are doped in the first doping region to form an N+ first implanting region;

于所述N+第一注入区域掺杂N++离子,以形成一N++第一注入区域。N++ ions are doped into the N+ first implanted region to form an N++ first implanted region.

优选的,于所述第二掺杂区域掺杂P+离子,以形成一P+第二注入区域;Preferably, the second doping region is doped with P+ ions to form a P+ second implanting region;

于所述P+第二注入区域掺杂P++离子,以形成一P++第二注入区域。P++ ions are doped into the P+ second implantation region to form a P++ second implantation region.

优选的,所述氮化硅波导的厚度至少为0.2um;Preferably, the thickness of the silicon nitride waveguide is at least 0.2um;

所述第一端的宽度为0.1-0.5um;The width of the first end is 0.1-0.5um;

所述第二端的宽度为0.5-1.5um。The width of the second end is 0.5-1.5um.

优选的,所述氮化硅波导与所述锗层之间的预设距离为0-0.2um。Preferably, the preset distance between the silicon nitride waveguide and the germanium layer is 0-0.2um.

一种横向锗探测器结构的制备方法,其特征在于,用于任意一项所述的横向锗探测器结构,所述横向锗探测器结构为横向光电二极管,包括:A method for preparing a lateral germanium detector structure, characterized in that it is used in any one of the lateral germanium detector structures, wherein the lateral germanium detector structure is a lateral photodiode, comprising:

提供一硅衬底,于所述硅衬底上依次形成一硅氧化层与一顶层硅;A silicon substrate is provided, and a silicon oxide layer and a top layer of silicon are sequentially formed on the silicon substrate;

所述制备方法具体包括:The preparation method specifically includes:

步骤S1、于所述顶层硅上沉积一硅氧化层,于所述硅氧化层上开设一工艺窗口,于所述工艺窗口内形成一锗层,所述锗层包括锗层主体,以及由所述锗层主体分别向两侧延伸的第一延伸部与第二延伸部;Step S1, depositing a silicon oxide layer on the top silicon layer, opening a process window on the silicon oxide layer, forming a germanium layer in the process window, the germanium layer comprising a germanium layer main body, and the a first extension part and a second extension part respectively extending to both sides of the germanium layer body;

步骤S2、于所述第一延伸部与所述第二延伸部分别进行掺杂,以形成一第一掺杂区域与一第二掺杂区域;Step S2, doping the first extension portion and the second extension portion respectively to form a first doping region and a second doping region;

步骤S3、于所述锗层上沉积一硅氧化层,于所述硅氧化层上形成一氮化硅波导,所述氮化硅波导为锥形结构,所述氮化硅波导具有一第一端与一第二端,所述第一端小于所述第二端;Step S3, depositing a silicon oxide layer on the germanium layer, forming a silicon nitride waveguide on the silicon oxide layer, the silicon nitride waveguide has a tapered structure, and the silicon nitride waveguide has a first end and a second end, the first end is smaller than the second end;

步骤S4、于所述氮化硅波导上沉积一硅氧化层,于所述硅氧化层上开设一第一接触孔与一第二接触孔,所述第一接触孔与所述第二接触孔分别位于所述第一掺杂区域与所述第二掺杂区域的上表面;Step S4, depositing a silicon oxide layer on the silicon nitride waveguide, opening a first contact hole and a second contact hole on the silicon oxide layer, the first contact hole and the second contact hole respectively located on the upper surfaces of the first doped region and the second doped region;

步骤S5、于所述第一接触孔与所述第二接触孔内分别填充金属,以形成一第一电极与一第二电极,所述第一电极与所述第二电极分别向上延伸出所述硅氧化层。Step S5 , filling the first contact hole and the second contact hole with metal respectively to form a first electrode and a second electrode, the first electrode and the second electrode respectively extend upwardly out of the hole. the silicon oxide layer.

优选的,所述锗层主体、所述第一延伸部以及所述第二延伸部形成一体成型的T型结构的所述锗层。Preferably, the germanium layer body, the first extension portion and the second extension portion form the germanium layer of an integrally formed T-shaped structure.

优选的,所述锗层主体、所述第一延伸部以及所述第二延伸部,全面覆盖所述顶层硅。Preferably, the germanium layer body, the first extension part and the second extension part fully cover the top layer silicon.

本发明的技术方案有益效果在于:横向锗探测器结构为横向光电二极管结构,通过改造锗层结构,并且对锗层的两侧分别进行掺杂,有效增强氮化硅波导耦合至锗探测器的耦合效率,可以实现光复用器与光解复用器与锗探测器的有效集成,并且相对于传统工艺的锗探测器,氮化硅耦合锗探测器还可以应用于高光功率及高带宽的光电探测领域中。The beneficial effect of the technical solution of the present invention is that the lateral germanium detector structure is a lateral photodiode structure, and by transforming the germanium layer structure and doping the two sides of the germanium layer respectively, the coupling of the silicon nitride waveguide to the germanium detector is effectively enhanced. The coupling efficiency can realize the effective integration of the optical multiplexer, the optical demultiplexer and the germanium detector. Compared with the traditional germanium detector, the silicon nitride coupled germanium detector can also be applied to high optical power and high bandwidth optoelectronics. in the detection field.

附图说明Description of drawings

参考所附附图,以更加充分的描述本发明的实施例。然而,所附附图仅用于说明和阐述,并不构成对本发明范围的限制。Embodiments of the present invention are described more fully with reference to the accompanying drawings. However, the accompanying drawings are for illustration and illustration only, and are not intended to limit the scope of the present invention.

图1为本发明中,关于横向锗探测器结构的一种较优实施例的整体结构示意图;FIG. 1 is a schematic diagram of the overall structure of a preferred embodiment of the lateral germanium detector structure in the present invention;

图2为本发明中,关于横向锗探测器结构的一种较优实施例的俯视结构图;FIG. 2 is a top plan view of a preferred embodiment of the lateral germanium detector structure in the present invention;

图3为本发明中,关于横向锗探测器结构的另一种较优实施例的整体结构示意图;3 is a schematic diagram of the overall structure of another preferred embodiment of the lateral germanium detector structure in the present invention;

图4为本发明中,关于横向锗探测器结构的制备方法的流程图。FIG. 4 is a flow chart of a method for fabricating a lateral germanium detector structure in the present invention.

具体实施方式Detailed ways

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有作出创造性劳动的前提下所获得的所有其他实施例,都属于本发明保护的范围。The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only a part of the embodiments of the present invention, but not all of the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by those of ordinary skill in the art without creative work fall within the protection scope of the present invention.

需要说明的是,在不冲突的情况下,本发明中的实施例及实施例中的特征可以相互组合。It should be noted that the embodiments of the present invention and the features of the embodiments may be combined with each other under the condition of no conflict.

下面结合附图和具体实施例对本发明作进一步说明,但不作为本发明的限定。The present invention will be further described below with reference to the accompanying drawings and specific embodiments, but it is not intended to limit the present invention.

本发明包括一种横向锗探测器结构,其中,横向锗探测器结构为横向光电二极管,具体包括:The present invention includes a lateral germanium detector structure, wherein the lateral germanium detector structure is a lateral photodiode, and specifically includes:

一硅衬底1;a silicon substrate 1;

一硅氧化层2,沉积于硅衬底1的上表面;硅氧化层2上包括:A silicon oxide layer 2 is deposited on the upper surface of the silicon substrate 1; the silicon oxide layer 2 includes:

一顶层硅20;a top layer of silicon 20;

一锗层21,形成于顶层硅20的上表面,锗层21包括锗层主体21,以及由锗层主体21分别向两侧延伸的第一延伸部210与第二延伸部211,于第一延伸部210与第二延伸部211分别形成一第一掺杂区域212与一第二掺杂区域213,于第一掺杂区域212与第二掺杂区域213的上表面分别形成一第一电极214与一第二电极214,第一电214与第二电极215分别向上延伸出硅氧化层2;A germanium layer 21 is formed on the upper surface of the top layer silicon 20. The germanium layer 21 includes a germanium layer main body 21, and a first extension portion 210 and a second extension portion 211 extending from the germanium layer main body 21 to two sides respectively. A first doped region 212 and a second doped region 213 are respectively formed on the extension portion 210 and the second extension portion 211 , and a first electrode is respectively formed on the upper surfaces of the first doped region 212 and the second doped region 213 214 and a second electrode 214, the first electrode 214 and the second electrode 215 respectively extend upward from the silicon oxide layer 2;

一氮化硅波导22,形成于锗层21的上方,氮化硅波导22为锥形结构,氮化硅波导22具有一第一端220与一第二端221,第一端220小于第二端221,氮化硅波导22用于接收光信号,并将光信号耦合至锗层21,锗层21用以接收光信号,并将光信号转换为电信号。A silicon nitride waveguide 22 is formed above the germanium layer 21. The silicon nitride waveguide 22 has a tapered structure. The silicon nitride waveguide 22 has a first end 220 and a second end 221. The first end 220 is smaller than the second end 220. At the end 221, the silicon nitride waveguide 22 is used for receiving the optical signal and coupling the optical signal to the germanium layer 21, and the germanium layer 21 is used for receiving the optical signal and converting the optical signal into an electrical signal.

通过上述横向锗探测器结构的技术方案,结合图1、2所示,横向锗探测器结构为横向光电二极管结构,硅氧化层2沉积于硅衬底1的上表面,硅氧化层2包括顶层硅20、锗层21及氮化硅波导22,其中,锗层21包括锗层主体21,以及由锗层主体21分别向两侧延伸的第一延伸部210与第二延伸部211,锗层主体21、第一延伸部210以及第二延伸部211形成一体成型的T型结构的锗层21,于第一延伸部210与第二延伸部211分别形成一第一掺杂区域212与一第二掺杂区域213,于第一掺杂区域212与第二掺杂区域213的上表面分别形成一第一电极214与一第二电极215,第一电214与第二电极215分别向上延伸出硅氧化层2;具体地,于第一掺杂区域212掺杂N+离子,以形成N+第一注入区域212a,于N+第一注入区域212a掺杂N++离子,以形成N++第一注入区域212b;于第二掺杂区域213掺杂P+离子,以形成P+第二注入区域213a,于P+第二注入区域213a掺杂P++离子,以形成P++第二注入区域213b;Through the technical solution of the above-mentioned lateral germanium detector structure, as shown in FIGS. 1 and 2 , the lateral germanium detector structure is a lateral photodiode structure, a silicon oxide layer 2 is deposited on the upper surface of the silicon substrate 1 , and the silicon oxide layer 2 includes a top layer The silicon 20, the germanium layer 21 and the silicon nitride waveguide 22, wherein the germanium layer 21 includes a germanium layer main body 21, and a first extension portion 210 and a second extension portion 211 extending from the germanium layer main body 21 to both sides respectively. The main body 21 , the first extension portion 210 and the second extension portion 211 form an integrally formed T-shaped germanium layer 21 , and a first doped region 212 and a first doped region are respectively formed in the first extension portion 210 and the second extension portion 211 . Two doped regions 213, a first electrode 214 and a second electrode 215 are respectively formed on the upper surfaces of the first doped region 212 and the second doped region 213, and the first electrode 214 and the second electrode 215 extend upward respectively Silicon oxide layer 2; Specifically, N+ ions are doped into the first doping region 212 to form an N+ first implant region 212a, and N+ ions are doped in the N+ first implant region 212a to form an N++ first implant region 212b; Doping P+ ions in the second doping region 213 to form a P+ second implanting region 213a, and doping P++ ions in the P+ second implanting region 213a to form a P++ second implanting region 213b;

进一步地,氮化硅波导22形成于锗层21的上方,其中,氮化硅波导22与锗层21之间的预设距离设置为0-0.2um,氮化硅波导22为锥形结构,氮化硅波导22的厚度t至少设置为0.2um,氮化硅波导22的第一端220的宽度设置为0.1-0.5um,氮化硅波导的22第二端221的宽度设置为0.5-1.5um,氮化硅波导22用于接收光信号,并将光信号耦合至锗层21,锗层21用以接收光信号,并将光信号转换为电信号;Further, the silicon nitride waveguide 22 is formed above the germanium layer 21, wherein the predetermined distance between the silicon nitride waveguide 22 and the germanium layer 21 is set to 0-0.2um, and the silicon nitride waveguide 22 has a tapered structure, The thickness t of the silicon nitride waveguide 22 is set to at least 0.2um, the width of the first end 220 of the silicon nitride waveguide 22 is set to 0.1-0.5um, and the width of the second end 221 of the silicon nitride waveguide 22 is set to 0.5-1.5 um, the silicon nitride waveguide 22 is used to receive the optical signal, and the optical signal is coupled to the germanium layer 21, and the germanium layer 21 is used to receive the optical signal and convert the optical signal into an electrical signal;

进一步地,通过改造锗层结构,并且对锗层的两侧分别进行掺杂,有效增强氮化硅波导耦合至锗探测器的耦合效率,可以实现光复用器与光解复用器与锗探测器的有效集成,并且相对于传统工艺的锗探测器,氮化硅耦合锗探测器还可以应用于高光功率及高带宽的光电探测领域中。Further, by modifying the structure of the germanium layer and doping the two sides of the germanium layer respectively, the coupling efficiency of the silicon nitride waveguide to the germanium detector can be effectively enhanced, and the optical multiplexer, the optical demultiplexer and the germanium detection can be realized. Compared with the traditional germanium detector, the silicon nitride coupled germanium detector can also be applied to the field of photodetection with high optical power and high bandwidth.

在一种较优的实施例中,如图3所示,锗层主体21、第一延伸部210以及第二延伸部211,全面覆盖顶层硅20,且于第一延伸部210与第二延伸部211分别形成一第一掺杂区域212与一第二掺杂区域213,于第一掺杂区域212与第二掺杂区域213的上表面分别形成一第一电极214与一第二电极215,第一电214与第二电极215分别向上延伸出硅氧化层2;具体地,于第一掺杂区域212掺杂N+离子,以形成N+第一注入区域212a,于N+第一注入区域212a掺杂N++离子,以形成N++第一注入区域212b;于第二掺杂区域213掺杂P+离子,以形成P+第二注入区域213a,于P+第二注入区域213a掺杂P++离子,以形成P++第二注入区域213b,通过改造锗层21结构,增强了氮化硅波导耦合至锗探测器的耦合效率,可以实现光复用器与光解复用器与锗探测器的有效集成,并且相对于传统工艺的锗探测器,氮化硅耦合锗探测器还可以应用于高光功率及高带宽的光电探测领域中。In a preferred embodiment, as shown in FIG. 3 , the germanium layer body 21 , the first extension part 210 and the second extension part 211 fully cover the top layer silicon 20 , and the first extension part 210 and the second extension part A first doped region 212 and a second doped region 213 are formed on the portion 211 respectively, and a first electrode 214 and a second electrode 215 are respectively formed on the upper surfaces of the first doped region 212 and the second doped region 213 , the first electrode 214 and the second electrode 215 extend upward from the silicon oxide layer 2 respectively; specifically, doping N+ ions in the first doping region 212 to form an N+ first implanting region 212a, and in the N+ first implanting region 212a Doping N++ ions to form the first N++ implantation region 212b; doping the second doping region 213 with P+ ions to form the P+ second implantation region 213a, and doping the P+ second implantation region 213a with P++ ions to form P++ In the second implantation region 213b, by modifying the structure of the germanium layer 21, the coupling efficiency of the silicon nitride waveguide to the germanium detector is enhanced, and the effective integration of the optical multiplexer, the optical demultiplexer and the germanium detector can be realized, and compared with that of the germanium detector. The traditional germanium detector and silicon nitride coupled germanium detector can also be used in the field of photodetection with high optical power and high bandwidth.

本发明还包括一种横向锗探测器结构的制备方法,应用于任意一项的横向锗探测器结构,其中,横向锗探测器结构为横向光电二极管,包括:The present invention also includes a method for preparing a lateral germanium detector structure, which is applied to any one of the lateral germanium detector structures, wherein the lateral germanium detector structure is a lateral photodiode, comprising:

提供一硅衬底1,于硅衬底1上依次形成一硅氧化层2与一顶层硅20;A silicon substrate 1 is provided, and a silicon oxide layer 2 and a top layer silicon 20 are sequentially formed on the silicon substrate 1;

制备方法具体包括:The preparation method specifically includes:

步骤S1、于顶层硅20上沉积一硅氧化层2,于硅氧化层2上开设一工艺窗口(在图中未示出),于工艺窗口(在图中未示出)内形成一锗层21,锗层21包括锗层主体21,以及由锗层主体21分别向两侧延伸的第一延伸部210与第二延伸部211;Step S1, depositing a silicon oxide layer 2 on the top layer silicon 20, opening a process window (not shown in the figure) on the silicon oxide layer 2, and forming a germanium layer in the process window (not shown in the figure) 21. The germanium layer 21 includes a germanium layer main body 21, and a first extension portion 210 and a second extension portion 211 extending from the germanium layer main body 21 to two sides respectively;

步骤S2、于第一延伸部210与第二延伸部211分别进行掺杂,以形成一第一掺杂区域212与一第二掺杂区域213;Step S2, doping the first extension portion 210 and the second extension portion 211 respectively to form a first doping region 212 and a second doping region 213;

步骤S3、于锗层21上沉积一硅氧化层2,于硅氧化层2上形成一氮化硅波导22,氮化硅波导22具有一第一端220与一第二端221,第一端220小于第二端221;Step S3, depositing a silicon oxide layer 2 on the germanium layer 21, forming a silicon nitride waveguide 22 on the silicon oxide layer 2, the silicon nitride waveguide 22 has a first end 220 and a second end 221, the first end 220 is smaller than the second end 221;

步骤S4、于氮化硅波导22上沉积一硅氧化层2,于硅氧化层2上开设一第一接触孔(在图中未示出)与一第二接触孔(在图中未示出),第一接触孔(在图中未示出)与第二接触孔(在图中未示出)分别位于第一掺杂区域212与第二掺杂区域213的上表面;Step S4, depositing a silicon oxide layer 2 on the silicon nitride waveguide 22, and opening a first contact hole (not shown in the figure) and a second contact hole (not shown in the figure) on the silicon oxide layer 2 ), the first contact hole (not shown in the figure) and the second contact hole (not shown in the figure) are respectively located on the upper surfaces of the first doped region 212 and the second doped region 213;

步骤S5、于第一接触孔(在图中未示出)与第二接触孔(在图中未示出)内分别填充金属,以形成一第一电极212与一第二电极213,第一电极212与第二电极213分别向上延伸出硅氧化层2。Step S5, respectively filling the first contact hole (not shown in the figure) and the second contact hole (not shown in the figure) with metal to form a first electrode 212 and a second electrode 213, the first The electrode 212 and the second electrode 213 extend upward from the silicon oxide layer 2 respectively.

具体地,横向锗探测器结构的制备方法适用于氮化硅耦合锗探测器结构,氮化硅耦合锗探测器结构为横向光电二极管结构,其制备工艺简单,如图4所示,首先提供硅衬底1,于硅衬底1上依次形成硅氧化层2与顶层硅20,其中,硅氧化层2为二氧化硅;于顶层硅20上沉积一硅氧化层2,于硅氧化层2上开设一工艺窗口(在图中未示出),于工艺窗口(在图中未示出)内形成一锗层21,锗层21包括锗层主体21,以及由锗层主体21分别向两侧延伸的第一延伸部210与第二延伸部211;于第一延伸部210与第二延伸部211分别进行掺杂,以形成一第一掺杂区域212与一第二掺杂区域213;Specifically, the preparation method of the lateral germanium detector structure is suitable for the silicon nitride coupled germanium detector structure, the silicon nitride coupled germanium detector structure is a lateral photodiode structure, and the preparation process is simple, as shown in FIG. Substrate 1, a silicon oxide layer 2 and a top layer silicon 20 are sequentially formed on the silicon substrate 1, wherein the silicon oxide layer 2 is silicon dioxide; a silicon oxide layer 2 is deposited on the top layer silicon 20, and on the silicon oxide layer 2 A process window (not shown in the figure) is opened, and a germanium layer 21 is formed in the process window (not shown in the figure). The extended first extension portion 210 and the second extension portion 211; the first extension portion 210 and the second extension portion 211 are respectively doped to form a first doped region 212 and a second doped region 213;

具体地,锗层主体21、第一延伸部210以及第二延伸部211形成一体成型的T型结构的锗层21,如图1所示;锗层主体21、第一延伸部210以及第二延伸部211,全面覆盖顶层硅20,如图3所示;其中,于第一掺杂区域212掺杂N+离子,以形成N+第一注入区域212a,于N+第一注入区域212a掺杂N++离子,以形成N++第一注入区域212b;于第二掺杂区域213掺杂P+离子,以形成P+第二注入区域213a,于P+第二注入区域213a掺杂P++离子,以形成P++第二注入区域213b;Specifically, the germanium layer body 21 , the first extension portion 210 and the second extension portion 211 form an integrally formed germanium layer 21 with a T-shaped structure, as shown in FIG. 1 ; the germanium layer body 21 , the first extension portion 210 and the second extension portion 211 The extension portion 211 fully covers the top layer silicon 20, as shown in FIG. 3; wherein, the first doping region 212 is doped with N+ ions to form the N+ first implanting region 212a, and the N+ first implanting region 212a is doped with N++ ions , to form the N++ first implantation region 212b; dope the second doping region 213 with P+ ions to form the P+ second implantation region 213a, and dope the P+ second implantation region 213a with P++ ions to form the P++ second implantation region 213b;

进一步地,于锗层21上沉积硅氧化层2,于硅氧化层2上形成氮化硅波导22,氮化硅波导22为锥形结构,氮化硅波导22具有一第一端220与一第二端221,第一端220小于第二端221,通过将氮化硅波导22设置为锥形结构,进一步增强了氮化硅波导22耦合至锗探测器的耦合效率;Further, a silicon oxide layer 2 is deposited on the germanium layer 21, and a silicon nitride waveguide 22 is formed on the silicon oxide layer 2. The silicon nitride waveguide 22 has a tapered structure, and the silicon nitride waveguide 22 has a first end 220 and a The second end 221, the first end 220 is smaller than the second end 221, by setting the silicon nitride waveguide 22 into a tapered structure, the coupling efficiency of the silicon nitride waveguide 22 to the germanium detector is further enhanced;

进一步地,于氮化硅波导22上沉积一硅氧化层2,于硅氧化层2上开设一第一接触孔(在图中未示出)与一第二接触孔(在图中未示出),第一接触孔(在图中未示出)与第二接触孔(在图中未示出)分别位于第一掺杂区域212与第二掺杂区域213的上表面;于第一接触孔(在图中未示出)与第二接触孔(在图中未示出)内分别填充金属,以形成一第一电极212与一第二电极213,第一电极212与第二电极213分别向上延伸出硅氧化层2。Further, a silicon oxide layer 2 is deposited on the silicon nitride waveguide 22, and a first contact hole (not shown in the figure) and a second contact hole (not shown in the figure) are opened on the silicon oxide layer 2 ), the first contact hole (not shown in the figure) and the second contact hole (not shown in the figure) are located on the upper surfaces of the first doped region 212 and the second doped region 213 respectively; The hole (not shown in the figure) and the second contact hole (not shown in the figure) are filled with metal respectively to form a first electrode 212 and a second electrode 213, the first electrode 212 and the second electrode 213 The silicon oxide layers 2 are respectively extended upward.

本发明的技术方案有益效果在于:横向锗探测器结构为横向光电二极管结构,通过改造锗层结构,并且对锗层的两侧分别进行掺杂,有效增强氮化硅波导耦合至锗探测器的耦合效率,可以实现光复用器与光解复用器与锗探测器的有效集成,并且相对于传统工艺的锗探测器,氮化硅耦合锗探测器还可以应用于高光功率及高带宽的光电探测领域中。The beneficial effect of the technical solution of the present invention is that the lateral germanium detector structure is a lateral photodiode structure, and by transforming the germanium layer structure and doping the two sides of the germanium layer respectively, the coupling of the silicon nitride waveguide to the germanium detector is effectively enhanced. The coupling efficiency can realize the effective integration of the optical multiplexer, the optical demultiplexer and the germanium detector. Compared with the traditional germanium detector, the silicon nitride coupled germanium detector can also be applied to high optical power and high bandwidth optoelectronics. in the detection field.

以上仅为本发明较佳的实施例,并非因此限制本发明的实施方式及保护范围,对于本领域技术人员而言,应当能够意识到凡运用本发明说明书及图示内容所作出的等同替换和显而易见的变化所得到的方案,均应当包含在本发明的保护范围内。The above are only preferred embodiments of the present invention, and are not intended to limit the embodiments and protection scope of the present invention. For those skilled in the art, they should be aware of the equivalent replacement and Solutions obtained by obvious changes shall all be included in the protection scope of the present invention.

Claims (10)

1. The utility model provides a horizontal germanium detector structure which characterized in that, horizontal germanium detector structure is horizontal photodiode, specifically includes:
a silicon substrate;
a silicon oxide layer deposited on the upper surface of the silicon substrate; the silicon oxide layer comprises thereon:
a top layer of silicon;
the germanium layer comprises a germanium layer main body, a first extension part and a second extension part, wherein the first extension part and the second extension part extend from the germanium layer main body to two sides respectively;
a silicon nitride waveguide formed over the germanium layer, the silicon nitride waveguide having a tapered configuration, the silicon nitride waveguide having a first end and a second end, the first end being smaller than the second end, the silicon nitride waveguide being configured to receive an optical signal and couple the optical signal to the germanium layer, the germanium layer being configured to receive the optical signal and convert the optical signal to an electrical signal.
2. The lateral germanium detector structure of claim 1, wherein said germanium layer body, said first extension and said second extension form an integrally formed T-shaped structure of said germanium layer.
3. The lateral germanium detector structure of claim 1, wherein said germanium layer body, said first extension, and said second extension entirely cover said top layer of silicon.
4. The lateral germanium detector structure of claim 1, wherein said first doped region is doped with N + ions to form an N + first implanted region;
and doping N + + ions in the N + first injection region to form an N + + first injection region.
5. The lateral germanium detector structure of claim 1, wherein said second doped region is doped with P + ions to form a P + second implanted region;
and doping P + + ions in the P + second injection region to form a P + + second injection region.
6. The lateral germanium detector structure of claim 1, wherein said silicon nitride waveguide has a thickness of at least 0.2 um;
the width of the first end is 0.1-0.5 um;
the width of second end is 0.5-1.5 um.
7. The lateral germanium detector structure of claim 1, wherein the predetermined distance between the silicon nitride waveguide and the germanium layer is 0-0.2 um.
8. A method of manufacturing a lateral germanium detector structure for use in a lateral germanium detector structure according to any of claims 1-7, said lateral germanium detector structure being a lateral photodiode comprising:
providing a silicon substrate, and sequentially forming a silicon oxide layer and a top silicon layer on the silicon substrate;
the preparation method specifically comprises the following steps:
step S1, depositing a silicon oxide layer on the top silicon, opening a process window on the silicon oxide layer, and forming a germanium layer in the process window, wherein the germanium layer includes a germanium layer main body, and a first extension portion and a second extension portion that extend from the germanium layer main body to two sides, respectively;
step S2, doping the first extension portion and the second extension portion respectively to form a first doped region and a second doped region;
step S3, depositing a silicon oxide layer on the germanium layer, and forming a silicon nitride waveguide on the silicon oxide layer, where the silicon nitride waveguide has a tapered structure and has a first end and a second end, and the first end is smaller than the second end;
step S4, depositing a silicon oxide layer on the silicon nitride waveguide, forming a first contact hole and a second contact hole on the silicon oxide layer, where the first contact hole and the second contact hole are respectively located on the upper surfaces of the first doped region and the second doped region;
step S5, filling metal into the first contact hole and the second contact hole respectively to form a first electrode and a second electrode, wherein the first electrode and the second electrode extend upward to form the silicon oxide layer respectively.
9. The method of making a lateral germanium detector structure according to claim 8, wherein said germanium layer body, said first extension and said second extension form an integrally formed T-shaped structure of said germanium layer.
10. The method of claim 8, wherein the germanium layer body, the first extension, and the second extension entirely cover the top silicon.
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