CN110165012A - A kind of photodetector structure and preparation method thereof with the anti-reflection effect of arc - Google Patents
A kind of photodetector structure and preparation method thereof with the anti-reflection effect of arc Download PDFInfo
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Abstract
本发明为一种具有弧形增透作用的光电探测器结构及其制备方法。该结构沿着外延生长方向依次包括衬底、P型重掺杂材料层、N型轻掺杂材料层、N型过渡材料层、N型轻掺杂材料层、N型重掺杂材料层和N型欧姆电极;P型欧姆电极位于N型轻掺杂材料层外侧的P型重掺杂材料层上;其中,N型欧姆电极为圆环状,位于N型重掺杂材料层的外缘,其中间显露的N型重掺杂材料层为光敏区,厚度为0.1~1μm,所述的光敏区的上表面含有弧形结构,所述的弧形结构为弧形、叠弧形或凹凸形。本发明制备方法简单,可操作性强,成本低,而且在进一步增强透光率的同时,也会使入射到器件内部的光分布的更加均匀,降低器件自热效应,改善量子效率。
The invention relates to a photodetector structure with arc-shaped anti-reflection effect and a preparation method thereof. The structure sequentially includes a substrate, a P-type heavily doped material layer, an N-type lightly doped material layer, an N-type transition material layer, an N-type lightly doped material layer, an N-type heavily doped material layer and N-type ohmic electrode; P-type ohmic electrode is located on the P-type heavily doped material layer outside the N-type lightly doped material layer; wherein, the N-type ohmic electrode is circular and located on the outer edge of the N-type heavily doped material layer The N-type heavily doped material layer exposed in the middle is a photosensitive area with a thickness of 0.1-1 μm, and the upper surface of the photosensitive area contains an arc structure, and the arc structure is arc, overlapping arc, or concave-convex shape. The preparation method of the invention is simple, strong in operability and low in cost, and while further enhancing the light transmittance, the light incident into the device can be distributed more uniformly, the self-heating effect of the device can be reduced, and the quantum efficiency can be improved.
Description
技术领域technical field
本发明涉及一种具有弧形增透作用的光电探测器结构及其制备方法,尤其涉及一种高响应度雪崩光电探测器的制备方法,属于半导体光电子器件技术领域。The invention relates to a photodetector structure with an arc anti-reflection effect and a preparation method thereof, in particular to a preparation method of an avalanche photodetector with high responsivity, belonging to the technical field of semiconductor optoelectronic devices.
背景技术Background technique
紫外探测技术是继红外和激光探测技术之后发展起来的一项军民两用光电探测技术,而紫外探测器是紫外探测系统的核心元器件,在火灾监测、紫外固化、紫外消毒、医疗保健、国防预警、导弹告警等领域有着非常重要的应用前景。近年来,基于宽禁带半导体雪崩光电二极管(APD)的固态紫外探测器引起国际广泛的研究兴趣,旨在替代目前被大量使用的体积大、价格昂贵且易破碎的光电倍增管(PMT)。Ultraviolet detection technology is a military-civilian dual-use photoelectric detection technology developed after infrared and laser detection technology, and ultraviolet detector is the core component of ultraviolet detection system, in fire monitoring, ultraviolet curing, ultraviolet disinfection, medical care, national defense Early warning, missile warning and other fields have very important application prospects. In recent years, solid-state ultraviolet detectors based on wide-bandgap semiconductor avalanche photodiodes (APDs) have attracted widespread international research interest, aiming to replace the bulky, expensive, and fragile photomultiplier tubes (PMTs) that are currently widely used.
氮化镓(GaN)、碳化硅(SiC)APD因具有独特的材料和器件性能优势,是有望可以同时实现高增益、高量子效率、低暗电流、低过载噪声及微弱信号“可见光盲”紫外探测的半导体器件。常见的光电探测器结构有:金属-半导体-金属(MSM)结构、PN/PIN结构、雪崩光电探测器(APD)结构。无论采用何种器件结构,都希望提高器件的响应度来增加探测的灵敏度,基于此,研究人员做了一系列的研究,专利号为CN106784121A的中国专利公开了一种表面等离子激元光电探测器及其制备方法,其将金属电极做成叉指型的周期性光栅,利用金属光栅中自由电子的电荷密度波与入射电磁波产生耦合作用,导致电荷密度涨落,引发集体震荡,致使在不降低探测器响应速度的同时增加响应度;专利号为CN107275441A的中国专利公开了一种ZnO增透膜光电探测器的制备方法,其通过改变烧结温度、保温时间等参数制备出了结晶良好、光滑致密、性能优良的ZnO溅射靶材,以此来提高ZnO增透膜的透光率,增加响应度。尽管探测器响应度得到了一定程度的改善,但是以复杂的工艺程序和高昂的制备成本为代价。Gallium Nitride (GaN) and Silicon Carbide (SiC) APDs are expected to simultaneously achieve high gain, high quantum efficiency, low dark current, low overload noise, and weak signal "visible light blind" ultraviolet due to their unique material and device performance advantages. probed semiconductor devices. Common photodetector structures include: metal-semiconductor-metal (MSM) structure, PN/PIN structure, and avalanche photodetector (APD) structure. No matter what kind of device structure is used, it is hoped to improve the responsivity of the device to increase the detection sensitivity. Based on this, researchers have done a series of research. The Chinese patent No. CN106784121A discloses a surface plasmon photodetector and a preparation method thereof, wherein the metal electrode is made into an interdigitated periodic grating, and the charge density wave of free electrons in the metal grating is used to couple with the incident electromagnetic wave, causing the charge density to fluctuate and cause collective oscillation, so that the charge density wave does not decrease The response speed of the detector is increased while the responsivity is increased; the Chinese patent No. CN107275441A discloses a preparation method of a ZnO anti-reflection film photodetector, which prepares a well-crystallized, smooth and compact photodetector by changing the parameters such as sintering temperature and holding time. , ZnO sputtering target with excellent performance, so as to improve the light transmittance of ZnO anti-reflection coating and increase the responsivity. Although the detector responsivity has been improved to a certain extent, it is at the cost of complicated process procedures and high preparation costs.
发明内容Contents of the invention
本发明的目的为针对当前技术存在的不足,提供一种具有弧形增透作用的光电探测器结构及其制备方法。该结构通过将器件最顶部的光敏区刻蚀成弧形结构,增加透光率。本发明制备方法简单,可操作性强,成本低,而且在进一步增强透光率的同时,也会使入射到器件内部的光分布的更加均匀,避免光生载流子大量积聚,降低器件自热效应,改善量子效率。The object of the present invention is to provide a photodetector structure with arc-shaped anti-reflection effect and a preparation method thereof for the deficiencies in the current technology. This structure increases light transmittance by etching the photosensitive area at the top of the device into an arc-shaped structure. The preparation method of the invention is simple, has strong operability and low cost, and while further enhancing the light transmittance, it can also make the light distribution incident into the device more uniform, avoid a large amount of photogenerated carriers from accumulating, and reduce the self-heating effect of the device , to improve quantum efficiency.
本发明解决该技术问题所采用的技术方案是:The technical solution adopted by the present invention to solve the technical problem is:
一种具有弧形增透作用的光电探测器结构,该结构沿着外延生长方向依次包括衬底、P型重掺杂材料层、N型轻掺杂材料层、N型过渡材料层、N型轻掺杂材料层、N型重掺杂材料层和N型欧姆电极;P型欧姆电极位于N型轻掺杂材料层外侧的P型重掺杂材料层上;其中,N型欧姆电极为圆环状,位于N型重掺杂材料层的外缘,其中间显露的N型重掺杂材料层为光敏区,厚度为0.1~1μm,所述的光敏区的上表面含有弧形结构,所述的弧形结构为弧形、叠弧形或凹凸形,所述的弧形结构的投影面积占上表面面积的70%~100%。A photodetector structure with an arc-shaped anti-reflection effect, the structure sequentially includes a substrate, a P-type heavily doped material layer, an N-type lightly doped material layer, an N-type transition material layer, and an N-type Lightly doped material layer, N-type heavily doped material layer and N-type ohmic electrode; P-type ohmic electrode is located on the P-type heavily doped material layer outside the N-type lightly doped material layer; wherein, the N-type ohmic electrode is a circle Annular, located on the outer edge of the N-type heavily doped material layer, the N-type heavily doped material layer exposed in the middle is a photosensitive area with a thickness of 0.1-1 μm, and the upper surface of the photosensitive area contains an arc structure, so The arc-shaped structure is arc-shaped, overlapping arc-shaped or concave-convex-shaped, and the projected area of the arc-shaped structure accounts for 70%-100% of the upper surface area.
当上表面为弧形时,所述的弧度大于0,且小于π;优选为π/20~π/3之间;所述的弧形为内弧或外弧;When the upper surface is arc-shaped, the radian is greater than 0 and less than π; preferably between π/20 and π/3; the arc is an inner arc or an outer arc;
当上表面的形状为叠弧时,即相互交错的弧形结构,所述的弧度大于0,且小于2π;优选为π/6~π/2之间;相邻弧形结构重叠比例为10%~30%;When the shape of the upper surface is an overlapping arc, that is, an interlaced arc structure, the radian is greater than 0 and less than 2π; preferably between π/6 and π/2; the overlapping ratio of adjacent arc structures is 10 %~30%;
当上表面的形状为凹凸形时,即凹凸相切的弧形结构,所述的弧度大于0,且小于2π;优选为π/6~π/2之间;When the shape of the upper surface is concave-convex, that is, a concave-convex tangent arc structure, the radian is greater than 0 and less than 2π; preferably between π/6 and π/2;
所述的衬底、P型重掺杂材料层均为圆台状,半径相同;The substrate and the P-type heavily doped material layer are all in the shape of a truncated cone with the same radius;
所述的N型轻掺杂材料层、N型过渡材料层、N型轻掺杂材料层、N型重掺杂材料层整体呈截面为梯形的圆台;梯形内角范围位于4°~30°之间;The N-type lightly doped material layer, the N-type transition material layer, the N-type lightly doped material layer, and the N-type heavily doped material layer have a trapezoidal cross-section as a whole; the internal angle range of the trapezoid is between 4° and 30° between;
所述的N型轻掺杂材料层占P型重掺杂材料层面积的60%~95%;The N-type lightly doped material layer accounts for 60% to 95% of the area of the P-type heavily doped material layer;
所述的P型欧姆电极的宽度占P型重掺杂材料层曝露出宽度的10%~90%;The width of the P-type ohmic electrode accounts for 10% to 90% of the exposed width of the P-type heavily doped material layer;
所述的N型欧姆电极的宽度占N型重掺杂材料层半径的2%~20%;The width of the N-type ohmic electrode accounts for 2% to 20% of the radius of the N-type heavily doped material layer;
所述衬底的材质为4H-SiC、蓝宝石、Si或GaN;The material of the substrate is 4H-SiC, sapphire, Si or GaN;
所述P型重掺杂材料层的材质为SiC、GaO、Ala1Inb1Ga1-a1-b1As或Alx1Iny1Ga1-x1-y1N,式中各元素的组分0≤a1≤1,0≤b1≤1,0≤1-a1-b1,0≤x1≤1,0≤y1≤1,0≤1-x1-y1,厚度为1~4μm,掺杂浓度为1×1017cm-3~1×1020cm-3;The material of the P-type heavily doped material layer is SiC, GaO, Al a1 In b1 Ga 1-a1-b1 As or Al x1 In y1 Ga 1-x1-y1 N, and the composition of each element in the formula is 0≤a1 ≤1,0≤b1≤1,0≤1-a1-b1,0≤x1≤1,0≤y1≤1,0≤1-x1-y1, thickness 1~4μm, doping concentration 1×10 17 cm -3 ~1×10 20 cm -3 ;
所述N型轻掺杂材料层的材质为SiC、GaO、Ala2Inb2Ga1-a2-b2As或Alx2Iny2Ga1-x2-y2N,式中各元素的组分0≤a2≤1,0≤b2≤1,0≤1-a2-b2,0≤x2≤1,0≤y2≤1,0≤1-x2-y2,厚度为0.1~2μm,掺杂浓度为5×1014cm-3~1×1017cm-3;The material of the N-type lightly doped material layer is SiC, GaO, Al a2 In b2 Ga 1-a2-b2 As or Al x2 In y2 Ga 1-x2-y2 N, and the composition of each element in the formula is 0≤a2 ≤1,0≤b2≤1,0≤1-a2-b2,0≤x2≤1,0≤y2≤1,0≤1-x2-y2, thickness 0.1~2μm, doping concentration 5×10 14 cm -3 ~1×10 17 cm -3 ;
所述N型过渡材料层的材质为SiC、GaO、Ala3Inb3Ga1-a3-b3As或Alx3Iny3Ga1-x3-y3N,式中各元素的组分0≤a3≤1,0≤b3≤1,0≤1-a3-b3,0≤x3≤1,0≤y3≤1,0≤1-x3-y3,厚度为0.1~2μm,掺杂浓度为1×1017cm-3~5×1018cm-3;The material of the N-type transition material layer is SiC, GaO, Al a3 In b3 Ga 1-a3-b3 As or Al x3 In y3 Ga 1-x3-y3 N, and the composition of each element in the formula is 0≤a3≤1 ,0≤b3≤1,0≤1-a3-b3,0≤x3≤1,0≤y3≤1,0≤1-x3-y3, thickness is 0.1~2μm, doping concentration is 1×10 17 cm -3 ~5×10 18 cm -3 ;
所述N型轻掺杂材料层的材质为SiC、GaO、Ala4Inb4Ga1-a4-b4As或Alx4Iny4Ga1-x4-y4N,式中各元素的组分0≤a4≤1,0≤b4≤1,0≤1-a4-b4,0≤x4≤1,0≤y4≤1,0≤1-x4-y4,厚度为0.1~2μm,掺杂浓度为5×1014cm-3~1×1017cm-3;The material of the N-type lightly doped material layer is SiC, GaO, Al a4 In b4 Ga 1-a4-b4 As or Al x4 In y4 Ga 1-x4-y4 N, and the composition of each element in the formula is 0≤a4 ≤1,0≤b4≤1,0≤1-a4-b4,0≤x4≤1,0≤y4≤1,0≤1-x4-y4, thickness 0.1~2μm, doping concentration 5×10 14 cm -3 ~1×10 17 cm -3 ;
所述N型重掺杂材料层的材质为SiC、GaO、Ala5Inb5Ga1-a5-b5As或Alx5Iny5Ga1-x5-y5N,式中各元素的组分0≤a5≤1,0≤b5≤1,0≤1-a5-b5,0≤x5≤1,0≤y5≤1,0≤1-x5-y5,厚度为0.1~1μm,掺杂浓度为1×1017cm-3~1×1020cm-3;The material of the N-type heavily doped material layer is SiC, GaO, Al a5 In b5 Ga 1-a5-b5 As or Al x5 In y5 Ga 1-x5-y5 N, and the composition of each element in the formula is 0≤a5 ≤1,0≤b5≤1,0≤1-a5-b5,0≤x5≤1,0≤y5≤1,0≤1-x5-y5, thickness 0.1~1μm, doping concentration 1×10 17 cm -3 ~1×10 20 cm -3 ;
所述N型欧姆电极的材质为Cr/Au或Ti/Au;The material of the N-type ohmic electrode is Cr/Au or Ti/Au;
所述P型欧姆电极的材质为Cr/Au或Ni/Au。The material of the P-type ohmic electrode is Cr/Au or Ni/Au.
所述的具有弧形增透作用的光电探测器结构的制备方法,该方法包括如下步骤:The preparation method of the photodetector structure with arc-shaped anti-reflection effect, the method comprises the following steps:
第一步,在超声中依次使用丙酮、无水乙醇、去离子水对衬底进行清洗,生长面朝上,每次超声清洗5~10分钟;The first step is to use acetone, absolute ethanol, and deionized water to clean the substrate in sequence in the ultrasonic wave, with the growth side facing upward, and ultrasonic cleaning for 5 to 10 minutes each time;
第二步,在MOCVD或者MBE反应炉中,在第一步处理后的衬底表面上依次外延生长厚度为1~4μm的P型重掺杂材料层、厚度为0.1~2μm的N型轻掺杂材料层、厚度为0.1~2μm的N型过渡材料层、厚度为0.1~2μm的N型轻掺杂材料层、厚度为0.1~1μm的N型重掺杂材料层;In the second step, in the MOCVD or MBE reactor, a P-type heavily doped material layer with a thickness of 1-4 μm and an N-type lightly doped material layer with a thickness of 0.1-2 μm are epitaxially grown on the surface of the substrate after the first step. Miscellaneous material layer, N-type transition material layer with a thickness of 0.1-2 μm, N-type lightly doped material layer with a thickness of 0.1-2 μm, N-type heavily doped material layer with a thickness of 0.1-1 μm;
第三步,在第二步得到的N型重掺杂材料层上,通过光刻胶变温回流技术和干法刻蚀工艺制作锥形台面,曝露出P型重掺杂材料层,其中,梯形倾斜台面内角范围位于4°~30°之间,刻蚀后的N型轻掺杂材料层占P型重掺杂材料层面积的60%~95%;In the third step, on the N-type heavily doped material layer obtained in the second step, a tapered mesa is fabricated through photoresist variable temperature reflow technology and dry etching process, exposing the P-type heavily doped material layer, wherein the trapezoidal The inner angle range of the inclined mesa is between 4° and 30°, and the etched N-type lightly doped material layer accounts for 60% to 95% of the area of the P-type heavily doped material layer;
第四步,在第三步得到台面上方蒸镀制备N型欧姆电极,在曝露出P型重掺杂材料层上方蒸镀制备P型欧姆电极;In the fourth step, an N-type ohmic electrode is prepared by evaporation above the mesa in the third step, and a P-type ohmic electrode is prepared by evaporation above the exposed P-type heavily doped material layer;
第五步,对于第四步N型重掺杂材料层制备完N型欧姆电极剩余的光敏区,通过光刻和干法刻蚀制作弧形图案化形状;The fifth step is to prepare the remaining photosensitive area of the N-type ohmic electrode for the N-type heavily doped material layer in the fourth step, and make an arc-shaped patterned shape by photolithography and dry etching;
由此得到所述的一种具有弧形增透作用的光电探测器结构。Thus, the above-mentioned photodetector structure with arc-shaped anti-reflection effect is obtained.
本发明的实质性特点为:Substantive features of the present invention are:
传统外延结构的光敏区是平面结构,光源入射到平面会有一部分光反射到空气中未进入到器件内部,最终只有少部分光入射到器件内部,导致光响应度不佳,严重制约探测器的灵敏度;而本发明外延结构的光敏区是弧形结构,根据菲涅尔定律可知,入射光的临界角减小,会减小光的反射率,导致入射到器件内部的光大量增加,并且此结构会使入射到器件内部的光分布的更加均匀,避免光生载流子大量积聚,光响应度和量子效率得到有效地改善。The photosensitive area of the traditional epitaxial structure is a planar structure. When the light source is incident on the plane, part of the light will be reflected into the air and not enter the device. In the end, only a small part of the light will enter the device, resulting in poor photoresponsivity and severely restricting the detector. Sensitivity; while the photosensitive region of the epitaxial structure of the present invention is an arc structure, according to Fresnel's law, the critical angle of incident light decreases, which will reduce the reflectivity of light, resulting in a large increase of light incident into the device interior, and this The structure can make the distribution of light incident into the device more uniform, avoid a large accumulation of photogenerated carriers, and effectively improve the photoresponsivity and quantum efficiency.
本发明的有益效果是:The beneficial effects of the present invention are:
(1)本发明光电探测器外延结构是将N型欧姆电极之间的光敏区刻蚀成弧形结构,根据菲涅尔定律,尽可能的减小入射光的临界角,能够减小光的反射概率,这样可以使更多的光进入到器件内部,致使入射光的透射率增加10%~50%,从而提高器件的光响应度10%~50%,以致于微弱光源信号都可敏感地探测到。(1) The epitaxial structure of the photodetector of the present invention is that the photosensitive area between the N-type ohmic electrodes is etched into an arc structure. According to Fresnel's law, the critical angle of the incident light can be reduced as much as possible, and the light intensity can be reduced. Reflection probability, so that more light can enter the interior of the device, resulting in an increase in the transmittance of incident light by 10% to 50%, thereby increasing the photoresponsivity of the device by 10% to 50%, so that weak light source signals can be sensitively detected.
(2)本发明利用光敏区的弧形结构,会使入射到器件内部的光分布更加均匀,则光生载流子可以均匀地分布在器件增益区中,避免了光生载流子拥挤产生器件自热效应,同时更多的载流子产生增益,致使量子效率增加10%~50%。(2) The present invention utilizes the arc-shaped structure of the photosensitive region to make the distribution of light incident into the device more uniform, and the photogenerated carriers can be evenly distributed in the gain region of the device, which avoids the photogenerated carrier crowding and the generation of device self-sufficiency. Thermal effects, and more carriers generate gain at the same time, resulting in an increase in quantum efficiency of 10% to 50%.
(3)本发明方法可操作性强,成本低,工艺简单可靠,适于工业上的推广使用。(3) The method of the present invention has strong operability, low cost, simple and reliable process, and is suitable for popularization and use in industry.
本发明一种具有弧形增透作用的光电探测器结构专门适用于光电子半导体器件,尤其适用于III-V族宽禁带半导体光电二极管。The photodetector structure with arc-shaped anti-reflection effect of the invention is specially suitable for optoelectronic semiconductor devices, especially suitable for III-V wide bandgap semiconductor photodiodes.
附图说明Description of drawings
图1为现有技术中标准的光电探测器的外延结构侧剖示意图,即不具备弧形增透结构。FIG. 1 is a schematic side sectional view of an epitaxial structure of a standard photodetector in the prior art, that is, it does not have an arc-shaped anti-reflection structure.
图2为本发明具有弧形增透作用的光电探测器结构一种实施例的结构侧剖示意图。FIG. 2 is a schematic side cross-sectional view of an embodiment of a photodetector structure with an arc-shaped anti-reflection function according to the present invention.
图3为实施例1标准光电探测器外延生长完P型重掺杂材料层、N型轻掺杂材料层、N型过渡材料层、N型轻掺杂材料层和N型重掺杂材料层后的结构侧剖示意图。Fig. 3 is the epitaxially grown P-type heavily doped material layer, N-type lightly doped material layer, N-type transition material layer, N-type lightly doped material layer and N-type heavily doped material layer for the standard photodetector in Example 1 Schematic diagram of the rear structure.
图4为实施例1的图3所示制品,通过光刻胶变温回流技术,刻蚀出倾斜台面后的结构侧剖示意图。FIG. 4 is a schematic side sectional view of the product shown in FIG. 3 of Example 1, after the inclined mesa is etched by the photoresist variable temperature reflow technology.
图5为实施例1中采用的一种弧形增透作用的光电探测器结构俯视示意图。FIG. 5 is a schematic top view of the structure of an arc-shaped anti-reflection photodetector used in Embodiment 1. FIG.
图6为实施例1中传统平面外延结构和具有一种弧形增透作用的光电探测器结构的光强分布图;其中图6a为传统平面外延结构光电探测器结构的光强分布图;图6b为实施例1中具有一种弧形增透作用的光电探测器结构的光强分布图;Fig. 6 is the light intensity distribution diagram of the traditional planar epitaxial structure and the photodetector structure with a kind of arc-shaped anti-reflection effect in embodiment 1; Wherein Fig. 6 a is the light intensity distribution diagram of the traditional planar epitaxial structure photodetector structure; Fig. 6b is a light intensity distribution diagram of a photodetector structure having an arc-shaped anti-reflection effect in embodiment 1;
图7为实施例2中采用的一种弧形增透作用的光电探测器结构侧剖示意图。FIG. 7 is a schematic side sectional view of the structure of an arc-shaped anti-reflection photodetector used in Embodiment 2. FIG.
图8为实施例2中采用的一种弧形增透作用的光电探测器结构俯视示意图。FIG. 8 is a schematic top view of the structure of an arc-shaped anti-reflection photodetector used in Embodiment 2. FIG.
图9为实施例3中采用的一种弧形增透作用的光电探测器结构侧剖示意图。FIG. 9 is a schematic side sectional view of the structure of an arc-shaped anti-reflection photodetector used in Embodiment 3. FIG.
其中,101.衬底,102.P型重掺杂材料层,103.N型轻掺杂材料层,104.N型过渡材料层,105.N型轻掺杂材料层,106.N型重掺杂材料层,107.P型欧姆电极,108.N型欧姆电极。Among them, 101. Substrate, 102. P-type heavily doped material layer, 103. N-type lightly doped material layer, 104. N-type transition material layer, 105. N-type lightly doped material layer, 106. N-type heavily doped material layer Doped material layer, 107. P-type ohmic electrode, 108. N-type ohmic electrode.
具体实施方式Detailed ways
下面结合实施例及附图对本发明作进一步说明,但并不以此作为对本申请权利要求保护范围的限定。The present invention will be further described below in conjunction with the embodiments and accompanying drawings, but this should not be used as a limitation to the protection scope of the claims of the present application.
本发明一种具有弧形增透作用的光电探测器结构(简称外延结构,参见图2)沿着外延生长方向依次包括衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106、N型欧姆电极108和P型欧姆电极107;所述N型重掺杂材料层106为光敏区,厚度为0.1~1μm,根据不同的器件结构设计需求,上表面形状为弧形(弧度大于0,且小于2π,优选为π/6~3π/2之间)、叠弧形、凹凸形等具有弧面结构的不规则图案。A photodetector structure (abbreviated as an epitaxial structure, see FIG. 2 ) with an arc-shaped anti-reflection effect of the present invention includes a substrate 101, a P-type heavily doped material layer 102, and an N-type lightly doped material in sequence along the epitaxial growth direction. Layer 103, N-type transition material layer 104, N-type lightly doped material layer 105, N-type heavily doped material layer 106, N-type ohmic electrode 108 and P-type ohmic electrode 107; the N-type heavily doped material layer 106 It is a photosensitive area with a thickness of 0.1-1μm. According to different device structure design requirements, the shape of the upper surface is arc-shaped (the arc is greater than 0 and less than 2π, preferably between π/6-3π/2), superimposed arc, Irregular patterns with curved surface structures such as concave and convex shapes.
本发明外延结构所述衬底101的材质可以是但不局限于4H-SiC、蓝宝石、Si或GaN;The material of the substrate 101 in the epitaxial structure of the present invention may be but not limited to 4H-SiC, sapphire, Si or GaN;
所述的衬底、P型重掺杂材料层均为圆台状,半径相同;The substrate and the P-type heavily doped material layer are all in the shape of a truncated cone with the same radius;
所述的N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106呈锥形圆台(通过中心的截面为梯形);梯形内角范围位于4°~30°之间;The N-type lightly doped material layer 103, the N-type transition material layer 104, the N-type lightly doped material layer 105, and the N-type heavily doped material layer 106 are in the shape of a conical cone (the section through the center is trapezoidal); trapezoidal The inner angle range is between 4° and 30°;
所述的P型欧姆电极107占P型重掺杂材料层102曝露出宽度的10%~90%;(说明,即圆环状P型欧姆电极107内外沿的距离,除以(P型重掺杂材料层102的半径-N型轻掺杂材料层103的半径)所得到的比例)The P-type ohmic electrode 107 accounts for 10% to 90% of the exposed width of the P-type heavily doped material layer 102; The radius of the dopant material layer 102-the radius of the N-type lightly doped material layer 103) obtained ratio)
所述的N型欧姆电极108的宽度(即内外沿的距离)占N型重掺杂材料层106半径的2%~20%;The width of the N-type ohmic electrode 108 (that is, the distance between the inner and outer edges) accounts for 2% to 20% of the radius of the N-type heavily doped material layer 106;
本发明外延结构所述P型重掺杂材料层102的材质为SiC、GaO、Ala1Inb1Ga1-a1-b1As或Alx1Iny1Ga1-x1-y1N,式中各元素的组分0≤a1≤1,0≤b1≤1,0≤1-a1-b1,0≤x1≤1,0≤y1≤1,0≤1-x1-y1,厚度为1~4μm,掺杂浓度为1×1017cm-3~1×1020cm-3;The material of the P-type heavily doped material layer 102 in the epitaxial structure of the present invention is SiC, GaO, Al a1 In b1 Ga 1-a1-b1 As or Al x1 In y1 Ga 1-x1-y1 N, where each element Composition 0≤a1≤1,0≤b1≤1,0≤1-a1-b1,0≤x1≤1,0≤y1≤1,0≤1-x1-y1, thickness 1~4μm, doped The concentration is 1×10 17 cm -3 ~1×10 20 cm -3 ;
本发明外延结构所述N型轻掺杂材料层103的材质为SiC、GaO、Ala2Inb2Ga1-a2-b2As或Alx2Iny2Ga1-x2-y2N,式中各元素的组分0≤a2≤1,0≤b2≤1,0≤1-a2-b2,0≤x2≤1,0≤y2≤1,0≤1-x2-y2,厚度为0.1~2μm,掺杂浓度为5×1014cm-3~1×1017cm-3;The material of the N-type lightly doped material layer 103 in the epitaxial structure of the present invention is SiC, GaO, Al a2 In b2 Ga 1-a2-b2 As or Al x2 In y2 Ga 1-x2-y2 N, where each element Composition 0≤a2≤1,0≤b2≤1,0≤1-a2-b2,0≤x2≤1,0≤y2≤1,0≤1-x2-y2, thickness 0.1~2μm, doped The concentration is 5×10 14 cm -3 ~1×10 17 cm -3 ;
本发明外延结构所述N型过渡材料层104的材质为SiC、GaO、Ala3Inb3Ga1-a3-b3As或Alx3Iny3Ga1-x3-y3N,式中各元素的组分0≤a3≤1,0≤b3≤1,0≤1-a3-b3,0≤x3≤1,0≤y3≤1,0≤1-x3-y3,厚度为0.1~2μm,掺杂浓度为1×1017cm-3~5×1018cm-3;The material of the N-type transition material layer 104 in the epitaxial structure of the present invention is SiC, GaO, Al a3 In b3 Ga 1-a3-b3 As or Al x3 In y3 Ga 1-x3-y3 N, the composition of each element in the formula 0≤a3≤1,0≤b3≤1,0≤1-a3-b3,0≤x3≤1,0≤y3≤1,0≤1-x3-y3, thickness is 0.1~2μm, doping concentration is 1×10 17 cm -3 ~5×10 18 cm -3 ;
本发明外延结构所述N型轻掺杂材料层105的材质为SiC、GaO、Ala4Inb4Ga1-a4-b4As或Alx4Iny4Ga1-x4-y4N,式中各元素的组分0≤a4≤1,0≤b4≤1,0≤1-a4-b4,0≤x4≤1,0≤y4≤1,0≤1-x4-y4,厚度为0.1~2μm,掺杂浓度为5×1014cm-3~1×1017cm-3;The material of the N-type lightly doped material layer 105 in the epitaxial structure of the present invention is SiC, GaO, Al a4 In b4 Ga 1-a4-b4 As or Al x4 In y4 Ga 1-x4-y4 N, the elements in the formula Composition 0≤a4≤1,0≤b4≤1,0≤1-a4-b4,0≤x4≤1,0≤y4≤1,0≤1-x4-y4, thickness 0.1~2μm, doped The concentration is 5×10 14 cm -3 ~1×10 17 cm -3 ;
本发明外延结构所述N型重掺杂材料层106的材质为SiC、GaO、Ala5Inb5Ga1-a5-b5As或Alx5Iny5Ga1-x5-y5N,式中各元素的组分0≤a5≤1,0≤b5≤1,0≤1-a5-b5,0≤x5≤1,0≤y5≤1,0≤1-x5-y5,厚度为0.1~1μm,掺杂浓度为1×1017cm-3~1×1020cm-3;The material of the N-type heavily doped material layer 106 in the epitaxial structure of the present invention is SiC, GaO, Al a5 In b5 Ga 1-a5-b5 As or Al x5 In y5 Ga 1-x5-y5 N, and the elements in the formula Composition 0≤a5≤1,0≤b5≤1,0≤1-a5-b5,0≤x5≤1,0≤y5≤1,0≤1-x5-y5, thickness 0.1~1μm, doped The concentration is 1×10 17 cm -3 ~1×10 20 cm -3 ;
所述N型欧姆电极108的材质为Cr/Au或Ti/Au;The material of the N-type ohmic electrode 108 is Cr/Au or Ti/Au;
所述P型欧姆电极107的材质为Cr/Au或Ni/Au。The material of the P-type ohmic electrode 107 is Cr/Au or Ni/Au.
本发明一种具有弧形增透作用的光电探测器结构的制备方法,该方法的步骤如下:A kind of preparation method of the photodetector structure with arc anti-reflection effect of the present invention, the steps of this method are as follows:
第一步,在超声中依次使用丙酮、无水乙醇、去离子水对衬底进行清洗,生长面朝上,每次超声清洗5~10分钟,以除掉附着在衬底101表面的异物;In the first step, the substrate is cleaned with acetone, absolute ethanol, and deionized water sequentially in ultrasound, with the growth side facing up, and ultrasonic cleaning is performed for 5 to 10 minutes each time to remove foreign matter attached to the surface of the substrate 101;
第二步,在MOCVD或者MBE反应炉中,在第一步处理后的衬底表面上依次外延生长厚度为1~4μm、掺杂浓度为1×1017cm-3~1×1020cm-3的P型重掺杂材料层102,厚度为0.1~2μm、掺杂浓度为5×1014cm-3~1×1017cm-3的N型轻掺杂材料层103,厚度为0.1~2μm、掺杂浓度为1×1017cm-3~5×1018cm-3的N型过渡材料层104,厚度为0.1~2μm、掺杂浓度为5×1014cm-3~1×1017cm-3的N型轻掺杂材料层105,厚度为0.1~1μm、掺杂浓度为1×1017cm-3~1×1020cm-3的N型重掺杂材料层106;In the second step, in the MOCVD or MBE reactor, on the surface of the substrate treated in the first step, epitaxial growth with a thickness of 1-4 μm and a doping concentration of 1×10 17 cm -3 to 1×10 20 cm - 3 P-type heavily doped material layer 102 with a thickness of 0.1-2 μm, and an N - type lightly doped material layer 103 with a thickness of 0.1-2 μm with a doping concentration of 5×10 14 cm −3 to 1×10 17 cm N - type transition material layer 104 with a thickness of 0.1 to 2 μm and a doping concentration of 5×10 14 cm -3 to 1 ×10 An N-type lightly doped material layer 105 with a thickness of 17 cm- 3 , an N-type heavily doped material layer 106 with a thickness of 0.1-1 μm and a doping concentration of 1×10 17 cm -3 to 1×10 20 cm -3 ;
第三步,在第二步得到的N型重掺杂材料层106上,通过光刻胶变温回流技术和干法刻蚀工艺制作倾斜台面,曝露出P型重掺杂材料层102,其中,梯形倾斜台面内角范围位于4°~30°之间,刻蚀后的N型轻掺杂材料层103占P型重掺杂材料层102面积的60%~95%;In the third step, on the N-type heavily doped material layer 106 obtained in the second step, an inclined mesa is fabricated by photoresist variable temperature reflow technology and dry etching process, exposing the P-type heavily doped material layer 102, wherein, The inner angle range of the trapezoidal inclined mesa is between 4° and 30°, and the etched N-type lightly doped material layer 103 accounts for 60% to 95% of the area of the P-type heavily doped material layer 102;
第四步,在第三步得到台面N型重掺杂材料层106上方蒸镀制备N型欧姆电极108,在曝露出P型重掺杂材料层102上方蒸镀制备P型欧姆电极107;The fourth step is to prepare an N-type ohmic electrode 108 by evaporation on the N-type heavily doped material layer 106 obtained in the third step, and prepare a P-type ohmic electrode 107 by evaporation on the exposed P-type heavily doped material layer 102;
第五步,对于第四步N型重掺杂材料层106制备完N型欧姆电极108剩余的光敏区,通过光刻和干法刻蚀制作弧形图案化形状,根据不同的器件结构设计需求,上表面形状为弧形(弧度大于0,且小于2π,优选为π/6~3π/2之间)、叠弧形、凹凸形等具有弧面结构的不规则图案;The fifth step is to prepare the remaining photosensitive area of the N-type ohmic electrode 108 for the N-type heavily doped material layer 106 in the fourth step, and make an arc-shaped patterned shape by photolithography and dry etching, according to different device structure design requirements , the shape of the upper surface is arc-shaped (the radian is greater than 0 and less than 2π, preferably between π/6 and 3π/2), overlapping arcs, concave-convex shapes and other irregular patterns with arc-shaped structures;
由此得到所述的一种具有弧形增透作用的光电探测器结构。Thus, the above-mentioned photodetector structure with arc-shaped anti-reflection effect is obtained.
经过我们研究发现,由于探测光源大多数不是平行光源,那么平面结构会存在严重的反射现象,若把探测器件光敏区做成弧形结构,根据菲涅尔定律,会大大增加透光率,从而省去制备增透膜复杂工艺步骤。After our research, we found that since most of the detection light sources are not parallel light sources, there will be serious reflections in the planar structure. If the photosensitive area of the detection device is made into an arc structure, according to Fresnel's law, the light transmittance will be greatly increased, thereby The complex process steps of preparing the anti-reflection film are omitted.
本发明利用具有弧形增透结构来减小入射光的临界角,减小反射率,增加光源的透射率,从而增强器件的光响应度,来提高探测器对于微弱信号光源的探测能力。The invention utilizes the arc-shaped anti-reflection structure to reduce the critical angle of incident light, reduce the reflectivity, and increase the transmittance of the light source, thereby enhancing the light responsivity of the device and improving the detector's ability to detect weak signal light sources.
图1为现有技术中标准的光电探测器的外延结构侧剖示意图,沿着外延生长方向依次包括:衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106、N型欧姆电极108和P型欧姆电极107。FIG. 1 is a schematic side sectional view of the epitaxial structure of a standard photodetector in the prior art, which sequentially includes a substrate 101, a P-type heavily doped material layer 102, an N-type lightly doped material layer 103, and an N-type lightly doped material layer along the epitaxial growth direction. N-type transition material layer 104, N-type lightly doped material layer 105, N-type heavily doped material layer 106, N-type ohmic electrode 108 and P-type ohmic electrode 107.
图2为本发明具有弧形增透作用的光电探测器结构一种实施例的结构侧剖示意图,沿着外延生长方向依次包括:衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106、N型欧姆电极108和P型欧姆电极107。Fig. 2 is a schematic side sectional view of an embodiment of a photodetector structure with an arc-shaped anti-reflection effect according to the present invention, which includes in sequence along the epitaxial growth direction: a substrate 101, a P-type heavily doped material layer 102, an N-type light Doping material layer 103 , N-type transition material layer 104 , N-type lightly doped material layer 105 , N-type heavily doped material layer 106 , N-type ohmic electrode 108 and P-type ohmic electrode 107 .
图3为实施例1标准光电探测器沿着衬底101外延生长完P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105和N型重掺杂材料层106后的结构侧剖示意图。Fig. 3 shows that the standard photodetector of Embodiment 1 has epitaxially grown a P-type heavily doped material layer 102, an N-type lightly doped material layer 103, an N-type transition material layer 104, and an N-type lightly doped material layer along the substrate 101. 105 and the N-type heavily doped material layer 106 is a schematic side cross-sectional view of the structure.
图4为实施例1的图3所示制品,通过光刻胶变温回流技术,刻蚀出倾斜台面后的结构侧剖示意图,沿着外延生长方向依次包括:衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105和N型重掺杂材料层106。Fig. 4 is the product shown in Fig. 3 of Example 1, a schematic side sectional view of the structure after the inclined mesa is etched by the photoresist variable temperature reflow technology, and it includes in sequence along the epitaxial growth direction: a substrate 101, a P-type heavily doped Material layer 102 , N-type lightly doped material layer 103 , N-type transition material layer 104 , N-type lightly doped material layer 105 and N-type heavily doped material layer 106 .
图5为实施例1中采用的一种弧形增透作用的光电探测器结构俯视示意图,由外向内依次包括:P型欧姆电极107、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106和N型欧姆电极108。5 is a top view schematic diagram of a photodetector structure with an arc-shaped anti-reflection effect adopted in Embodiment 1, which includes: a P-type ohmic electrode 107, a P-type heavily doped material layer 102, and an N-type lightly doped material layer from outside to inside. Material layer 103 , N-type transition material layer 104 , N-type lightly doped material layer 105 , N-type heavily doped material layer 106 and N-type ohmic electrode 108 .
图6为传统平面外延结构和实施例1中具有弧形增透作用的光电探测器结构的光强分布图,从图中可以明显地看出,对于传统平面外延结构而言,光入射到器件内部以后主要聚集在器件中间位置,而采用弧形增透结构以后,入射光在器件内部的分布相对更加均匀,有效避免光生载流子大量积聚,降低载流子积聚导致的器件自热效应,使更多的载流子发生碰撞电离,提高探测器的光响应度和量子效率。Fig. 6 is the light intensity distribution diagram of the traditional planar epitaxial structure and the photodetector structure with arc-shaped anti-reflection effect in Embodiment 1. It can be clearly seen from the figure that for the traditional planar epitaxial structure, the light incident on the device Afterwards, the interior mainly gathers in the middle of the device, and after adopting the arc-shaped anti-reflection structure, the distribution of incident light inside the device is relatively more uniform, which can effectively avoid the accumulation of a large number of photogenerated carriers and reduce the self-heating effect of the device caused by the accumulation of carriers. More carriers undergo impact ionization, which improves the photoresponsivity and quantum efficiency of the detector.
图7为实施例2中采用的一种弧形增透作用的光电探测器结构侧剖示意图,沿着外延生长方向依次包括:衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106、N型欧姆电极108和P型欧姆电极107。Fig. 7 is a schematic side sectional view of a curved anti-reflection photodetector structure adopted in Embodiment 2, which sequentially includes a substrate 101, a P-type heavily doped material layer 102, an N-type lightly doped material layer along the epitaxial growth direction. Impurity material layer 103 , N-type transition material layer 104 , N-type lightly doped material layer 105 , N-type heavily doped material layer 106 , N-type ohmic electrode 108 and P-type ohmic electrode 107 .
图8为实施例2中采用的一种弧形增透作用的光电探测器结构俯视示意图,由外向内依次包括:P型欧姆电极107、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106和N型欧姆电极108。Fig. 8 is a top view schematic diagram of an arc-shaped anti-reflection photodetector structure adopted in Embodiment 2, which includes: P-type ohmic electrode 107, P-type heavily doped material layer 102, N-type lightly doped material layer from outside to inside Material layer 103 , N-type transition material layer 104 , N-type lightly doped material layer 105 , N-type heavily doped material layer 106 and N-type ohmic electrode 108 .
图9为实施例3中采用的一种弧形增透作用的光电探测器结构侧剖示意图,沿着外延生长方向依次包括:衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106、N型欧姆电极108和P型欧姆电极107。Fig. 9 is a schematic side sectional view of an arc-shaped anti-reflection photodetector structure adopted in Embodiment 3, which sequentially includes a substrate 101, a P-type heavily doped material layer 102, an N-type lightly doped material layer along the epitaxial growth direction. Impurity material layer 103 , N-type transition material layer 104 , N-type lightly doped material layer 105 , N-type heavily doped material layer 106 , N-type ohmic electrode 108 and P-type ohmic electrode 107 .
实施例1Example 1
本实施例一种具有弧形增透作用的光电探测器结构,其该外延结构沿着外延生长方向依次包括:衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106、N型欧姆电极108和P型欧姆电极107,其中N型重掺杂材料层106的厚度为0.3μm、掺杂浓度为1×1019cm-3,光敏区的形状为π/3弧度的单一凹形弧面,弧形结构的投影面积占上表面面积的100%。其中,衬底101的直径为800μm,N型轻掺杂材料层103的直径为700μm,P型欧姆电极107的宽度为50μm,N型欧姆电极108的宽度为50μm。In this embodiment, a photodetector structure with an arc-shaped anti-reflection effect, the epitaxial structure sequentially includes a substrate 101, a P-type heavily doped material layer 102, and an N-type lightly doped material layer 103 along the epitaxial growth direction. , N-type transition material layer 104, N-type lightly doped material layer 105, N-type heavily doped material layer 106, N-type ohmic electrode 108 and P-type ohmic electrode 107, wherein the thickness of N-type heavily doped material layer 106 is 0.3 μm, doping concentration of 1×10 19 cm -3 , the shape of the photosensitive region is a single concave arc surface of π/3 radians, and the projected area of the arc structure accounts for 100% of the upper surface area. Wherein, the diameter of the substrate 101 is 800 μm, the diameter of the N-type lightly doped material layer 103 is 700 μm, the width of the P-type ohmic electrode 107 is 50 μm, and the width of the N-type ohmic electrode 108 is 50 μm.
上述中,衬底101为4H-SiC;P型重掺杂材料层102的材质为SiC、厚度为3μm、掺杂浓度为1×1019cm-3;N型轻掺杂材料层103材质为SiC、厚度为0.3μm、掺杂浓度为1×1015cm-3;N型过渡材料层104材质为SiC、厚度为0.1μm、掺杂浓度为1×1018cm-3;N型轻掺杂材料层105材质为SiC、厚度为0.3μm、掺杂浓度为1×1015cm-3;N型重掺杂材料层106材质为SiC、厚度为0.3μm、掺杂浓度为1×1019cm-3;N型欧姆电极108的材质为Ti/Au;P型欧姆电极107的材质为Ni/Au。In the above, the substrate 101 is 4H-SiC; the material of the P-type heavily doped material layer 102 is SiC, the thickness is 3 μm, and the doping concentration is 1×10 19 cm -3 ; the material of the N-type lightly doped material layer 103 is SiC with a thickness of 0.3 μm and a doping concentration of 1×10 15 cm -3 ; the N-type transition material layer 104 is made of SiC with a thickness of 0.1 μm and a doping concentration of 1×10 18 cm -3 ; N-type lightly doped The impurity material layer 105 is made of SiC with a thickness of 0.3 μm and a doping concentration of 1×10 15 cm −3 ; the N-type heavily doped material layer 106 is made of SiC with a thickness of 0.3 μm and a doping concentration of 1×10 19 cm −3 ; the material of the N-type ohmic electrode 108 is Ti/Au; the material of the P-type ohmic electrode 107 is Ni/Au.
上述一种具有弧形增透作用的光电探测器结构,其制备方法如下:The above-mentioned photodetector structure with arc-shaped anti-reflection effect has a preparation method as follows:
第一步,在超声中依次使用丙酮、无水乙醇、去离子水对衬底进行清洗,生长面朝上,每次超声清洗8分钟,以除掉附着在衬底101表面的异物;In the first step, the substrate is cleaned by using acetone, absolute ethanol, and deionized water in sequence in the ultrasonic wave, with the growth side facing up, and ultrasonic cleaning is performed for 8 minutes each time to remove foreign matter attached to the surface of the substrate 101;
第二步,在MOCVD反应炉中,在第一步处理后的衬底表面上依次外延生长厚度为3μm、掺杂浓度为1×1019cm-3的碳化硅P型重掺杂材料层102,厚度为0.3μm、掺杂浓度为1×1015cm-3的碳化硅N型轻掺杂材料层103,厚度为0.2μm、掺杂浓度为1×1018cm-3的N型过渡材料层104,厚度为0.3μm、掺杂浓度为1×1015cm-3的N型轻掺杂材料层105,厚度为0.3μm、掺杂浓度为1×1019cm-3的N型重掺杂材料层106,生长温度为1500℃,气压为80mbar;In the second step, in the MOCVD reaction furnace, a silicon carbide P-type heavily doped material layer 102 with a thickness of 3 μm and a doping concentration of 1×10 19 cm -3 is sequentially epitaxially grown on the surface of the substrate treated in the first step , a silicon carbide N-type lightly doped material layer 103 with a thickness of 0.3 μm and a doping concentration of 1×10 15 cm -3 , an N-type transition material with a thickness of 0.2 μm and a doping concentration of 1×10 18 cm -3 Layer 104, an N-type lightly doped material layer 105 with a thickness of 0.3 μm and a doping concentration of 1×10 15 cm -3 , and an N-type heavily doped material with a thickness of 0.3 μm and a doping concentration of 1×10 19 cm -3 For the heterogeneous material layer 106, the growth temperature is 1500° C., and the air pressure is 80 mbar;
第三步,在第二步得到的N型重掺杂材料层106上,通过光刻胶变温回流技术和干法刻蚀工艺制作倾斜台面,曝露出P型重掺杂材料层102,其中,梯形倾斜台面内角为8°,刻蚀后的N型轻掺杂材料层103占P型重掺杂材料层面积102的89%;In the third step, on the N-type heavily doped material layer 106 obtained in the second step, an inclined mesa is fabricated by photoresist variable temperature reflow technology and dry etching process, exposing the P-type heavily doped material layer 102, wherein, The inner angle of the trapezoidal inclined mesa is 8°, and the etched N-type lightly doped material layer 103 accounts for 89% of the area of the P-type heavily doped material layer 102;
第四步,在第三步得到台面N型重掺杂材料层106上方蒸镀制备N型欧姆电极108,在曝露出P型重掺杂材料层102上方蒸镀制备P型欧姆电极107,其中,P型欧姆电极107占P型重掺杂材料层102曝露出宽度的50%,P型欧姆电极107和N型欧姆电极108均为圆环状;In the fourth step, an N-type ohmic electrode 108 is prepared by vapor deposition on the N-type heavily doped material layer 106 obtained in the third step, and a P-type ohmic electrode 107 is prepared by vapor deposition on the exposed P-type heavily doped material layer 102, wherein , the P-type ohmic electrode 107 accounts for 50% of the exposed width of the P-type heavily doped material layer 102, and the P-type ohmic electrode 107 and the N-type ohmic electrode 108 are both ring-shaped;
第五步,对于第四步N型重掺杂材料层106制备完N型欧姆电极108剩余的光敏区,通过涂覆光刻胶,曝光和显影,将不需要刻蚀的地方用进行光刻胶保护,需要刻蚀的地方光刻胶去除,然后采用ICP干法刻蚀,通过调节载物台的移动速率和ICP设备的刻蚀功率来制作弧形图案化形状,根据器件结构设计需求,光敏区上表面形状为π/3弧度的凹形弧面;The fifth step is to prepare the remaining photosensitive area of the N-type ohmic electrode 108 for the N-type heavily doped material layer 106 in the fourth step. By coating photoresist, exposing and developing, the place that does not need to be etched is used for photolithography Glue protection, remove the photoresist where etching is required, and then use ICP dry etching to make arc-shaped patterned shapes by adjusting the moving rate of the stage and the etching power of the ICP equipment. According to the design requirements of the device structure, The shape of the upper surface of the photosensitive area is a concave arc surface of π/3 radian;
由此得到本实施例的一种具有弧形增透作用的光电探测器结构。Thus, a photodetector structure with arc-shaped anti-reflection effect of this embodiment is obtained.
图6为光强分布示意图,从图中可以明显地看出,对于传统平面外延结构而言,光入射到器件内部以后主要聚集在器件中间位置,而采用弧形增透结构以后,入射光在器件内部的分布相对更加均匀,有效避免光生载流子大量积聚,提高探测器的光响应度和量子效率。Figure 6 is a schematic diagram of the light intensity distribution. It can be clearly seen from the figure that for the traditional planar epitaxy structure, the light is mainly concentrated in the middle of the device after it is incident inside the device, but after the arc-shaped anti-reflection structure is adopted, the incident light The distribution inside the device is relatively more uniform, effectively avoiding a large amount of accumulation of photogenerated carriers, and improving the photoresponsivity and quantum efficiency of the detector.
实施例2Example 2
本实施例一种具有弧形增透作用的光电探测器结构,其该外延结构沿着外延生长方向依次包括:衬底101、P型重掺杂材料层102、N型轻掺杂材料层103、N型过渡材料层104、N型轻掺杂材料层105、N型重掺杂材料层106、N型欧姆电极108和P型欧姆电极107,其中N型重掺杂材料层106的厚度为0.3μm、掺杂浓度为1×1019cm-3,光敏区的形状为π/4弧度凹凸相间的弧面,其中每个弧面的直径(即圆弧本身的直径)为100μm,弧形结构的投影面积占上表面面积的95%,相邻的凹形弧面和凸形弧面刚好相切。In this embodiment, a photodetector structure with an arc-shaped anti-reflection effect, the epitaxial structure sequentially includes a substrate 101, a P-type heavily doped material layer 102, and an N-type lightly doped material layer 103 along the epitaxial growth direction. , N-type transition material layer 104, N-type lightly doped material layer 105, N-type heavily doped material layer 106, N-type ohmic electrode 108 and P-type ohmic electrode 107, wherein the thickness of N-type heavily doped material layer 106 is 0.3μm, the doping concentration is 1×10 19 cm -3 , the shape of the photosensitive area is a π/4 radian concave and convex arc surface, and the diameter of each arc surface (that is, the diameter of the arc itself) is 100 μm. The projected area of the structure accounts for 95% of the upper surface area, and the adjacent concave and convex arcs are just tangent.
上述中,衬底101为蓝宝石;P型重掺杂材料层102的材质为Al0.4Ga0.6N、厚度为2.5μm、掺杂浓度为2×1018cm-3;N型轻掺杂材料层103材质为Al0.4Ga0.6N、厚度为0.2μm、掺杂浓度为1×1016cm-3;N型过渡材料层104材质为Al0.4Ga0.6N、厚度为0.1μm、掺杂浓度为1×1018cm-3;N型轻掺杂材料层105材质为Al0.4Ga0.6N、厚度为0.2μm、掺杂浓度为1×1016cm-3;N型重掺杂材料层106材质为Al0.45Ga0.55N、厚度为0.3μm、掺杂浓度为2×1018cm-3;N型欧姆电极108的材质为Cr/Au;P型欧姆电极107的材质为Cr/Au。In the above, the substrate 101 is sapphire; the material of the P-type heavily doped material layer 102 is Al 0.4 Ga 0.6 N, the thickness is 2.5 μm, and the doping concentration is 2×10 18 cm -3 ; the N-type lightly doped material layer 103 is made of Al 0.4 Ga 0.6 N with a thickness of 0.2 μm and a doping concentration of 1×10 16 cm -3 ; the N-type transition material layer 104 is made of Al 0.4 Ga 0.6 N with a thickness of 0.1 μm and a doping concentration of 1 ×10 18 cm -3 ; N-type lightly doped material layer 105 is made of Al 0.4 Ga 0.6 N with a thickness of 0.2 μm and a doping concentration of 1×10 16 cm -3 ; N-type heavily doped material layer 106 is made of Al 0.45 Ga 0.55 N, thickness 0.3 μm, doping concentration 2×10 18 cm −3 ; N-type ohmic electrode 108 is made of Cr/Au; P-type ohmic electrode 107 is made of Cr/Au.
上述一种具有弧形增透作用的光电探测器结构,其制备方法如下:The above-mentioned photodetector structure with arc-shaped anti-reflection effect has a preparation method as follows:
第一步,在超声中依次使用丙酮、无水乙醇、去离子水对衬底进行清洗,生长面朝上,每次超声清洗8分钟,以除掉附着在衬底101表面的异物;In the first step, the substrate is cleaned by using acetone, absolute ethanol, and deionized water in sequence in the ultrasonic wave, with the growth side facing up, and ultrasonic cleaning is performed for 8 minutes each time to remove foreign matter attached to the surface of the substrate 101;
第二步,在MOCVD反应炉中,在第一步处理后的衬底表面上依次外延生长厚度为2.5μm、掺杂浓度为2×1018cm-3的Al0.4Ga0.6N材料层102,厚度为0.2μm、掺杂浓度为1×1016cm-3的Al0.4Ga0.6N材料层103,厚度为0.1μm、掺杂浓度为1×1018cm-3的Al0.4Ga0.6N材料层104,厚度为0.2μm、掺杂浓度为1×1016cm-3的Al0.4Ga0.6N材料层105,厚度为0.3μm、掺杂浓度为2×1018cm-3的Al0.45Ga0.55N材料层106,生长温度为970℃,气压为90mbar;In the second step, in the MOCVD reaction furnace, an Al 0.4 Ga 0.6 N material layer 102 with a thickness of 2.5 μm and a doping concentration of 2×10 18 cm −3 is epitaxially grown sequentially on the surface of the substrate treated in the first step, Al 0.4 Ga 0.6 N material layer 103 with a thickness of 0.2 μm and a doping concentration of 1×10 16 cm -3 , and an Al 0.4 Ga 0.6 N material layer with a thickness of 0.1 μm and a doping concentration of 1×10 18 cm -3 104, an Al 0.4 Ga 0.6 N material layer with a thickness of 0.2 μm and a doping concentration of 1×10 16 cm −3 105, an Al 0.45 Ga 0.55 N material layer with a thickness of 0.3 μm and a doping concentration of 2×10 18 cm −3 For the material layer 106, the growth temperature is 970° C., and the air pressure is 90 mbar;
第三步,在第二步得到的N型重掺杂材料层106上,通过光刻胶变温回流技术和干法刻蚀工艺制作倾斜台面,曝露出P型重掺杂材料层102,其中,梯形倾斜台面内角为8°,刻蚀后的N型轻掺杂材料层103占P型重掺杂材料层面积102的89%;In the third step, on the N-type heavily doped material layer 106 obtained in the second step, an inclined mesa is fabricated by photoresist variable temperature reflow technology and dry etching process, exposing the P-type heavily doped material layer 102, wherein, The inner angle of the trapezoidal inclined mesa is 8°, and the etched N-type lightly doped material layer 103 accounts for 89% of the area of the P-type heavily doped material layer 102;
第四步,在第三步得到台面N型重掺杂材料层106上方蒸镀制备N型欧姆电极108,在曝露出P型重掺杂材料层102上方蒸镀制备P型欧姆电极107,其中,P型欧姆电极107占P型重掺杂材料层102曝露出宽度的50%;In the fourth step, an N-type ohmic electrode 108 is prepared by vapor deposition on the N-type heavily doped material layer 106 obtained in the third step, and a P-type ohmic electrode 107 is prepared by vapor deposition on the exposed P-type heavily doped material layer 102, wherein , the P-type ohmic electrode 107 accounts for 50% of the exposed width of the P-type heavily doped material layer 102;
第五步,对于第四步N型重掺杂材料层106制备完N型欧姆电极108剩余的光敏区,通过涂覆光刻胶,曝光和显影,将不需要刻蚀的地方用进行光刻胶保护,需要刻蚀的地方光刻胶去除,然后采用ICP干法刻蚀,通过调节载物台的移动速率和ICP设备的刻蚀功率来制作凸形图案化形状;接着再将样品涂覆光刻胶,曝光和显影,将凸形图案化结构用进行光刻胶保护,需要刻蚀的地方光刻胶去除,同样采用ICP干法刻蚀,通过调节载物台的移动速率和ICP设备的刻蚀功率来制作凹形图案化形状,得到器件结构设计需求的图案形状,光敏区的形状为π/4弧度凹凸相间的弧面;The fifth step is to prepare the remaining photosensitive area of the N-type ohmic electrode 108 for the N-type heavily doped material layer 106 in the fourth step. By coating photoresist, exposing and developing, the place that does not need to be etched is used for photolithography Protected by glue, remove the photoresist where it needs to be etched, and then use ICP dry etching to make a convex patterned shape by adjusting the moving rate of the stage and the etching power of the ICP equipment; then coat the sample Photoresist, exposure and development, protect the convex patterned structure with photoresist, remove the photoresist where it needs to be etched, and also use ICP dry etching, by adjusting the moving rate of the stage and ICP equipment The etching power is used to make a concave patterned shape, and the pattern shape required by the device structure design is obtained. The shape of the photosensitive area is a curved surface with alternating concave and convex in π/4 radians;
由此得到本实施例的一种具有弧形增透作用的光电探测器结构。Thus, a photodetector structure with arc-shaped anti-reflection effect of this embodiment is obtained.
实施例3Example 3
本实施例各部分组成及连接同实施例1,不同之处在于本实施例中其中最顶部N型重掺杂材料层106的光敏区的形状为π/6弧度的凹形曲面相叠加的弧面结构,,其中每个弧面的直径为150μm,相邻弧面之间重叠10%,弧形结构的投影面积占上表面面积的98%,其入射光的透射率较目前平面结构增加20%,从而提高器件的光响应度10%。The composition and connection of the various parts of this embodiment are the same as those of Embodiment 1, except that the shape of the photosensitive region of the topmost N-type heavily doped material layer 106 in this embodiment is an arc superimposed by concave curved surfaces of π/6 radians. Surface structure, in which the diameter of each arc surface is 150 μm, the overlap between adjacent arc surfaces is 10%, the projected area of the arc structure accounts for 98% of the upper surface area, and the transmittance of incident light is increased by 20% compared with the current planar structure %, thereby increasing the photoresponsivity of the device by 10%.
上述实施例均能达到,减少表面的光反射率,增加光的透射率,提高探测器的光响应度和灵敏度,且本发明方法可操作性强,工艺简单,成本低,易于实现。All the above-mentioned embodiments can reduce the light reflectance of the surface, increase the light transmittance, and improve the light responsivity and sensitivity of the detector, and the method of the present invention has strong operability, simple process, low cost and easy implementation.
本发明所涉及的原材料均可通过公知途径获得,其制备方法中的操作工艺是本技术领域的技术人员能够掌握的。The raw materials involved in the present invention can be obtained through known channels, and the operating techniques in the preparation methods are within the grasp of those skilled in the art.
本发明未述及之处适用于现有技术。What is not mentioned in the present invention is applicable to the prior art.
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