CN114628424A - Single photon avalanche diode - Google Patents
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Abstract
本发明公开了一种单光子雪崩二极管,包括阵列排布的多个像素单元以及设置在相邻像素单元之间的共享阴极和隔离单元,其中,所述像素单元包括二极管有源区、纳米蛾眼减反结构和微透镜,所述纳米蛾眼减反结构设置在所述二极管有源区的上表面,所述微透镜设置在所述纳米蛾眼减反结构的上表面;所述共享阴极设置在每相邻四个所述像素单元的顶角围成的区域中;所述隔离单元设置在相邻两个所述像素单元之间,用于对相邻像素单元进行光学及电学隔离。本发明将纳米蛾眼减反微结构、微透镜与光电探测器件相结合,减少特定波段光的反射,增加了回波信号中光子的利用率,从而提高量子效率,并提高系统的探测效率。
The invention discloses a single-photon avalanche diode, comprising a plurality of pixel units arranged in an array, a shared cathode and an isolation unit arranged between adjacent pixel units, wherein the pixel unit includes a diode active area, a nano-moth An eye anti-reflection structure and a microlens, the nano moth-eye anti-reflection structure is arranged on the upper surface of the active region of the diode, the microlens is arranged on the upper surface of the nano moth-eye anti-reflection structure; the shared cathode The isolation unit is arranged in the area surrounded by the top corners of every four adjacent pixel units; the isolation unit is arranged between two adjacent pixel units, and is used for optically and electrically isolating the adjacent pixel units. The invention combines the nano moth-eye antireflection microstructure, the microlens and the photoelectric detection device to reduce the reflection of light in a specific wavelength band and increase the utilization rate of photons in the echo signal, thereby improving the quantum efficiency and the detection efficiency of the system.
Description
技术领域technical field
本发明属于微电子光电器件技术领域,具体涉及一种单光子雪崩二极管。The invention belongs to the technical field of microelectronic optoelectronic devices, and in particular relates to a single-photon avalanche diode.
背景技术Background technique
近年来,远距离主动成像能够提供探测目标的高分辨三维成像,在遥感和目标识别领域具有广阔的应用前景。作为实现远距离主动成像的重要手段,单光子激光雷达通过用激光束照射探测目标,并测量反射光信号的飞行时间(Time of Flight,ToF),从而得到目标的距离信息,通过对探测物体进行二维扫描,就能得到三维的距离信息。In recent years, long-distance active imaging can provide high-resolution 3D imaging of detected targets, and has broad application prospects in the fields of remote sensing and target recognition. As an important means to achieve long-distance active imaging, single-photon lidar detects the target by irradiating the laser beam and measures the Time of Flight (ToF) of the reflected light signal, thereby obtaining the distance information of the target. Two-dimensional scanning can obtain three-dimensional distance information.
单光子雪崩二极管(Single Photon Avalanche Diode,SPAD)由于具有几乎无限增益、高时间分辨率和单光子灵敏度等优点而成为远距离微光探测的最优候选器件之一。此外,由于具有高成本效益、量产能力和易于集成等特点,SPAD在CMOS(ComplementaryMetal Oxide Semiconductor,互补金属氧化物半导体)工艺中的集成备受关注。许多先进的解决方案已经出现,包括最先进的技术节点、微透镜和3D集成。Single-photon avalanche diodes (SPADs) have become one of the best candidates for long-range low-light detection due to their almost infinite gain, high temporal resolution, and single-photon sensitivity. In addition, the integration of SPAD in CMOS (Complementary Metal Oxide Semiconductor, Complementary Metal Oxide Semiconductor) process has attracted much attention due to its high cost-effectiveness, mass production capability, and ease of integration. Many advanced solutions have emerged, including state-of-the-art technology nodes, microlenses, and 3D integration.
然而,随着成像距离的不断增加,从目标返回的光子信号愈发稀少。因此,提高器件的探测效率变得尤为重要,探测效率理论上直接受限于探测概率和量子效率,而如何提高光子利用率是提高量子效率亟待解决的问题。However, as the imaging distance continues to increase, the photon signal returned from the target becomes rarer. Therefore, it is particularly important to improve the detection efficiency of the device. The detection efficiency is theoretically directly limited by the detection probability and quantum efficiency. How to improve the photon utilization rate is an urgent problem to be solved to improve the quantum efficiency.
发明内容SUMMARY OF THE INVENTION
为了解决现有技术中存在的上述问题,本发明提供了一种单光子雪崩二极管。本发明要解决的技术问题通过以下技术方案实现:In order to solve the above problems existing in the prior art, the present invention provides a single photon avalanche diode. The technical problem to be solved by the present invention is realized by the following technical solutions:
本发明提供了一种单光子雪崩二极管,包括阵列排布的多个像素单元以及设置在相邻像素单元之间的共享阴极和隔离单元,其中,The present invention provides a single-photon avalanche diode, comprising a plurality of pixel units arranged in an array and a shared cathode and an isolation unit arranged between adjacent pixel units, wherein,
所述像素单元包括二极管有源区、纳米蛾眼减反结构和微透镜,所述纳米蛾眼减反结构设置在所述二极管有源区的上表面,所述微透镜设置在所述纳米蛾眼减反结构的上表面;The pixel unit includes a diode active region, a nano moth-eye anti-reflection structure, and a microlens, the nano-moth-eye anti-reflection structure is arranged on the upper surface of the diode active region, and the microlens is arranged on the nano-moth eye anti-reflection structure. the upper surface of the ocular antireflection structure;
所述共享阴极设置在每相邻四个所述像素单元的顶角围成的区域中;所述隔离单元设置在相邻两个所述像素单元之间,用于对相邻像素单元进行光学及电学隔离。The shared cathode is arranged in the area enclosed by the top corners of every four adjacent pixel units; the isolation unit is arranged between two adjacent pixel units, and is used for optically conducting optical imaging on adjacent pixel units. and electrical isolation.
在本发明的一个实施例中,所述二极管有源区包括P型衬底层、P型外延层、N型埋层、p+有源层、有源区光子反射金属板、阳极电极以及布线层,其中,In an embodiment of the present invention, the diode active region includes a P-type substrate layer, a P-type epitaxial layer, an N-type buried layer, a p+ active layer, an active region photon reflective metal plate, an anode electrode and a wiring layer, in,
所述布线层、所述P型外延层、所述N型埋层和所述P型衬底层自下而上层叠设置,所述纳米蛾眼减反结构设置在所述P型衬底层的上表面;The wiring layer, the P-type epitaxial layer, the N-type buried layer and the P-type substrate layer are stacked from bottom to top, and the nano moth-eye anti-reflection structure is arranged on the P-type substrate layer surface;
所述p+有源层设置在所述P型外延层的下表面中心;the p+ active layer is arranged at the center of the lower surface of the p-type epitaxial layer;
所述阳极电极镶嵌在所述布线层的上表面且所述阳极电极的上表面与所述p+有源层的下表面接触,所述有源区光子反射金属板镶嵌在所述布线层的下表面。The anode electrode is embedded on the upper surface of the wiring layer and the upper surface of the anode electrode is in contact with the lower surface of the p+ active layer, and the active region photon reflective metal plate is embedded under the wiring layer surface.
在本发明的一个实施例中,所述P型衬底层为掺杂有磷或锑的Si基衬底,厚度为3~10μm。In an embodiment of the present invention, the P-type substrate layer is a Si-based substrate doped with phosphorus or antimony, and has a thickness of 3-10 μm.
在本发明的一个实施例中,所述隔离单元包括自上而下依次堆叠在相邻所述像素单元之间的深槽隔离区、隔离N阱和浅槽隔离层,其中,In an embodiment of the present invention, the isolation unit includes a deep trench isolation region, an isolation N-well and a shallow trench isolation layer sequentially stacked between adjacent pixel units from top to bottom, wherein,
所述浅槽隔离层镶嵌在所述P型外延层的下表面,所述隔离N阱设置在所述浅槽隔离层的上表面且与所述N型埋层的下表面接触;The shallow trench isolation layer is embedded on the lower surface of the P-type epitaxial layer, and the isolation N well is disposed on the upper surface of the shallow trench isolation layer and is in contact with the lower surface of the N-type buried layer;
所述深槽隔离区从所述P型衬底层的上表面延伸至所述隔离N阱的内部且能够间隔相邻所述像素单元的N型埋层。The deep trench isolation region extends from the upper surface of the P-type substrate layer to the interior of the isolation N-well and can space an N-type buried layer adjacent to the pixel unit.
在本发明的一个实施例中,所述共享阴极包括自上而下依次层叠设置的深N阱、N+掺杂阱和阴极电极,其中,In an embodiment of the present invention, the shared cathode includes a deep N well, an N+ doped well and a cathode electrode that are stacked in sequence from top to bottom, wherein,
所述深N阱和所述N+掺杂阱设置在所述P型外延层内部,所述阴极电极位于所述布线层内部,且所述深N阱的上表面与所述N型埋层的下表面接触。The deep N well and the N+ doped well are arranged inside the P-type epitaxial layer, the cathode electrode is located inside the wiring layer, and the upper surface of the deep N well and the N-type buried layer contact with the lower surface.
在本发明的一个实施例中,所述纳米蛾眼减反结构包括蛾眼减反微结构、增反膜以及平坦层,其中,In an embodiment of the present invention, the nano moth-eye anti-reflection structure includes a moth-eye anti-reflection microstructure, an anti-reflection film and a flat layer, wherein,
所述蛾眼减反微结构包括多个纳米蛾眼减反微结构,所述多个纳米蛾眼减反微结构的高度、密度及直径分别在平均高度、平均密度及平均直径左右呈随机分布且自下而上直径逐渐减小;The moth-eye anti-reflection microstructure includes a plurality of nano moth-eye anti-reflection microstructures, and the height, density and diameter of the plurality of nano moth-eye anti-reflection microstructures are randomly distributed around the average height, average density and average diameter respectively. And the diameter gradually decreases from bottom to top;
所述平坦层填充在所述多个纳米蛾眼减反微结构的间隙中,以形成平坦的上下表面,所述微透镜设置在所述平坦层上方;the flat layer is filled in the gaps of the plurality of nano moth-eye anti-reflection microstructures to form flat upper and lower surfaces, and the microlenses are disposed above the flat layer;
所述增反膜位于相邻两个由所述蛾眼减反微结构和所述平坦层组成的结构之间。The antireflection film is located between two adjacent structures composed of the moth-eye antireflection microstructure and the flat layer.
在本发明的一个实施例中,所述蛾眼减反微结构和所述平坦层均为可生长在Si表面的薄膜材料,所述微透镜材料的折射率<所述平坦层材料的折射率<所述蛾眼减反微结构材料的折射率In an embodiment of the present invention, the moth-eye anti-reflection microstructure and the flat layer are both thin film materials that can be grown on the Si surface, and the refractive index of the microlens material<the refractive index of the flat layer material <Refractive index of the moth-eye anti-reflection microstructure material
在本发明的一个实施例中,所述增反膜为TiO2、ZrO2或者其组合。In an embodiment of the present invention, the anti-reflection film is TiO 2 , ZrO 2 or a combination thereof.
在本发明的一个实施例中,所述蛾眼减反微结构为子弹状纳米结构、纳米圆台结构、抛物面状纳米结构、高斯面状纳米结构或纳米椎结构。In an embodiment of the present invention, the moth-eye antireflection microstructure is a bullet-shaped nanostructure, a nano-truncated cone structure, a parabolic nano-structure, a Gaussian-shaped nano-structure or a nano-pyramid structure.
与现有技术相比,本发明的有益效果在于:Compared with the prior art, the beneficial effects of the present invention are:
1、本发明的单光子雪崩二极管,将纳米蛾眼减反微结构、微透镜与光电探测器件相结合,在传统光电探测器件上刻蚀或生长纳米蛾眼减反结构,并在像素单元之间利用增反结构增加无用光子的反射,最大限度地利用照射到探测芯片上的光子,并针对特定波长对微结构和微透镜尺寸进行优化,实现特定波段的高窗口透射率,提高量子效率从而提高探测效率。实现高效的远距离微光探测。1. The single-photon avalanche diode of the present invention combines nano-moth-eye anti-reflection microstructures, microlenses and photodetector devices, etches or grows nano-moth-eye anti-reflection structures on traditional photodetector devices, and places them between pixel units. Using the anti-reflection structure to increase the reflection of useless photons, maximize the use of photons irradiated on the detection chip, and optimize the size of the microstructure and microlens for specific wavelengths to achieve high window transmittance in specific wavelengths and improve quantum efficiency. Improve detection efficiency. Achieve efficient long-distance low-light detection.
2、本发明的单光子雪崩二极管通过增加微透镜结构增加了器件的有效填充率,通过纳米蛾眼减反结构减少光的反射,增加了回波信号中光子的利用率,通过n+/P结构使得在高场吸收区范围内,主要由电子参与雪崩,电子雪崩电离率较高,可进一步提高量子效率,通过提高填充率、量子效率、光子利用率最终可以提高器件的探测效率。2. The single-photon avalanche diode of the present invention increases the effective filling rate of the device by increasing the microlens structure, reduces the reflection of light through the nano moth-eye anti-reflection structure, and increases the utilization rate of photons in the echo signal. Through the n+/P structure In the high-field absorption region, electrons are mainly involved in avalanche, and the electron avalanche ionization rate is high, which can further improve the quantum efficiency. By improving the filling rate, quantum efficiency, and photon utilization rate, the detection efficiency of the device can be improved.
以下将结合附图及实施例对本发明做进一步详细说明。The present invention will be further described in detail below with reference to the accompanying drawings and embodiments.
附图说明Description of drawings
图1是本发明实施例提供的一种单光子雪崩二极管的部分4×4阵列像素结构的顶视图;1 is a top view of a partial 4×4 array pixel structure of a single-photon avalanche diode provided by an embodiment of the present invention;
图2是沿图1中的A-A线截取的截面图;Figure 2 is a cross-sectional view taken along line A-A in Figure 1;
图3是本发明实施例提供的一种位于器件边缘的像素单元的截面示意图;3 is a schematic cross-sectional view of a pixel unit located at the edge of a device provided by an embodiment of the present invention;
图4是本发明实施例提供的一种共享阴极的截面示意图;4 is a schematic cross-sectional view of a shared cathode provided by an embodiment of the present invention;
图5是本发明实施例提供的一种具有随机分布三角锥的蛾眼减反微结构的结构示意图;5 is a schematic structural diagram of a moth-eye antireflection microstructure with randomly distributed triangular pyramids provided by an embodiment of the present invention;
图6是本发明实施例提供的一种平均直径为100nm、平均高度为400nm的随机分布蛾眼微结构的反射曲线图。6 is a reflection curve diagram of a randomly distributed moth-eye microstructure with an average diameter of 100 nm and an average height of 400 nm provided by an embodiment of the present invention.
附图标记说明:Description of reference numbers:
1-像素单元;11-二极管有源区;111-P型衬底层;112-P型外延层;113-N型埋层;114-p+有源层;115-有源区光子反射金属板;116-阳极电极;117-布线层;12-蛾眼减反结构;121-蛾眼减反微结构;122-增反膜;123-平坦层;13-微透镜;2-共享阴极;21-深N阱;22-N+掺杂阱;23-阴极电极;3-隔离单元;31-深槽隔离区;32-隔离N阱;33-浅槽隔离层。1-pixel unit; 11-diode active region; 111-P-type substrate layer; 112-P-type epitaxial layer; 113-N-type buried layer; 114-p+active layer; 115-active region photon reflective metal plate; 116-anode electrode; 117-wiring layer; 12-moth-eye anti-reflection structure; 121-moth-eye anti-reflection microstructure; 122-reflection enhancement film; 123-flat layer; 13-microlens; 2-shared cathode; 21- 22-N+ doped well; 23-cathode electrode; 3-isolation unit; 31-deep trench isolation region; 32-isolated N-well; 33-shallow trench isolation layer.
具体实施方式Detailed ways
为了进一步阐述本发明为达成预定发明目的所采取的技术手段及功效,以下结合附图及具体实施方式,对依据本发明提出的一种单光子雪崩二极管进行详细说明。In order to further illustrate the technical means and effects adopted by the present invention to achieve the predetermined purpose of the invention, a single photon avalanche diode according to the present invention will be described in detail below with reference to the accompanying drawings and specific embodiments.
有关本发明的前述及其他技术内容、特点及功效,在以下配合附图的具体实施方式详细说明中即可清楚地呈现。通过具体实施方式的说明,可对本发明为达成预定目的所采取的技术手段及功效进行更加深入且具体地了解,然而所附附图仅是提供参考与说明之用,并非用来对本发明的技术方案加以限制。The foregoing and other technical contents, features and effects of the present invention can be clearly presented in the following detailed description of the specific implementation with the accompanying drawings. Through the description of the specific embodiments, the technical means and effects adopted by the present invention to achieve the predetermined purpose can be more deeply and specifically understood. However, the accompanying drawings are only for reference and description, and are not used for the technical description of the present invention. program is restricted.
应当说明的是,在本文中,诸如第一和第二等之类的关系术语仅仅用来将一个实体或者操作与另一个实体或操作区分开来,而不一定要求或者暗示这些实体或操作之间存在任何这种实际的关系或者顺序。而且,术语“包括”、“包含”或者任何其他变体意在涵盖非排他性的包含,从而使得包括一系列要素的物品或者设备不仅包括那些要素,而且还包括没有明确列出的其他要素。在没有更多限制的情况下,由语句“包括一个……”限定的要素,并不排除在包括所述要素的物品或者设备中还存在另外的相同要素。It should be noted that, in this document, relational terms such as first and second are used only to distinguish one entity or operation from another entity or operation, and do not necessarily require or imply any relationship between these entities or operations. any such actual relationship or sequence exists. Moreover, the terms "comprising", "comprising" or any other variation are intended to encompass a non-exclusive inclusion, whereby an article or device comprising a list of elements includes not only those elements, but also other elements not expressly listed. Without further limitation, an element qualified by the phrase "comprising a..." does not preclude the presence of additional identical elements in the article or device that includes the element.
请参见图1和图2,图1是本发明实施例提供的一种单光子雪崩二极管的部分4×4阵列像素结构的顶视图,图2是沿图1中的A-A线截取的截面图。本实施例的单光子雪崩二极管包括阵列排布的多个像素单元1以及设置在相邻像素单元1之间的共享阴极2和隔离单元3,其中,像素单元1包括二极管有源区11、纳米蛾眼减反结构12和微透镜13,纳米蛾眼减反结构12设置在二极管有源区11的上表面,微透镜13设置在纳米蛾眼减反结构12的上表面。具体地,微透镜13覆盖像素单元1的整个像素感光区域,用于实现聚焦,将较大入射面的入射光聚集至二极管有源区11,纳米蛾眼减反结构12用于减少光的反射,增大感光区域的透光量,二极管有源区11通过雪崩倍增效应将单个光子倍增为光生电流。Please refer to FIGS. 1 and 2 . FIG. 1 is a top view of a partial 4×4 pixel structure of a single photon avalanche diode according to an embodiment of the present invention, and FIG. 2 is a cross-sectional view taken along line A-A in FIG. 1 . The single-photon avalanche diode of this embodiment includes a plurality of pixel units 1 arranged in an array, a shared
共享阴极2设置在每相邻四个像素单元1的顶角围成的区域中,用于为二极管有源区11供电。隔离单元3设置在相邻两个像素单元1之间,用于对相邻像素单元1进行光学及电学隔离。The shared
进一步地,每个像素单元1的二极管有源区11均包括P型衬底层111、P型外延层112、N型埋层113、p+有源层114、有源区光子反射金属板115、阳极电极116以及布线层117,其中,布线层117、P型外延层112、N型埋层113和P型衬底层111自下而上层叠设置,纳米蛾眼减反结构12设置在P型衬底层111的上表面。N型埋层113与P型外延层112形成倍增主结,构成强电场,以感知光子的到来。在制备过程中,在生长P型外延层112之前,在P型衬底层111上进行掺杂形成N型埋层113,为高浓度掺杂。优选地,N型埋层113的掺杂元素为磷、锑等III族元素,掺杂浓度为约5e18cm-3。P型衬底层111为掺杂有磷或锑的Si基衬底,厚度为3~10μm,掺杂浓度为约5e15cm-3;P型外延层112的掺杂浓度为约1e15cm-3,需要说明的是,本实施例中的P型掺杂为掺杂了Ⅴ族元素,例如:硼、铝等,N型掺杂为掺杂了III族元素,例如:磷、锑等。由于P型外延层112的掺杂浓度较低,耗尽区宽度较宽,有助于提高器件探测概率和光谱响应范围。Further, the diode
在本实施例中,N型埋层113为所有像素单元所共享的,形成一整个连续的区域。In this embodiment, the N-type buried
由N型埋层113和P型外延层112构成的雪崩倍增区主要耗尽宽度延伸在P型外延层112,电场从P型外延层112指向N型埋层113,在高场吸收区范围内,主要由电子参与雪崩,电子雪崩电离率较高,可进一步提高量子效率。The main depletion width of the avalanche multiplication region formed by the N-type buried
p+有源层114设置在P型外延层112的下表面中心,即单个像素单元的P+有源层114位于单个像素中心,在制备过程中是通过在P型外延层112进行掺杂形成的。优选地,p+有源层114掺杂有磷或锑,掺杂浓度为1e19cm-3-5e20cm-3。The p+
阳极电极116镶嵌在布线层117的上表面且阳极电极116的上表面与p+有源层114的下表面接触,有源区光子反射金属板115镶嵌在布线层117的下表面。进一步地,有源区光子反射金属板115位于p+有源层114正下方,可以将照射到其上的光子反射回器件内部,以增加光子的利用率,可以在更长的波长上增强器件探测概率。The
阳极电极116位于P+有源层114下表面的中心位置,其为浮动电位,与后续电路相连接,通过雪崩倍增效应产生的大电流使后续电路重固定节点产生电位变化,从而体现出光子的到来。进一步地,为避免阳极电极116连接较大负载电容,阳极电极116与有源区光子反射金属板115被布线层117内的介质电学隔离,并且阳极电极116通过布线层117内水平和垂直布线与下层芯片的电路连接,有源区光子反射金属板115为浮空状态。The
进一步地,隔离单元3包括自上而下依次堆叠在相邻像素单元1之间的深槽隔离区31、隔离N阱32和浅槽隔离层33,其中,浅槽隔离层33镶嵌在P型外延层112的下表面,隔离N阱32设置在浅槽隔离层33的上表面且与N型埋层113的下表面接触;深槽隔离区31从P型衬底层111的上表面延伸至隔离N阱32的内部。Further, the
隔离N阱32隔离两个相邻像素单元,并且通过与P型外延层102形成反向偏置的PN结结构,避免载流子漂移或隧穿形成的相邻像素单元串扰。The isolation N well 32 isolates two adjacent pixel units, and by forming a reverse biased PN junction structure with the P-type epitaxial layer 102 , crosstalk between adjacent pixel units caused by carrier drift or tunneling is avoided.
深槽隔离区31位于两个像素单元之间,用来隔离相邻像素单元,深槽隔离区31的宽度小于隔离N阱32的宽度,隔离N阱32与N型埋层113在垂直方向上相接,作为N型埋层113与P型外延层112形成的倍增主结的保护环,留出足够的安全距离,以防止蚀刻和填充过程造成的陷阱对暗计数率和后脉冲产生负面影响。The deep
请参见图3,图3是本发明实施例提供的一种位于器件边缘的像素单元的截面示意图。如上所述,本实施例的单光子雪崩二极管包括阵列排布的多个像素单元1,对于位于器件边缘的像素单元,其N型埋层113的尺寸略小于P型衬底层111和P型外延层112,即N型埋层113的边缘包裹在P型衬底层111和P型外延层112内部,同时,N型埋层113的边缘下表面依次设置有隔离N阱32和浅槽隔离层33。同样的,有隔离N阱32和浅槽隔离层33与p+有源层114间隔开,且包裹在P型外延层112内部。Please refer to FIG. 3 , which is a schematic cross-sectional view of a pixel unit located at an edge of a device provided by an embodiment of the present invention. As mentioned above, the single-photon avalanche diode of this embodiment includes a plurality of pixel units 1 arranged in an array. For the pixel unit located at the edge of the device, the size of the N-type buried
进一步地,请参见图4,图4是本发明实施例提供的一种共享阴极的截面示意图。本实施例的共享阴极2包括自上而下依次层叠设置的深N阱21、N+掺杂阱22和阴极电极23,其中,深N阱21和N+掺杂阱22设置在P型外延层112内部,阴极电极23位于布线层117内部,且深N阱21的上表面与N型埋层113的下表面接触。Further, please refer to FIG. 4 , which is a schematic cross-sectional view of a shared cathode provided by an embodiment of the present invention. The shared
阴极电极23通过N+掺杂阱22、深N阱21与N型埋层113形成电学接触,为相邻二极管有源区1中的N型埋层113提供反向偏置电压。为了避免N阱埋层113的横向电阻损耗导致的电位不一致,每个共享阴极2为临近4个像素提供偏置电压。The
进一步地,蛾眼减反结构12包括蛾眼减反微结构121、增反膜122以及平坦层123,其中,蛾眼减反微结构121包括多个纳米蛾眼减反微结构,多个纳米蛾眼减反微结构的高度、密度及直径分别在平均高度、平均密度及平均直径左右呈随机分布且自下而上直径逐渐减小,如图5所示;平坦层123填充在多个纳米蛾眼减反微结构的间隙中,以形成平坦的上下表面,利于微透镜的制作及稳定,微透镜13设置在平坦层123上方;增反膜122位于相邻两个由蛾眼减反微结构121和平坦层123组成的结构之间。微透镜13设置在平坦层123上方,覆盖整个像素感光区域,通过折射作用将光子聚集到p+有源层114。Further, the moth-
优选地,本实施例的蛾眼减反微结构121和平坦层123均为可生长在Si表面的薄膜材料。进一步地,蛾眼减反微结构121的直径自下而上逐渐减小,优选地,蛾眼减反微结构121为子弹状纳米结构、纳米圆台结构、抛物面状纳米结构,高斯面状纳米结构或纳米椎结构。微透镜13的折射率<平坦层123的折射率<蛾眼减反微结构121的折射率<Si的折射率。平坦层123可以选择SiO2,蛾眼减反微结构可以选择SiN。蛾眼减反微结构121可以使大部分的入射光线被吸收,折射率自上而下连续变化不发生反射,从而提高光子利用率。Preferably, the moth-
需要说明的是,前述随机阵列纳米蛾眼减反微结构121的高度、密度及直径分别在平均高度、平均密度及平均直径左右呈随机分布。其相较于周期性纳米结构,具有更好的减反特性,具体分布针对不同波长进行优化,可使光电探测器件具有窗口增透作用。图6是本发明实施例提供的一种平均直径为100nm,平均高度为400nm的随机分布蛾眼微结构的反射曲线图,可见其在550nm处反射率很低,透光性好。进一步地,蛾眼减反微结构121的制作工艺可以是二元光刻技术、激光直写技术、电子束光刻、反应离子刻蚀等。It should be noted that the height, density and diameter of the aforementioned random array nano moth-
增反膜122能够将雪崩倍增区无法利用的光子进行反射,避免侧边击穿及暗计数。增反膜122是抗激光损伤性能小、折射率高的薄膜,可以是二氧化钛(TiO2)\氧化锆(ZrO2)等或者其组合,厚度根据激光波长在光学仿真软件内仿真优化得到最优值。The
微透镜13针对不同波长具有不同曲率,其将所有照射到感光器件表面的光线聚集到雪崩倍增区,提高光子利用率。The
进一步地,本实施例的单光子雪崩二极管常用于激光雷达的接收端,具体工作过程为:光电探测器接收从目标反射回来的目标回波,目标回波首先接触到微透镜,微透镜实现聚光作用,将照射到二极管表面的光聚焦到雪崩倍增区上方的蛾眼减反结构表面,蛾眼减反结构减少光的反射,增大感光区域的透光量。与此同时,器件通过阴极共享电极被偏置到高击击穿电压的反向偏置状态,当器件吸收到一个光子时,二极管有源区载流子的雪崩倍增效应吸收单个光子放大为一个脉冲电流,该电流通过阳极电极流到后续电路,后续电路通过感应脉冲电流来预测光子的到来。Further, the single-photon avalanche diode of this embodiment is often used at the receiving end of the lidar, and the specific working process is as follows: the photodetector receives the target echo reflected from the target, the target echo first contacts the microlens, and the microlens realizes the convergence. The effect of light is to focus the light irradiated on the surface of the diode to the surface of the moth-eye anti-reflection structure above the avalanche multiplication area. The moth-eye anti-reflection structure reduces the reflection of light and increases the amount of light transmission in the photosensitive area. At the same time, the device is biased to a reverse-biased state with a high breakdown voltage through the cathode shared electrode. When the device absorbs a photon, the avalanche multiplication effect of the carriers in the active region of the diode absorbs a single photon and amplifies it into a single photon. A pulsed current, which flows through the anode electrode to a subsequent circuit, which predicts the arrival of photons by inducing the pulsed current.
综上,本实施例的单光子雪崩二极管,将纳米蛾眼减反微结构、微透镜与光电探测器件相结合,在传统光电探测器件上刻蚀或生长纳米蛾眼减反结构,并在像素单元之间利用增反结构增加无用光子的反射,最大限度地利用照射到探测芯片上的光子,并针对特定波长对微结构和微透镜尺寸进行优化,实现特定波段的高窗口透射率,提高量子效率从而提高探测效率。实现高效的远距离微光探测。此外,该单光子雪崩二极管通过增加微透镜结构增加了器件的有效填充率,通过纳米蛾眼减反结构减少光的反射,增加了回波信号中光子的利用率,通过n+/P结构使得在高场吸收区范围内,主要由电子参与雪崩,电子雪崩电离率较高,可进一步提高量子效率,通过提高填充率、量子效率、光子利用率最终可以提高器件的探测效率。To sum up, the single-photon avalanche diode of this embodiment combines nano-moth-eye anti-reflection microstructures, microlenses and photodetection devices, and etches or grows nano-moth-eye anti-reflection structures on traditional photodetector devices. The enhancement and reflection structure is used between the units to increase the reflection of useless photons, maximize the use of photons irradiated on the detection chip, and optimize the microstructure and microlens size for specific wavelengths to achieve high window transmittance in specific wavelength bands and improve quantum efficiency to improve detection efficiency. Achieve efficient long-distance low-light detection. In addition, the single-photon avalanche diode increases the effective filling rate of the device by increasing the micro-lens structure, reduces the reflection of light through the nano moth-eye anti-reflection structure, and increases the utilization rate of photons in the echo signal. In the high-field absorption region, electrons are mainly involved in avalanche, and the electron avalanche ionization rate is high, which can further improve the quantum efficiency.
以上内容是结合具体的优选实施方式对本发明所作的进一步详细说明,不能认定本发明的具体实施只局限于这些说明。对于本发明所属技术领域的普通技术人员来说,在不脱离本发明构思的前提下,还可以做出若干简单推演或替换,都应当视为属于本发明的保护范围。The above content is a further detailed description of the present invention in combination with specific preferred embodiments, and it cannot be considered that the specific implementation of the present invention is limited to these descriptions. For those of ordinary skill in the technical field of the present invention, without departing from the concept of the present invention, some simple deductions or substitutions can be made, which should be regarded as belonging to the protection scope of the present invention.
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