CN110233423A - The high-power vertical cavity surface emitting laser of metal grill - Google Patents
The high-power vertical cavity surface emitting laser of metal grill Download PDFInfo
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- H01S5/183—Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities having only vertical cavities, e.g. vertical cavity surface-emitting lasers [VCSEL]
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Abstract
本发明提供一种金属网格大功率垂直腔面发射激光器,其具有发射孔以及上电极结构,所述上电极结构包括外围电极以及多根栅线电极,其中,所述外围电极设置于所述发射孔的外周,所述多根栅线电极与所述外围电极相连且延伸至所述发射孔之内。本发明通过多根栅线电极,将大氧化孔径的垂直腔面发射激光器的以增加电流路径的方式分割成多个窄长块状区域,一方面可有效增加大氧化孔径的垂直腔面发射激光器的中部区域的电流密度,另一方面,电流可从所述多个栅线电极进行横向传播,大大提高了发光孔内的电流密度分布的均匀性,提高了转化效率。同时,大范围的保持了出射光的相干性。该发明可以应用在激光雷达、红外摄像头和深度识别探测器等领域。
The present invention provides a metal grid high-power vertical cavity surface emitting laser, which has an emission hole and an upper electrode structure, and the upper electrode structure includes a peripheral electrode and a plurality of grid line electrodes, wherein the peripheral electrode is arranged on the The outer periphery of the emission hole, the plurality of grid electrodes are connected to the peripheral electrodes and extend into the emission hole. The present invention divides the vertical cavity surface emitting laser with large oxidation aperture into a plurality of narrow and long block regions by increasing the current path through a plurality of gate wire electrodes, on the one hand, it can effectively increase the vertical cavity surface emitting laser with large oxidation aperture The current density in the central region, on the other hand, the current can be transmitted laterally from the plurality of grid electrodes, which greatly improves the uniformity of the current density distribution in the light-emitting hole and improves the conversion efficiency. At the same time, the coherence of the outgoing light is maintained in a wide range. The invention can be applied in fields such as laser radar, infrared camera and depth recognition detector.
Description
技术领域technical field
本发明属于半导体激光器设计及制造领域,特别是涉及一种金属网格大功率垂直腔面发射激光器。The invention belongs to the field of semiconductor laser design and manufacture, in particular to a metal grid high-power vertical cavity surface emitting laser.
背景技术Background technique
垂直腔面发射激光器(VCSEL)是以砷化镓半导体材料为基础研制,有别于发光二极管(LED)和激光二极管(LD)等其他光源,具有体积小、圆形输出光斑、单纵模输出、阈值电流小、价格低廉、易集成为大面积阵列等优点,广泛应用与光通信、光互连、光存储等领域。Vertical cavity surface emitting laser (VCSEL) is developed on the basis of gallium arsenide semiconductor materials. It is different from other light sources such as light-emitting diodes (LEDs) and laser diodes (LDs). It has small size, circular output spot, and single longitudinal mode output. , small threshold current, low price, easy integration into large-area arrays, etc., are widely used in optical communication, optical interconnection, optical storage and other fields.
垂直腔面发射激光器(VCSEL)是一种垂直表面出光的新型激光器,与传统边发射激光器不同的结构带来了许多优势:小的发散角和圆形对称的远、近场分布使其与光纤的耦合效率大大提高,而不需要复杂昂贵的光束整形系统,现已证实与多模光纤的耦合效率竟能大于90%;光腔长度极短,导致其纵模间距拉大,可在较宽的温度范围内实现单纵模工作,动态调制频率高;可以在片测试,极大地降低了开发成本;出光方向垂直衬底,可以很容易地实现高密度二维面阵的集成,实现更高功率输出,并且因为在垂直于衬底的方向上可并行排列着多个激光器,所以非常适合应用在并行光传输以及并行光互连等领域,它以空前的速度成功地应用于单通道和并行光互联,以它很高的性能价格比,在宽带以太网、高速数据通信网中得到了大量的应用;最吸引人的是它的制造工艺与发光二极管(LED)兼容,大规模制造的成本很低。The Vertical Cavity Surface Emitting Laser (VCSEL) is a new type of laser that emits light from the vertical surface. Its different structure from the traditional edge emitting laser brings many advantages: small divergence angle and circular symmetrical far and near field distribution make it compatible with optical fiber The coupling efficiency is greatly improved without the need for complex and expensive beam shaping systems. It has been confirmed that the coupling efficiency with multimode fibers can be greater than 90%; The single longitudinal mode operation can be realized within a certain temperature range, and the dynamic modulation frequency is high; on-chip testing can be performed, which greatly reduces the development cost; the light output direction is perpendicular to the substrate, which can easily realize the integration of high-density two-dimensional area arrays and achieve higher Power output, and because multiple lasers can be arranged in parallel in the direction perpendicular to the substrate, it is very suitable for applications in the fields of parallel optical transmission and parallel optical interconnection. It has been successfully applied to single-channel and parallel lasers at an unprecedented speed Optical interconnection, with its high cost performance, has been widely used in broadband Ethernet and high-speed data communication networks; the most attractive thing is that its manufacturing process is compatible with light-emitting diodes (LEDs), and the cost of large-scale manufacturing very low.
垂直腔面发射激光器(VCSEL)在光通信、光存储、光互联、光计算、固态照明、激光打印和生物传感等领域受到广泛应用。近年来,在3D人脸识别,接近感应器,激光雷达,红外摄像,深度探测等新兴市场出现更大规模的使用。在不少实际应用中都要求垂直腔面发射激光器(VCSEL)能够实现高能量密度的工作,有些还要求保持激光光源有一定的相干性。把发光孔径做成阵列可以增大发光功率,但是能量密度受限于发光点之间的间距,并且相干性也会消除(对某些应用是好事,另外一些应用则希望保留相干性)。增大氧化孔径是提高能量密度并且保持相干性的一个简单可行的方案。但是大氧化孔径的垂直腔面发射激光器(VCSEL)面临电流密度分布不均匀,导致转换功率较低,光强分布一致性较差的问题。Vertical-cavity surface-emitting lasers (VCSELs) are widely used in optical communications, optical storage, optical interconnection, optical computing, solid-state lighting, laser printing, and biosensing. In recent years, there have been larger-scale applications in emerging markets such as 3D face recognition, proximity sensors, lidar, infrared cameras, and depth detection. In many practical applications, it is required that the vertical cavity surface emitting laser (VCSEL) can achieve high energy density, and some also require the laser source to have a certain degree of coherence. Arraying the light-emitting apertures can increase the luminous power, but the energy density is limited by the spacing between the light-emitting points, and the coherence will be eliminated (good for some applications, others want to preserve coherence). Enlarging the oxide pore size is a simple and feasible solution to increase energy density while maintaining coherence. However, vertical-cavity surface-emitting lasers (VCSELs) with large oxide apertures face the problem of uneven current density distribution, resulting in low conversion power and poor consistency of light intensity distribution.
发明内容Contents of the invention
鉴于以上所述现有技术的缺点,本发明的目的在于提供一种金属网格大功率垂直腔面发射激光器,用于解决大氧化孔径垂直腔面发射激光器电流密度分布不均匀等问题。In view of the above-mentioned shortcomings of the prior art, the object of the present invention is to provide a metal grid high-power vertical cavity surface emitting laser, which is used to solve the problem of uneven current density distribution of the large oxide aperture vertical cavity surface emitting laser.
为实现上述目的及其他相关目的,本发明提供一种金属网格大功率垂直腔面发射激光器,所述垂直腔面发射激光器具有发射孔以及上电极结构,所述上电极结构包括外围电极以及多根栅线电极,其中,所述外围电极设置于所述发射孔的外周,所述多根栅线电极与所述外围电极相连且延伸至所述发射孔之内。To achieve the above purpose and other related purposes, the present invention provides a metal grid high-power vertical cavity surface emitting laser, the vertical cavity surface emitting laser has an emission hole and an upper electrode structure, and the upper electrode structure includes peripheral electrodes and multiple A grid line electrode, wherein the peripheral electrode is arranged on the periphery of the emission hole, and the plurality of grid line electrodes are connected to the peripheral electrode and extend into the emission hole.
可选地,所述多根栅线电极间隔连接于所述外围电极上,并朝所述发射孔的中心延伸。Optionally, the plurality of gate wire electrodes are connected to the peripheral electrodes at intervals and extend toward the center of the emission hole.
可选地,所述栅线电极的宽度自所述外围电极朝所述发射孔内部逐渐减小。Optionally, the width of the gate line electrode gradually decreases from the peripheral electrode toward the interior of the emission hole.
可选地,所述上电极结构还包括若干根栅线连接电极,所述栅线连接电极设置于所述发射孔内,且所述与所述多根栅线电极中的若干根相连。Optionally, the upper electrode structure further includes several gate line connection electrodes, the gate line connection electrodes are arranged in the emission holes, and are connected to several of the plurality of gate line electrodes.
可选地,所述发射孔为圆形发射孔,所述栅线电极自所述外围电极朝所述发射孔的圆心延伸,所述栅线连接电极为圆环形栅线连接电极,所述圆环形栅线连接电极自所述外围电极朝所述发射孔的圆心方向直径逐渐减小,且各所述圆环形栅线连接电极均与所述若干栅线电极相连。Optionally, the emission hole is a circular emission hole, the grid electrode extends from the peripheral electrode toward the center of the emission hole, the grid connection electrode is a ring-shaped grid connection electrode, and the The diameter of the ring-shaped grid wire connecting electrodes gradually decreases from the peripheral electrode toward the center of the emission hole, and each of the ring-shaped grid wire connecting electrodes is connected to the plurality of grid wire electrodes.
可选地,所述多根栅线电极间隔连接于所述外围电极上,并在所述发射孔内平行排布。Optionally, the plurality of grid line electrodes are connected to the peripheral electrodes at intervals and arranged in parallel in the emission hole.
可选地,所述多根栅线电极形成偏振结构,通过调节多根栅线电极之间的间距,以调节所述垂直腔面发射激光器的出射光线的偏振度。Optionally, the plurality of grid electrodes form a polarization structure, and by adjusting the distance between the plurality of grid electrodes, the degree of polarization of the outgoing light of the vertical cavity surface emitting laser can be adjusted.
可选地,任意相邻的两根栅线电极之间的间距范围介于4微米~30微米之间。Optionally, the distance between any two adjacent grid line electrodes ranges from 4 microns to 30 microns.
可选地,所述栅线电极的宽度范围介于0.1微米~2微米之间,高度范围介于100纳米~5微米之间。Optionally, the grid electrode has a width ranging from 0.1 micron to 2 microns, and a height ranging from 100 nanometers to 5 microns.
可选地,所述栅线电极的数量不小于2根。Optionally, the number of the grid line electrodes is not less than 2.
可选地,所述发射孔的径向宽度不小于15微米。Optionally, the radial width of the emission hole is not less than 15 microns.
可选地,所述发射孔的径向宽度范围介于50微米~1000微米之间。Optionally, the emission hole has a radial width ranging from 50 microns to 1000 microns.
可选地,所述多根栅线电极与所述垂直腔面发射激光器的发射孔区域内的衬底、P型导电反射镜或N型导电反射镜形成欧姆接触。Optionally, the plurality of grid wire electrodes form ohmic contacts with the substrate, the P-type conductive mirror or the N-type conductive mirror in the region of the emission hole of the vertical cavity surface emitting laser.
可选地,所述垂直腔面发射激光器为正面发射结构,所述垂直腔面发射激光器还包括:衬底,所述衬底的背面具有下电极结构;N型导电下反射镜,位于所述衬底之上;有源层,位于所述N型导电下反射镜之上;P型导电上反射镜,位于所述有源层之上,所述P型导电上反射镜中具有电流限制层,并由所述电流限制层定义所述发射孔;以及介质层,位于所述P型导电上反射镜之上;其中,所述多根栅线电极穿过所述介质层并与所述P型导电上反射镜形成欧姆接触。Optionally, the vertical cavity surface emitting laser is a front emitting structure, and the vertical cavity surface emitting laser further includes: a substrate, the back of the substrate has a lower electrode structure; an N-type conductive lower reflector located on the On the substrate; the active layer is located on the N-type conductive lower reflector; the P-type conductive upper reflector is located on the active layer, and the P-type conductive upper reflector has a current confinement layer , and the emission hole is defined by the current confinement layer; and a dielectric layer is located on the P-type conductive upper mirror; wherein, the plurality of grid electrodes pass through the dielectric layer and are connected to the P Type conductive upper mirror forms an ohmic contact.
可选地,所述栅线电极包括自下而上的Ti层、Pt层及Au层所组成的叠层结构。Optionally, the gate electrode includes a stacked structure composed of a Ti layer, a Pt layer and an Au layer from bottom to top.
可选地,所述垂直腔面发射激光器为背面发射结构,所述垂直腔面发射激光器还包括:P型导电下反射镜,所述P型导电下反射镜的背面具有下电极结构;有源层,位于所述P型导电下反射镜之上;N型导电上反射镜,位于所述有源层之上,所述N型导电上反射镜中具有电流限制层,并由所述电流限制层定义所述发射孔;衬底,位于所述N型导电上反射镜之上;以及介质层,形成于所述衬底上;其中,所述多根栅线电极穿过所述介质层并与所述衬底形成欧姆接触。Optionally, the vertical cavity surface emitting laser is a back emitting structure, and the vertical cavity surface emitting laser further includes: a P-type conductive lower reflector, the back of the P-type conductive lower reflector has a lower electrode structure; Layer, located on the P-type conductive lower reflector; N-type conductive upper reflector, located on the active layer, the N-type conductive upper reflector has a current confinement layer, and is limited by the current A layer defines the emission hole; a substrate, located on the N-type conductive upper mirror; and a dielectric layer, formed on the substrate; wherein, the plurality of grid electrodes pass through the dielectric layer and Ohmic contacts are formed with the substrate.
可选地,所述栅线电极包括自下而上的Au层、Ge层、Ni层及Au层所组成的叠层结构。Optionally, the grid line electrode includes a stacked structure composed of Au layer, Ge layer, Ni layer and Au layer from bottom to top.
可选地,所述垂直腔面发射激光器为背面发射结构,所述垂直腔面发射激光器还包括:P型导电下反射镜,所述P型导电下反射镜的背面具有下电极结构;有源层,位于所述P型导电下反射镜之上;N型导电上反射镜,位于所述有源层之上,所述N型导电上反射镜中具有电流限制层,并由所述电流限制层定义所述发射孔;衬底,位于所述N型导电上反射镜之上,位于所述发射孔区域的所述衬底被去除形成发射空腔,以显露所述N型导电上反射镜;以及介质层,形成于显露的所述N型导电上反射镜之上;其中,所述多根栅线电极穿过所述介质层并与所述N型导电上反射镜形成欧姆接触。Optionally, the vertical cavity surface emitting laser is a back emitting structure, and the vertical cavity surface emitting laser further includes: a P-type conductive lower reflector, the back of the P-type conductive lower reflector has a lower electrode structure; Layer, located on the P-type conductive lower reflector; N-type conductive upper reflector, located on the active layer, the N-type conductive upper reflector has a current confinement layer, and is limited by the current The layer defines the emission hole; the substrate is located on the N-type conductive upper reflector, and the substrate located in the region of the emission hole is removed to form an emission cavity to expose the N-type conductive upper reflector and a dielectric layer formed on the exposed N-type conductive upper reflector; wherein, the plurality of grid electrodes pass through the dielectric layer and form ohmic contact with the N-type conductive upper reflector.
可选地,所述栅线电极包括自下而上的Au层、Ge层、Ni层及Au层所组成的叠层结构。Optionally, the grid line electrode includes a stacked structure composed of Au layer, Ge layer, Ni layer and Au layer from bottom to top.
可选地,所述电流限制层包括空气柱型电流限制结构、离子注入型电流限制结构、掩埋异质结型电流限制结构与氧化限型电流限制结构中的一种。Optionally, the current confinement layer includes one of an air column current confinement structure, an ion implantation current confinement structure, a buried heterojunction current confinement structure, and an oxidation-limitation current confinement structure.
本发明还提供一种激光雷达,所述激光雷达的光源采用如上所述垂直腔面发射激光器。The present invention also provides a laser radar. The light source of the laser radar adopts the above-mentioned vertical cavity surface emitting laser.
本发明还提供一种红外摄像头,所述红外摄像头的光源采用如上所述垂直腔面发射激光器。The present invention also provides an infrared camera, wherein the light source of the infrared camera adopts the above-mentioned vertical cavity surface emitting laser.
本发明还提供一种3D深度识别探测器,所述深度识别探测器的光源采用如上所述垂直腔面发射激光器。The present invention also provides a 3D depth recognition detector, the light source of the depth recognition detector adopts the above-mentioned vertical cavity surface emitting laser.
如上所述,本发明的金属网格大功率垂直腔面发射激光器,具有以下有益效果:As mentioned above, the metal grid high-power vertical cavity surface emitting laser of the present invention has the following beneficial effects:
本发明通过多根栅线电极,将大氧化孔径的垂直腔面发射激光器的以增加电流路径的方式分割成多个窄长块状区域,一方面可有效增加大氧化孔径的垂直腔面发射激光器的中部区域的电流密度,另一方面,电流可从所述多个栅线电极进行横向传播,大大提高了发光孔内的电流密度分布的均匀性,提高了转化效率。通过线宽和间距等参数的优化,本发明的垂直腔面发射激光器的转化效率可达30~50%。The present invention divides the vertical cavity surface emitting laser with large oxidation aperture into a plurality of narrow and long block-shaped regions by increasing the current path through a plurality of grid wire electrodes, on the one hand, it can effectively increase the vertical cavity surface emitting laser with large oxidation aperture The current density in the central region, on the other hand, the current can be transmitted laterally from the plurality of grid electrodes, which greatly improves the uniformity of the current density distribution in the luminescent hole and improves the conversion efficiency. Through the optimization of parameters such as line width and spacing, the conversion efficiency of the vertical cavity surface emitting laser of the present invention can reach 30-50%.
本发明上述的多个窄长块状区域位于同一发射孔内,具有连贯性,可以与衍射光学元件(DOE)配合,从而可以显著提高垂直腔面发射激光器的信噪比。同时,大范围的保持了出射光的相干性。该发明可以应用在激光雷达、红外摄像头和深度识别探测器等领域。The above-mentioned multiple narrow and long block-shaped regions of the present invention are located in the same emission hole, have coherence, and can cooperate with diffractive optical elements (DOE), so that the signal-to-noise ratio of the vertical cavity surface emitting laser can be significantly improved. At the same time, the coherence of the outgoing light is maintained in a wide range. The invention can be applied in fields such as laser radar, infrared camera and depth recognition detector.
本发明的栅线电极可同时实现电流注入的功能和光学偏振等功能,不需要额外增加光学元件便可实现激光器的光学偏振等,可有效降节约体积及成本。金属网格大功率垂直腔面发射激光器的结构及其制作方法。The grid line electrode of the present invention can realize the function of current injection and optical polarization at the same time, and can realize the optical polarization of the laser without adding additional optical elements, which can effectively reduce volume and cost. The structure and fabrication method of metal grid high power vertical cavity surface emitting laser.
本发明可有效提高垂直腔面发射激光器的功率密度,即提高了激光器或激光阵列在单位面积下的功率,在相同光功率要求下,可减小所需采用的激光器的数量,在实质上可提高芯片的集成度,并有效降低芯片的成本。The present invention can effectively improve the power density of the vertical cavity surface emitting laser, that is, the power per unit area of the laser or laser array is improved, and the number of lasers to be used can be reduced under the same optical power requirement, and the Improve the integration level of the chip and effectively reduce the cost of the chip.
附图说明Description of drawings
图1~图3显示为本发明的金属网格大功率垂直腔面发射激光器的上电极结构的示意图。1 to 3 are schematic diagrams showing the upper electrode structure of the metal grid high-power vertical cavity surface emitting laser of the present invention.
图4~图5显示为本发明的实施例1中的金属网格大功率垂直腔面发射激光器的结构示意图。4 to 5 are schematic structural diagrams of the metal grid high-power vertical cavity surface emitting laser in Embodiment 1 of the present invention.
图6显示为本发明实施例2中的一种金属网格大功率垂直腔面发射激光器的结构示意图。FIG. 6 is a schematic structural diagram of a metal grid high-power vertical-cavity surface-emitting laser in Embodiment 2 of the present invention.
图7显示为本发明实施例2中的另一种金属网格大功率垂直腔面发射激光器的结构示意图。FIG. 7 is a schematic structural diagram of another metal grid high-power vertical-cavity surface-emitting laser in Embodiment 2 of the present invention.
图8~图9分别显示为本发明的垂直腔面发射激光器与传统的金属网格大功率垂直腔面发射激光的电流注入分布示意图。8 to 9 are schematic diagrams showing the current injection distribution of the vertical cavity surface emitting laser of the present invention and the traditional metal grid high-power vertical cavity surface emitting laser, respectively.
图10~图11显示为本发明实施例3中的金属网格大功率垂直腔面发射激光器的结构示意图。10 to 11 are schematic structural diagrams of a metal grid high-power vertical cavity surface emitting laser in Embodiment 3 of the present invention.
元件标号说明Component designation description
100 发射孔100 embrasures
101 外围电极101 Peripheral electrodes
102 栅线电极102 grid electrode
103 栅线连接电极103 grid wire connection electrode
104 衬底104 substrate
105 下电极结构105 Bottom electrode structure
106 N型导电下反射镜106 N type conductive lower reflector
107 有源层107 active layer
108 P型导电上反射镜108 P type conductive upper reflector
109 电流限制层109 Current Limiting Layer
110 介质层110 medium layer
111 窄长块状区域111 Narrow and long blocky area
206 N型导电上反射镜206 N type conductive upper reflector
208 P型导电下反射镜208 P type conductive lower reflector
具体实施方式Detailed ways
以下通过特定的具体实例说明本发明的实施方式,本领域技术人员可由本说明书所揭露的内容轻易地了解本发明的其他优点与功效。本发明还可以通过另外不同的具体实施方式加以实施或应用,本说明书中的各项细节也可以基于不同观点与应用,在没有背离本发明的精神下进行各种修饰或改变。Embodiments of the present invention are described below through specific examples, and those skilled in the art can easily understand other advantages and effects of the present invention from the content disclosed in this specification. The present invention can also be implemented or applied through other different specific implementation modes, and various modifications or changes can be made to the details in this specification based on different viewpoints and applications without departing from the spirit of the present invention.
请参阅图1~图11。需要说明的是,本实施例中所提供的图示仅以示意方式说明本发明的基本构想,遂图示中仅显示与本发明中有关的组件而非按照实际实施时的组件数目、形状及尺寸绘制,其实际实施时各组件的型态、数量及比例可为一种随意的改变,且其组件布局型态也可能更为复杂。Please refer to Figure 1 to Figure 11. It should be noted that the diagrams provided in this embodiment are only schematically illustrating the basic idea of the present invention, so that only the components related to the present invention are shown in the diagrams rather than the number, shape and Dimensional drawing, the type, quantity and proportion of each component can be changed arbitrarily during actual implementation, and the component layout type may also be more complicated.
实施例1Example 1
如图1~图5所示,本实施例提供一种金属网格大功率垂直腔面发射激光器,经研究分析,现有的具有环形上电极结构的垂直腔面发射激光器,其电流注入时,电流会主要集中的发射孔100的边缘区域,而发射孔100的中部区域电流较小甚至是没有电流,发射孔100的边缘区域电流分布较为拥挤,而中部区域电几乎没有电流分布,会导致垂直腔面发射激光器的整体转换效率较低,发射孔100中的光强分布也不均匀。为了解决以上所发现的问题,本实施例提供一种垂直腔面发射激光器,所述垂直腔面发射激光器具有发射孔100以及上电极结构,所述发射孔100的径向宽度不小于15微米,所述上电极结构包括外围电极101以及多根栅线电极102,其中,所述外围电极101设置于所述发射孔100的外周,所述多根栅线电极102与所述外围电极101相连且延伸至所述发射孔100之内,如图1所示。As shown in Figures 1 to 5, this embodiment provides a metal grid high-power vertical cavity surface emitting laser. After research and analysis, the existing vertical cavity surface emitting laser with a ring-shaped upper electrode structure, when the current is injected, The current will mainly concentrate on the edge area of the emission hole 100, while the current in the middle area of the emission hole 100 is small or even has no current. The current distribution in the edge area of the emission hole 100 is relatively crowded, while the central area has almost no current distribution, which will lead to vertical The overall conversion efficiency of the cavity surface emitting laser is low, and the light intensity distribution in the emission hole 100 is not uniform. In order to solve the problems found above, this embodiment provides a vertical cavity surface emitting laser, the vertical cavity surface emitting laser has an emission hole 100 and an upper electrode structure, the radial width of the emission hole 100 is not less than 15 microns, The upper electrode structure includes a peripheral electrode 101 and a plurality of grid line electrodes 102, wherein the peripheral electrode 101 is arranged on the outer periphery of the emission hole 100, and the plurality of grid line electrodes 102 are connected to the peripheral electrode 101 and extending into the emission hole 100, as shown in FIG. 1 .
所述多根栅线电极102可以间隔连接于所述外围电极101上,并朝所述发射孔100的中心延伸。所述上电极结构还可以包括若干根栅线连接电极103,所述栅线连接电极103设置于所述发射孔100内,且所述与所述多根栅线电极102中的若干根相连。The plurality of gate electrodes 102 may be connected to the peripheral electrodes 101 at intervals, and extend toward the center of the emission hole 100 . The upper electrode structure may further include several gate line connecting electrodes 103 , the gate line connecting electrodes 103 are disposed in the emission holes 100 and connected to several of the plurality of gate line electrodes 102 .
所述栅线电极102与所述栅线连接电极103将可以将所述发射孔100分割成多个窄长块状区域111,多个窄长块状区域111位于同一发射孔100内,具有连贯性,各窄长块状区域111光线的相位基本相同,使得所述垂直腔面发射激光器可以与衍射光学元件(DOE)配合,从而可以显著提高垂直腔面发射激光器的信噪比。具体来说,对于传统的垂直腔面发射激光器阵列(VCSEL array)来说,其出射光线是不相干的,而且发光区域整体比较大,发光点之间的间隙也较大。本发明垂直腔面发射激光器采用单个大孔径的方式,其发光点是整体发光,可有效减小光斑,提高信噪比,同时保持激光的相干性,这样对于用DOE等光学组件有一定优势。另外,传统的边发射激光器有快轴和慢轴的区分,其光斑为椭圆形,而且快轴和慢轴的发散角不同,本发明与目前用于激光雷达的边发射激光器相比,又具有光斑为圆形,并且发散角为旋转对称的优点。The gate line electrode 102 and the gate line connection electrode 103 can divide the emission hole 100 into a plurality of narrow and long block-shaped regions 111, and the plurality of narrow and long block-shaped regions 111 are located in the same emission hole 100, with a continuous The phases of the light rays in the narrow and long block-shaped regions 111 are basically the same, so that the vertical cavity surface emitting laser can cooperate with diffractive optical elements (DOE), so that the signal-to-noise ratio of the vertical cavity surface emitting laser can be significantly improved. Specifically, for a traditional vertical cavity surface emitting laser array (VCSEL array), the emitted light is irrelevant, and the overall light-emitting area is relatively large, and the gap between light-emitting points is also relatively large. The vertical-cavity surface-emitting laser of the present invention adopts a single large-aperture mode, and its light-emitting point emits light as a whole, which can effectively reduce the light spot, improve the signal-to-noise ratio, and maintain the coherence of the laser, which has certain advantages for optical components such as DOE. In addition, the traditional edge-emitting laser has a distinction between the fast axis and the slow axis, and its light spot is elliptical, and the divergence angles of the fast axis and the slow axis are different. The light spot is circular, and the divergence angle is the advantage of rotational symmetry.
具体地,如图1所示,所述发射孔100为圆形发射孔100,所述栅线电极102自所述外围电极101朝所述发射孔100的圆心延伸,所述栅线连接电极103为圆环形栅线连接电极103,所述圆环形栅线连接电极103自所述外围电极101朝所述发射孔100的圆心方向直径逐渐减小,且各所述圆环形栅线连接电极103均与所述若干栅线电极102相连。对于发射孔100的径向宽度范围为15微米~200微米之间的垂直腔面发射激光器,其上电极结构可以采用如图1所示的结构,所述栅线电极102的数量优选为不小于2根,在如图1所示的示例中,所述栅线电极102的数量可以选择为8根,其等间距连接于所述外围电极101上,以提高电流的均匀性,该径向宽度范围内的垂直腔面发射激光器,所述栅线电极102的宽度可以为等宽设置,既能保证电流均匀性,同时可以降低栅线电极102的制造难度,降低工艺成本。所述圆环形栅线连接电极103的数量可以为3根等,各所述圆环形栅线连接电极103也优选为等间距排布于所述发射孔100中,且每根圆环形栅线连接电极103与所有的栅线电极102均相连,以降所述上电极结构的电阻,提高电流的注入密度。所述上电极结构可以采用如金属剥离工艺(lift-off)等制作。Specifically, as shown in FIG. 1, the emission hole 100 is a circular emission hole 100, the grid line electrode 102 extends from the peripheral electrode 101 toward the center of the emission hole 100, and the grid line connection electrode 103 It is a ring-shaped grid line connection electrode 103, and the diameter of the ring-shaped grid line connection electrode 103 gradually decreases from the peripheral electrode 101 toward the center of the emission hole 100, and each of the ring-shaped grid line connections The electrodes 103 are all connected to the plurality of grid line electrodes 102 . For vertical cavity surface emitting lasers with emission holes 100 whose radial width ranges from 15 microns to 200 microns, the upper electrode structure can be as shown in Figure 1, and the number of grid electrodes 102 is preferably not less than 2, in the example shown in Figure 1, the number of the grid line electrodes 102 can be selected as 8, which are connected to the peripheral electrodes 101 at equal intervals to improve the uniformity of the current, the radial width For the vertical cavity surface emitting laser within the range, the width of the grid line electrode 102 can be set at equal width, which can not only ensure the uniformity of the current, but also reduce the manufacturing difficulty of the grid line electrode 102 and reduce the process cost. The number of the ring-shaped grid line connection electrodes 103 can be 3, etc., and each of the ring-shaped grid line connection electrodes 103 is also preferably arranged at equal intervals in the emission hole 100, and each ring-shaped grid line The gate line connection electrode 103 is connected to all the gate line electrodes 102 to reduce the resistance of the upper electrode structure and increase the current injection density. The upper electrode structure can be fabricated by using, for example, a metal lift-off process.
当然,在其他的实施例中,所述发射孔100的形状也可以为矩形、椭圆形等或其他的所需形状,所述栅线电极102及所述栅线连接电极103也可以为波浪线、弧线等或其他所需的线条形状,并不限于此处所列举的示例。Certainly, in other embodiments, the shape of the emission hole 100 can also be rectangular, elliptical, etc. or other desired shapes, and the grid line electrode 102 and the grid line connecting electrode 103 can also be wavy lines , arcs, etc., or other desired line shapes are not limited to the examples listed here.
如图2及图3所示,对于发射孔100在200微米以上的垂直腔面发射激光器,所述栅线电极102的宽度可以设置为自所述外围电极101朝所述发射孔100内部逐渐减小,这种设置可以与发射孔100不同区域内的电流密度大小匹配,在保证电流有效注入的同时,降低由于栅线电极102的遮挡而造成的出射激光的损失,如图2所示。为了保证电流的有效注入,所述栅线电极102的数量也可以适当增加,如图3所示的发射孔100为400微米~1000微米的垂直腔面发射激光器,其栅线电极102的数量可以为32根或更多,其中,可以包含部分宽度较大且朝发射孔100中心逐渐减小的栅线电极102,以及部分等宽设置的栅线电极102。As shown in Figures 2 and 3, for a vertical cavity surface emitting laser with an emission hole 100 above 200 microns, the width of the gate electrode 102 can be set to gradually decrease from the peripheral electrode 101 toward the interior of the emission hole 100. This setting can match the current density in different regions of the emission hole 100, while ensuring the effective injection of current, and reducing the loss of the emitted laser light caused by the shielding of the grid electrode 102, as shown in FIG. 2 . In order to ensure the effective injection of current, the number of the grid line electrodes 102 can also be appropriately increased. The emission hole 100 shown in FIG. There are 32 or more grid electrodes 102 with a larger width and gradually decreasing towards the center of the emission hole 100 , and some grid electrodes 102 with equal width.
需要说明的是,数量较多的栅线电极102及栅线连接电极103可以更有效提高电流的注入强度及均匀性,但是会造成较大面积的激光遮挡,而导致激光的光强变弱,数量较少的栅线电极102,则可能不能满足电流注入强度的需求,因此,在本发明中,所述栅线电极102的数量优选为2~32根之间,所述栅线连接电极103的数量优选为2~12根之间,可依据发射孔100的径向宽度不同进行优化设计,并不限于图1~图3所列举的示例。It should be noted that a large number of grid line electrodes 102 and grid line connecting electrodes 103 can more effectively improve the injection intensity and uniformity of the current, but it will cause a large area of laser shielding, resulting in weakening of the laser light intensity. A small number of grid line electrodes 102 may not be able to meet the current injection strength requirements. Therefore, in the present invention, the number of the grid line electrodes 102 is preferably between 2 and 32, and the grid line connection electrodes 103 The number is preferably between 2 and 12, and can be optimally designed according to the radial width of the emission hole 100 , and is not limited to the examples listed in FIGS. 1 to 3 .
基于以上原理,本实施例对所述栅线电极102与栅线连接电极103的宽度和高度进行了优化,由于电极的电阻与其横截面积呈反比关系,即为了改善电极的电阻,需要一定程度增加其横截面积,但是,较大横截面积的电极,会造成更多的激光遮挡,本示例通过提高栅线电极102以及栅线连接电极103的高宽比,例如,将所述栅线电极102以及栅线连接电极103的高宽比设置为1:1~6:1之间,可以在降低栅线电极102以及栅线连接电极103的电阻的同时,大大降低其对出射激光的遮挡。在本实施例中,所述栅线电极102及所述栅线连接电极103的宽度范围可以介于0.1微米~2微米之间,高度范围可以介于100纳米~5微米之间。Based on the above principles, this embodiment optimizes the width and height of the grid line electrode 102 and the grid line connection electrode 103. Since the resistance of the electrode is inversely proportional to its cross-sectional area, that is, in order to improve the resistance of the electrode, a certain degree of Increase its cross-sectional area, but electrodes with a larger cross-sectional area will cause more laser shielding. In this example, by improving the aspect ratio of the grid line electrode 102 and the grid line connection electrode 103, for example, the grid line The aspect ratio of the electrode 102 and the grid line connection electrode 103 is set between 1:1 and 6:1, which can greatly reduce the shielding of the outgoing laser light while reducing the resistance of the grid line electrode 102 and the grid line connection electrode 103 . In this embodiment, the width range of the gate line electrodes 102 and the gate line connection electrodes 103 may be between 0.1 micrometers and 2 micrometers, and the height range may be between 100 nanometers and 5 micrometers.
图5显示为图4中A-A’处的截面结构示意图,所述垂直腔面发射激光器为正面发射结构,所述垂直腔面发射激光器包括衬底104、N型导电下反射镜106、有源层107、P型导电上反射镜108、介质层110以及上电极结构。FIG. 5 is a schematic diagram of a cross-sectional structure at AA' in FIG. The source layer 107, the P-type conductive upper mirror 108, the dielectric layer 110 and the upper electrode structure.
所述衬底104可以为砷化镓衬底104,所述衬底104的背面具有下电极结构105。The substrate 104 may be a gallium arsenide substrate 104 , and the backside of the substrate 104 has a lower electrode structure 105 .
所述N型导电下反射镜106位于所述衬底104之上,所述N型导电下反射镜106可以为N型导电的布拉格反射镜DBR,其主要的材料可以为砷化镓等。The N-type conductive lower reflector 106 is located on the substrate 104. The N-type conductive lower reflector 106 may be an N-type conductive Bragg reflector DBR, and its main material may be gallium arsenide or the like.
所述有源层107位于所述N型导电下反射镜106之上,所述有源层107用以将电能转换为光能,其材料可以为砷化镓等。The active layer 107 is located on the N-type conductive lower reflector 106. The active layer 107 is used to convert electric energy into light energy, and its material may be gallium arsenide or the like.
所述P型导电上反射镜108位于所述有源层107之上,所述P型导电上反射镜108中具有电流限制层109,并由所述电流限制层109定义所述发射孔100,所述P型导电上反射镜108可以为P型导电的布拉格反射镜DBR,其主要的材料可以为砷化镓等。所述N型导电下反射镜106及所述P型导电上反射镜108用于对所述有源层107产生的光线进行反射增强,最后形成激光从所述P型导电上反射镜108的表面射出。所述电流限制层109包括空气柱型电流限制结构、离子注入型电流限制结构、掩埋异质结型电流限制结构与氧化限型电流限制结构中的一种,在本实施例中,所述电流限制层109为氧化限型电流限制结构。The P-type conductive upper mirror 108 is located on the active layer 107, the P-type conductive upper mirror 108 has a current confinement layer 109 therein, and the emission hole 100 is defined by the current confinement layer 109, The P-type conductive upper reflector 108 may be a P-type conductive Bragg reflector DBR, and its main material may be gallium arsenide or the like. The N-type conductive lower reflector 106 and the P-type conductive upper reflector 108 are used to reflect and enhance the light generated by the active layer 107, and finally form a laser beam from the surface of the P-type conductive upper reflector 108. shoot out. The current confinement layer 109 includes one of an air column current confinement structure, an ion implantation current confinement structure, a buried heterojunction current confinement structure, and an oxidation-limited current confinement structure. In this embodiment, the current confinement The confinement layer 109 is an oxidation-limited current confinement structure.
所述介质层110位于所述P型导电上反射镜108之上,用于保护所述P型导电上反射镜108。The dielectric layer 110 is located on the P-type conductive upper reflector 108 for protecting the P-type conductive upper reflector 108 .
所述上电极结构位于所述介质层110之上,所述外围电极101穿过所述介质层110并与所述P型导电上反射镜108形成欧姆接触,所述多根栅线电极102及所述多根栅极连接线穿过所述介质层110并与所述P型导电上反射镜108形成欧姆接触。The upper electrode structure is located on the dielectric layer 110, the peripheral electrode 101 passes through the dielectric layer 110 and forms an ohmic contact with the P-type conductive upper mirror 108, the plurality of grid electrodes 102 and The plurality of gate connecting wires pass through the dielectric layer 110 and form an ohmic contact with the P-type conductive upper mirror 108 .
所述栅线电极102及所述栅线连接电极103可以包括自下而上的Ti层、Pt层及Au层所组成的叠层结构,该叠层结构可以与所述P型导电上反射镜108具有较好的结合强度,且形成欧姆接触后,具有较小的接触电阻。当然,所述栅线电极102及所述栅线连接电极103也可以由其他的金属叠层组成,并不限于此处所列举的示例。The grid line electrode 102 and the grid line connection electrode 103 may include a stacked structure composed of a Ti layer, a Pt layer and an Au layer from bottom to top, and the stacked structure may be connected to the P-type conductive upper mirror 108 has good bonding strength, and after forming an ohmic contact, it has a small contact resistance. Certainly, the gate line electrodes 102 and the gate line connection electrodes 103 may also be composed of other metal stacks, and are not limited to the examples listed here.
图9显示为图4中B-B’处的截面结构示意图,图9剪头为电流的注入示意曲线,图8剪头则为传统的垂直腔面发射激光器的电流的注入示意曲线,由图8及图9可见,传统的垂直腔面发射激光器发射孔100的边缘区域电流分布较为拥挤,而中部区域电几乎没有电流分布,会导致垂直腔面发射激光器的整体转换效率较低,而本发明的垂直腔面发射激光器,其电流可以有效注入至发射孔100的中部区域,一方面可有效增加大氧化孔径的垂直腔面发射激光器的中部区域的电流密度,另一方面,电流可从所述多个栅线电极102进行横向传播,大大提高了发光孔内的电流密度分布的均匀性,提高了转化效率。Fig. 9 is a schematic diagram of the cross-sectional structure at BB' in Fig. 4, Fig. 9 is a schematic diagram of current injection curve, and Fig. 8 is a schematic diagram of current injection curve of a traditional vertical cavity surface emitting laser, as shown in Fig. 8 and FIG. 9, it can be seen that the current distribution in the edge region of the emission hole 100 of the traditional vertical cavity surface emitting laser is relatively crowded, while there is almost no current distribution in the central region, which will lead to a low overall conversion efficiency of the vertical cavity surface emitting laser, and the present invention The vertical cavity surface emitting laser, its current can be effectively injected into the middle region of the emission hole 100, on the one hand, it can effectively increase the current density in the middle region of the vertical cavity surface emitting laser with a large oxide aperture, on the other hand, the current can be from the said Transverse propagation by multiple grid line electrodes 102 greatly improves the uniformity of the current density distribution in the luminescent hole and improves the conversion efficiency.
本实施例还提供一种激光雷达,其中,所述激光雷达的光源采用本实施例所述垂直腔面发射激光器。传统的边发射激光器有快轴和慢轴的区分,其光斑为椭圆形,而且快轴和慢轴的发散角不同,本发明与目前用于激光雷达的边发射激光器相比,具有光斑为圆形,并且发散角为旋转对称的优点。This embodiment also provides a laser radar, wherein the light source of the laser radar adopts the vertical cavity surface emitting laser described in this embodiment. The traditional edge-emitting laser has a distinction between the fast axis and the slow axis, and its light spot is elliptical, and the divergence angles of the fast axis and the slow axis are different. Compared with the edge-emitting laser currently used for lidar, the present invention has a circular light spot. shape, and the divergence angle is the advantage of rotational symmetry.
本实施例还提供一种红外摄像头,所述红外摄像头的光源采用如上所述垂直腔面发射激光器。This embodiment also provides an infrared camera, where the light source of the infrared camera adopts the above-mentioned vertical cavity surface emitting laser.
本实施例还提供一种3D深度识别探测器,所述深度识别探测器的光源采用如上所述垂直腔面发射激光器。This embodiment also provides a 3D depth recognition detector, the light source of the depth recognition detector adopts the above-mentioned vertical cavity surface emitting laser.
实施例2Example 2
如图4及图6所示,本实施例提供一种金属网格大功率垂直腔面发射激光器,其基本结构如实施例1,其中,与实施例1的不同之处在于,所述垂直腔面发射激光器为背面发射结构的垂直腔面发射激光器,所述垂直腔面发射激光器包括:P型导电下反射镜208,所述P型导电下反射镜208的背面具有下电极结构105;有源层107,位于所述P型导电下反射镜208之上;N型导电上反射镜206,位于所述有源层107之上,所述N型导电上反射镜206中具有电流限制层109,并由所述电流限制层109定义所述发射孔100;衬底104,位于所述N型导电上反射镜206之上;介质层110,形成于所述衬底104上;以及上电极结构,位于所述介质层110之上,所述外围电极101穿过所述介质层110并与所述衬底104形成欧姆接触,所述多根栅线电极102及所述多根栅极连接线穿过所述介质层110并与所述衬底104形成欧姆接触。所述栅线电极102包括自下而上的Au层、Ge层、Ni层及Au层所组成的叠层结构。当然,所述栅线电极102也可以由其他的金属叠层组成,并不限于此处所列举的示例。As shown in Figure 4 and Figure 6, this embodiment provides a metal grid high-power vertical cavity surface emitting laser, the basic structure of which is as in Embodiment 1, wherein the difference from Embodiment 1 is that the vertical cavity The surface-emitting laser is a vertical-cavity surface-emitting laser with a back-emitting structure, and the vertical-cavity surface-emitting laser includes: a P-type conductive lower reflector 208, and the back of the P-type conductive lower reflector 208 has a lower electrode structure 105; Layer 107, located on the P-type conductive lower reflector 208; N-type conductive upper reflector 206, located on the active layer 107, the N-type conductive upper reflector 206 has a current confinement layer 109, And the emission hole 100 is defined by the current confinement layer 109; the substrate 104 is located on the N-type conductive upper mirror 206; the dielectric layer 110 is formed on the substrate 104; and the upper electrode structure, Located on the dielectric layer 110, the peripheral electrode 101 passes through the dielectric layer 110 and forms an ohmic contact with the substrate 104, the plurality of gate electrodes 102 and the plurality of gate connection lines pass through through the dielectric layer 110 and form an ohmic contact with the substrate 104 . The grid line electrode 102 includes a stacked structure composed of Au layer, Ge layer, Ni layer and Au layer from bottom to top. Certainly, the gate electrode 102 may also be composed of other metal stacks, and is not limited to the examples listed here.
如图4及图7所示,本实施例还提供另一种垂直腔面发射激光器,所述垂直腔面发射激光器为背面发射结构的垂直腔面发射激光器,其包括所述垂直腔面发射激光器为背面发射结构,所述垂直腔面发射激光器包括:P型导电下反射镜208,所述P型导电下反射镜208的背面具有下电极结构105;有源层107,位于所述P型导电下反射镜208之上;N型导电上反射镜206,位于所述有源层107之上,所述N型导电上反射镜206中具有电流限制层109,并由所述电流限制层109定义所述发射孔100;衬底104,位于所述N型导电上反射镜206之上,位于所述发射孔100区域的所述衬底104被去除形成发射空腔,以显露所述N型导电上反射镜206;介质层110,形成于显露的所述N型导电上反射镜206之上;以及上电极结构,所述上电极结构的所述外围电极101与所述衬底104形成欧姆接触,所述上电极结构的所述多根栅线电极102及所述多根栅极连接线穿过所述介质层110并与所述N型导电上反射镜206形成欧姆接触。所述栅线电极102包括自下而上的Au层、Ge层、Ni层及Au层所组成的叠层结构。当然,所述栅线电极102也可以由其他的金属叠层组成,并不限于此处所列举的示例。As shown in Figure 4 and Figure 7, this embodiment also provides another vertical cavity surface emitting laser, the vertical cavity surface emitting laser is a vertical cavity surface emitting laser with a back emitting structure, which includes the vertical cavity surface emitting laser It is a back-emitting structure, and the vertical cavity surface-emitting laser includes: a P-type conductive lower reflector 208, and the back of the P-type conductive lower reflector 208 has a lower electrode structure 105; an active layer 107 is located on the P-type conductive On the lower reflector 208; N-type conductive upper reflector 206, located on the active layer 107, the N-type conductive upper reflector 206 has a current confinement layer 109, and is defined by the current confinement layer 109 The emission hole 100; the substrate 104 is located on the N-type conductive upper mirror 206, and the substrate 104 located in the region of the emission hole 100 is removed to form an emission cavity to reveal the N-type conductive An upper mirror 206; a dielectric layer 110 formed on the exposed N-type conductive upper mirror 206; and an upper electrode structure, the peripheral electrode 101 of the upper electrode structure forms an ohmic contact with the substrate 104 The plurality of gate electrodes 102 and the plurality of gate connection lines of the upper electrode structure pass through the dielectric layer 110 and form an ohmic contact with the N-type conductive upper mirror 206 . The grid line electrode 102 includes a stacked structure composed of Au layer, Ge layer, Ni layer and Au layer from bottom to top. Certainly, the gate electrode 102 may also be composed of other metal stacks, and is not limited to the examples listed here.
实施例3Example 3
如图10~图11所示,其中,图11显示为图10中C-C’处的截面结构示意图,本实施例提供一种金属网格大功率垂直腔面发射激光器,其基本结构如实施例1,其中,与实施例1的不同之处在于,所述上电极的所述多根栅线电极102间隔连接于所述外围电极101上,并在所述发射孔100内平行排布,藉由所述多根栅线电极102形成偏振结构,通过调节多根栅线电极102之间的间距,以调节所述垂直腔面发射激光器的出射光线的偏振度,例如,所述多根栅线电极102之间的间距越小,则所述垂直腔面发射激光器最终出射的激光的偏振度越高,所述多根栅线电极102之间的间距越大,则所述垂直腔面发射激光器最终出射的激光的偏振度越低。优选地,任意相邻的两根栅线电极102之间的间距范围介于4微米~30微米之间,所述栅线电极102的宽度范围介于0.1微米~2微米之间,高度范围介于100纳米~5微米之间。As shown in Figures 10 to 11, among them, Figure 11 shows a schematic cross-sectional structure at CC' in Figure 10. This embodiment provides a metal grid high-power vertical cavity surface emitting laser, and its basic structure is as shown in the implementation Example 1, wherein, the difference from Example 1 is that the plurality of gate electrodes 102 of the upper electrode are connected to the peripheral electrode 101 at intervals and arranged in parallel in the emission hole 100, The polarization structure is formed by the plurality of grid electrodes 102, and the polarization degree of the outgoing light of the vertical cavity surface emitting laser is adjusted by adjusting the distance between the plurality of grid electrodes 102, for example, the plurality of grid electrodes 102 The smaller the spacing between the wire electrodes 102, the higher the degree of polarization of the laser light finally emitted by the vertical cavity surface emitting laser, and the larger the spacing between the plurality of grid wire electrodes 102, the higher the polarization degree of the vertical cavity surface emitting laser. The lower the degree of polarization of the laser light finally emitted by the laser. Preferably, the distance between any two adjacent grid line electrodes 102 is between 4 microns and 30 microns, the width of the grid line electrodes 102 is between 0.1 micron and 2 microns, and the height is between 0.1 micron and 2 microns. Between 100 nanometers and 5 microns.
本实施例的栅线电极102可同时实现电流注入的功能和光学偏振等功能,不需要额外增加光学元件便可实现激光器的光学偏振等,可有效降节约体积及成本。The grid wire electrode 102 of this embodiment can realize the functions of current injection and optical polarization at the same time, and can realize the optical polarization of the laser without adding additional optical elements, which can effectively reduce volume and cost.
如上所述,本发明的金属网格大功率垂直腔面发射激光器,具有以下有益效果:As mentioned above, the metal grid high-power vertical cavity surface emitting laser of the present invention has the following beneficial effects:
本发明通过多根栅线电极102,将大氧化孔径的垂直腔面发射激光器的以增加电流路径的方式分割成多个窄长块状区域111,一方面可有效增加大氧化孔径的垂直腔面发射激光器的中部区域的电流密度,另一方面,电流可从所述多个栅线电极102进行横向传播,大大提高了发光孔内的电流密度分布的均匀性,提高了转化效率,本发明的垂直腔面发射激光器的转化效率通常可以达到30%以上,甚至40-50%,取决于优化的程度(是否可以做到均匀注入电流的同时遮光最小)。The present invention divides the vertical cavity surface emitting laser with large oxidation aperture into a plurality of narrow and long block regions 111 by increasing the current path through multiple gate electrodes 102, on the one hand, it can effectively increase the vertical cavity surface with large oxidation aperture The current density of the middle region of the emitting laser, on the other hand, the current can be transmitted laterally from the plurality of grid electrodes 102, which greatly improves the uniformity of the current density distribution in the light-emitting hole and improves the conversion efficiency. The conversion efficiency of vertical cavity surface emitting lasers can usually reach more than 30%, or even 40-50%, depending on the degree of optimization (whether uniform injection current can be achieved while shading is minimized).
本发明上述的多个窄长块状区域111位于同一发射孔100内,具有连贯性,可以与衍射光学元件(DOE)配合,从而可以显著提高垂直腔面发射激光器的信噪比。同时,大范围的保持了出射光的相干性。该发明可以应用在激光雷达、红外摄像头和深度识别探测器等领域。The above-mentioned multiple narrow and long block regions 111 of the present invention are located in the same emission hole 100 and are coherent, and can cooperate with diffractive optical elements (DOE), thereby significantly improving the signal-to-noise ratio of the vertical cavity surface emitting laser. At the same time, the coherence of the outgoing light is maintained in a wide range. The invention can be applied in fields such as laser radar, infrared camera and depth recognition detector.
本发明的栅线电极102可同时实现电流注入的功能和光学偏振等功能,不需要额外增加光学元件便可实现激光器的光学偏振等,可有效降节约体积及成本。The grid wire electrode 102 of the present invention can realize the functions of current injection and optical polarization at the same time, and realize the optical polarization of the laser without adding additional optical elements, which can effectively reduce volume and cost.
本发明可有效提高垂直腔面发射激光器的功率密度,即提高了激光器或激光阵列在单位面积下的功率,在相同光功率要求下,可减小所需采用的激光器的数量,在实质上可提高芯片的集成度,并有效降低芯片的成本。The present invention can effectively improve the power density of the vertical cavity surface emitting laser, that is, the power per unit area of the laser or laser array is improved, and the number of lasers to be used can be reduced under the same optical power requirement, and the Improve the integration level of the chip and effectively reduce the cost of the chip.
所以,本发明有效克服了现有技术中的种种缺点而具高度产业利用价值。Therefore, the present invention effectively overcomes various shortcomings in the prior art and has high industrial application value.
上述实施例仅例示性说明本发明的原理及其功效,而非用于限制本发明。任何熟悉此技术的人士皆可在不违背本发明的精神及范畴下,对上述实施例进行修饰或改变。因此,举凡所属技术领域中具有通常知识者在未脱离本发明所揭示的精神与技术思想下所完成的一切等效修饰或改变,仍应由本发明的权利要求所涵盖。The above-mentioned embodiments only illustrate the principles and effects of the present invention, but are not intended to limit the present invention. Anyone skilled in the art can modify or change the above-mentioned embodiments without departing from the spirit and scope of the present invention. Therefore, all equivalent modifications or changes made by those skilled in the art without departing from the spirit and technical ideas disclosed in the present invention shall still be covered by the claims of the present invention.
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CN109326958A (en) | 2019-02-12 |
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