WO2021056617A1 - Semiconductor laser and carrier injection method therefor - Google Patents

Semiconductor laser and carrier injection method therefor Download PDF

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WO2021056617A1
WO2021056617A1 PCT/CN2019/111045 CN2019111045W WO2021056617A1 WO 2021056617 A1 WO2021056617 A1 WO 2021056617A1 CN 2019111045 W CN2019111045 W CN 2019111045W WO 2021056617 A1 WO2021056617 A1 WO 2021056617A1
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semiconductor laser
dielectric film
ridge
film
cavity
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PCT/CN2019/111045
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French (fr)
Chinese (zh)
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王俊
赵智德
谭少阳
程洋
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苏州长光华芯半导体激光创新研究院有限公司
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Publication of WO2021056617A1 publication Critical patent/WO2021056617A1/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/06Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/0604Arrangements for controlling the laser output parameters, e.g. by operating on the active medium comprising a non-linear region, e.g. generating harmonics of the laser frequency
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
    • H01S5/22Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers having a ridge or stripe structure

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  • This application relates to the technical field of semiconductor lasers, in particular to a semiconductor laser and a carrier injection method thereof.
  • the traditional semiconductor laser adopts a uniform carrier injection scheme, and the electrodes are uniformly distributed along the longitudinal direction, so that the carrier density of the entire ridge injection is completely consistent.
  • the two ends of the laser will be treated with anti-reflection (AR) film and high-reflection (HR) film respectively, so that the laser is concentrated on the end of the anti-reflection film.
  • AR anti-reflection
  • HR high-reflection
  • the injection current is less than the threshold current, the photon density in the semiconductor laser cavity is very low, so it shows a uniform distribution along the longitudinal direction (AR cavity surface to HR cavity surface); when the injection current is greater than the threshold current, the laser starts lasing.
  • the photon density in the resonant cavity will gradually increase as the injection current increases, and the photon density in the laser resonant cavity shows a gradual decrease along the longitudinal direction (AR cavity surface to HR cavity surface). Due to the effect of stimulated emission, the higher the photon density, the faster the carrier consumption rate and the lower the carrier density. Therefore, the carrier density will gradually increase from the AR cavity surface to the HR cavity surface. Trend, the uneven distribution of the carrier density along the longitudinal direction will cause the uneven distribution of the gain in the longitudinal direction, leading to the degradation of the semiconductor laser performance and the decrease of the optical output power.
  • the present application provides a semiconductor laser and a carrier injection method thereof, which overcomes the non-uniform distribution of carrier density along the longitudinal direction in the prior art, which can cause the non-uniform distribution of gain in the longitudinal direction, which leads to the degradation of semiconductor laser performance and light emission. Insufficient output power drop.
  • an embodiment of the present application provides a carrier injection method for a semiconductor laser, including: preparing a semiconductor laser epitaxial structure on a substrate to obtain an epitaxial structure wafer; preparing a ridge structure of the semiconductor laser on the wafer ; Preparation of dielectric film on the ridge structure; etching of the dielectric film on the ridge surface of the ridge structure to form a dielectric film with a non-uniform shape distribution along the longitudinal direction; preparation of electrodes on the dielectric film; Carry out cleavage, and prepare anti-reflection film and high-reflection film on the front and back ends of the cleavage surface respectively; from the anti-reflection film cavity surface to the high-reflection film cavity surface, carry out carrier injection of the semiconductor laser.
  • the step of etching the dielectric film on the ridge surface of the ridge structure to form a dielectric film with a non-uniform shape distribution along the longitudinal direction includes: obtaining a current carrier when the semiconductor laser is uniformly injected into the electrode According to the non-linear distribution curve of carriers, the ridge surface of the ridge structure is divided into multiple regions along the longitudinal direction, and the non-uniform shape distribution of the dielectric film in each region The area ratio gradually increases from the surface of the anti-reflective film cavity to the surface of the high-reflective film cavity.
  • the area of the dielectric film with non-uniform shape distribution in each section of the region is not completely the same.
  • the length of the division of the region close to the cavity surface of the high-reflective film is shorter than the length of the division of the region close to the cavity surface of the anti-reflective film.
  • the length of the dielectric film in each region is determined according to the cavity length of the semiconductor laser, the reflectivity of the anti-reflection film cavity surface and the high-reflection film cavity surface, the working current and the nonlinear distribution curve of carriers.
  • the present application provides a semiconductor laser, including: a substrate; a semiconductor laser epitaxial structure formed on the substrate; a ridge structure formed on the epitaxial structure; a dielectric film formed on the ridge Structurally; a dielectric film with a longitudinal non-uniform shape distribution is formed above the ridge surface of the ridge structure; an electrode is formed on the dielectric film; an anti-reflection film and a high-reflection film are formed on the front and rear surfaces of the cleavage surface of the epitaxial structure .
  • the area ratio of the dielectric film distributed in a longitudinally non-uniform shape gradually increases from the cavity surface of the anti-reflection film to the cavity surface of the high-reflection film.
  • the areas of the dielectric films with longitudinal non-uniform shape distribution are not completely the same.
  • the shape of the dielectric film with longitudinal non-uniform shape distribution is polygonal, circular or elliptical.
  • the carrier injection method of the semiconductor laser controls the actual current injection area by controlling the shape of the dielectric film above the ridge surface, and realizes the non-uniform injection of current along the longitudinal direction of the ridge, thereby offsetting the long cavity length and the cavity at both ends.
  • the non-uniform distribution of carriers caused by the difference in surface reflectivity improves the uniformity of the longitudinal distribution of the gain in the working state of the semiconductor laser, and improves the optical output power of the semiconductor laser.
  • Fig. 1 is a flowchart of an example of a carrier injection method of a semiconductor laser provided by an embodiment of the application;
  • FIG. 2 is a schematic diagram of a substrate and an epitaxial structure wafer provided by an embodiment of the application;
  • Figure 3 is a schematic diagram of a ridge structure provided by an embodiment of the application.
  • FIG. 4 is a schematic diagram of a dielectric film provided by an embodiment of the application.
  • FIG. 5 is a schematic diagram of a dielectric film with a non-uniform shape distribution provided by an embodiment of the application.
  • FIG. 6 is a schematic diagram of an electrode structure provided by an embodiment of the application.
  • FIG. 7 is a schematic diagram of an AR cavity surface and an HR cavity surface provided by an embodiment of the application.
  • FIG. 8 is an example flow chart of forming a dielectric film with a non-uniform shape distribution according to an embodiment of the application
  • FIG. 9 is a schematic diagram of a non-linear distribution curve diagram of carriers when the electrodes are uniformly injected according to an embodiment of the application.
  • FIG. 10 is a cross-sectional view of a dielectric film with a non-uniform shape distribution provided by an embodiment of the application;
  • FIG. 11 is a comparison diagram of the longitudinal distribution of the carrier concentration of the ridges divided by equal length and unequal length according to the embodiment of the application;
  • FIG. 12 is a schematic structural diagram of a semiconductor laser provided by an embodiment of the application.
  • connection should be understood in a broad sense, unless otherwise clearly specified and limited.
  • it can be a fixed connection or a detachable connection.
  • Connected or integrally connected it can be a mechanical connection or an electrical connection; it can be directly connected, or indirectly connected through an intermediate medium, or it can be the internal connection of the two components, it can be a wireless connection, or it can be a wired connection connection.
  • the specific meanings of the above-mentioned terms in this application can be understood under specific circumstances.
  • An embodiment of the present application provides a carrier injection method for a semiconductor laser, as shown in FIG. 1, including:
  • Step S1 Prepare a semiconductor laser epitaxial structure on a substrate to obtain an epitaxial structure wafer.
  • the existing MOCVD, MBE and other equipment can be used to grow the semiconductor laser epitaxial structure on the substrate, as shown in FIG. 2, to obtain the laser epitaxial structure wafer.
  • Step S2 preparing the ridge structure of the semiconductor laser on the wafer.
  • a ridge structure is prepared on a wafer by photolithography.
  • the ridge structure can be a trapezoidal structure with a height in the middle part and two sides.
  • it may be a ridge structure with other shapes.
  • Step S3 preparing a dielectric film on the ridge structure.
  • the material of the dielectric film may be SiO 2 or SiN.
  • the prepared dielectric film covers the entire surface of the ridge structure.
  • Step S4 etching the dielectric film on the ridge surface of the ridge structure to form a dielectric film with a non-uniform shape distribution along the longitudinal direction.
  • the dielectric film is etched on the ridge surface of the ridge structure by photolithography, so that the dielectric film on the ridge surface has a non-uniform shape distribution, so that it can be evenly distributed during carrier injection.
  • the non-uniform shape distribution of the dielectric film formed on it is shown in Figure 5.
  • Step S5 preparing electrodes on the dielectric film.
  • an electrode structure formed by a metal electrode is formed on a dielectric thin film by deposition.
  • Step S6 The wafer is cleaved, and anti-reflection films and high-reflection films are prepared on the front and back ends of the cleaved surface respectively.
  • an anti-reflection (AR) film and a high-reflection (HR) film can be formed on the front and rear ends of the cleavage surface by evaporation. Form AR cavity surface and HR cavity surface.
  • Step S7 Perform carrier injection of the semiconductor laser from the surface of the anti-reflective film cavity to the surface of the high-reflective film cavity.
  • the carrier injection method of a semiconductor laser provided in this application is to etch the dielectric film on the ridge surface. Only the surface of the wafer that is not covered with the dielectric film on the ridge can contact the metal electrode, thus along the longitudinal direction. Non-uniform carrier injection can be obtained, and the patterned electrode is used to achieve non-uniform injection of carriers, thereby offsetting the non-uniform distribution of carriers caused by the long cavity length and the difference in the reflectivity of the cavity surfaces at both ends, and improving the working state of the semiconductor laser The uniformity of the lower gain along the longitudinal distribution improves the optical output power of the semiconductor laser.
  • the specific process of performing step S4, as shown in FIG. 8, includes:
  • Step S41 Obtain a nonlinear distribution curve of carriers when the semiconductor laser is uniformly injected into the electrode.
  • the laser starts lasing.
  • the photon density in the cavity will gradually increase with the increase of the injection current, and the photon density in the laser cavity is along the longitudinal direction (AR cavity surface to HR cavity The surface) shows a gradually decreasing trend, resulting in a lower carrier concentration on the AR side, and a higher carrier concentration on the high-reflective film (HR) side, as shown in Figure 9
  • the carrier is a non-linear distribution curve.
  • Step S42 According to the non-linear distribution curve of carriers, the ridge surface of the ridge structure is divided into multiple sections along the longitudinal direction, and the area of the non-uniformly distributed dielectric film in each section is It gradually increases from the surface of the anti-reflective film cavity to the surface of the high-reflective film cavity.
  • the area ratio of the dielectric film is the area of the dielectric film/the area of the small area.
  • the ridge structure is divided into three parts from left to right, and the middle part is the ridge surface.
  • the dielectric film above the ridge surface is not completely removed and is divided into several regions.
  • the area of the dielectric film distributed in non-uniform shapes in each region is not exactly the same, and along the AR
  • the longitudinal direction from the cavity surface to the HR cavity surface increases linearly.
  • the length of the region division close to the high-reflection film cavity surface is shorter than the length of the region division close to the anti-reflection film cavity surface.
  • the present application can effectively improve the uniformity of the carrier concentration and gain along the longitudinal distribution, by increasing the optical output power of the semiconductor laser by 10%.
  • An embodiment of the present application provides a semiconductor laser, as shown in FIG. 12, comprising: a substrate; a semiconductor laser epitaxial structure formed on the substrate; a ridge structure formed on the epitaxial structure; a dielectric film formed on the substrate On the ridge structure; a dielectric film with a longitudinal non-uniform shape distribution is formed above the ridge surface of the ridge structure; an electrode is formed on the dielectric film; an anti-reflection film and a high-reflection film are formed on the cleavage of the epitaxial structure The front and rear faces of the face.
  • the area ratio of the dielectric film distributed in the longitudinal non-uniform shape gradually increases along the direction from the cavity surface of the anti-reflective film to the cavity surface of the high-reflection film, and the area of the dielectric film distributed in the longitudinal non-uniform shape is different.
  • the arrangement of the dielectric film with exactly the same, non-uniform shape distribution is shown in Figure 10.
  • the ridge structure is divided into three parts from left to right.
  • the middle part is the ridge surface, and the area close to the HR cavity surface is divided into long sections.
  • the region near the AR cavity surface is divided into longer length regions.
  • the specific length should be determined according to the laser cavity length, the reflectivity of the cavity surfaces at both ends, the operating current, and the carrier distribution curve.
  • the dielectric film that is not etched in FIG. 10 is rectangular, which is only an example, and is not limited to this. In other embodiments, it may be elliptical, circular, or other polygonal shapes.
  • the shape of the non-uniformly distributed dielectric film is arranged above the ridge surface to control the actual current injection area, so as to realize the non-uniform injection of current along the longitudinal direction of the ridge, thereby offsetting the long cavity length and both ends.
  • the non-uniform distribution of carriers caused by the difference in the reflectivity of the cavity surface improves the uniformity of the longitudinal distribution of the gain in the working state of the semiconductor laser, and improves the optical output power of the semiconductor laser.

Abstract

A semiconductor laser and a carrier injection method therefor. The method comprises: preparing a semiconductor laser epitaxial structure on a substrate, and obtaining an epitaxial structure wafer (S1); preparing a ridge-shaped structure of the semiconductor laser on the wafer (S2); preparing a dielectric film on the ridge-shaped structure (S3); etching the dielectric film on a ridge surface of the ridge-shaped structure to form a dielectric film which is distributed in a non-uniform shape along a longitudinal direction (S4); preparing an electrode on the dielectric film (S5); cleaving the wafer, and respectively preparing an anti-reflection film and a high-reflection film at a front end and a rear end of a cleaved surface (S6); and carrying out carrier injection from an anti-reflection film cavity surface to a high-reflection film cavity surface (S7). By controlling the shape of the dielectric film on the ridge surface, non-uniform injection of current along the longitudinal direction of the ridge is realized, and therefore, carrier non-uniform distribution caused by long cavity length and the reflectivity difference of the cavity surfaces at the two ends is offset, the distribution uniformity of gains of the semiconductor laser along a longitudinal direction under a working state is improved, and the light output power of the semiconductor laser is improved.

Description

一种半导体激光器及其载流子注入方法Semiconductor laser and its carrier injection method 技术领域Technical field
本申请涉及半导体激光器技术领域,具体涉及一种半导体激光器及其载流子注入方法。This application relates to the technical field of semiconductor lasers, in particular to a semiconductor laser and a carrier injection method thereof.
背景技术Background technique
传统的半导体激光器采用载流子均匀注入的方案,将电极沿纵向均匀分布,使得整个脊形注入的载流子密度是完全一致。为了提高斜率效率及最大化输出功率,激光器的两端会分别作减反(AR)膜和高反(HR)膜处理,让激光集中在减反膜这端出射。当注入电流小于阈值电流时,半导体激光器谐振腔内的光子密度很低,因而沿纵向(AR腔面到HR腔面)呈现出均匀的分布;当注入电流大于阈值电流时,激光器开始激射,谐振腔内的光子密度会随着注入电流的增加而逐渐增加,且激光器谐振腔内的光子密度沿纵向(AR腔面到HR腔面)呈现出逐渐减小的趋势。由于受激辐射效应的影响,光子密度越高的区域,载流子的消耗速度越快,载流子的密度越低,因而载流子密度沿AR腔面到HR腔面会呈现出逐渐增加的趋势,载流子密度沿纵向的不均匀分布会引起增益在纵向的不均匀分布,导致半导体激光器性能退化、光输出功率下降。The traditional semiconductor laser adopts a uniform carrier injection scheme, and the electrodes are uniformly distributed along the longitudinal direction, so that the carrier density of the entire ridge injection is completely consistent. In order to improve the slope efficiency and maximize the output power, the two ends of the laser will be treated with anti-reflection (AR) film and high-reflection (HR) film respectively, so that the laser is concentrated on the end of the anti-reflection film. When the injection current is less than the threshold current, the photon density in the semiconductor laser cavity is very low, so it shows a uniform distribution along the longitudinal direction (AR cavity surface to HR cavity surface); when the injection current is greater than the threshold current, the laser starts lasing. The photon density in the resonant cavity will gradually increase as the injection current increases, and the photon density in the laser resonant cavity shows a gradual decrease along the longitudinal direction (AR cavity surface to HR cavity surface). Due to the effect of stimulated emission, the higher the photon density, the faster the carrier consumption rate and the lower the carrier density. Therefore, the carrier density will gradually increase from the AR cavity surface to the HR cavity surface. Trend, the uneven distribution of the carrier density along the longitudinal direction will cause the uneven distribution of the gain in the longitudinal direction, leading to the degradation of the semiconductor laser performance and the decrease of the optical output power.
发明内容Summary of the invention
因此,本申请提供一种半导体激光器及其载流子注入方法,克服了现有技术中载流子密度沿纵向的不均匀分布会引起增益在纵向的不均匀分布, 导致半导体激光器性能退化、光输出功率下降的不足。Therefore, the present application provides a semiconductor laser and a carrier injection method thereof, which overcomes the non-uniform distribution of carrier density along the longitudinal direction in the prior art, which can cause the non-uniform distribution of gain in the longitudinal direction, which leads to the degradation of semiconductor laser performance and light emission. Insufficient output power drop.
第一方面,本申请实施例提供一种半导体激光器的载流子注入方法,包括:在衬底上制备半导体激光器外延结构,获取外延结构晶圆片;在晶圆片上制备半导体激光器的脊形结构;在脊形结构上制备介质薄膜;将位于脊形结构脊面上的介质薄膜进行刻蚀处理,形成沿纵向方向的非均匀形状分布的介质薄膜;在介质薄膜上制备电极;将晶圆片进行解理,并在解理面的前后两端分别制备减反薄膜及高反薄膜;从减反薄膜腔面到高反薄膜腔面进行半导体激光器的载流子注入。In the first aspect, an embodiment of the present application provides a carrier injection method for a semiconductor laser, including: preparing a semiconductor laser epitaxial structure on a substrate to obtain an epitaxial structure wafer; preparing a ridge structure of the semiconductor laser on the wafer ; Preparation of dielectric film on the ridge structure; etching of the dielectric film on the ridge surface of the ridge structure to form a dielectric film with a non-uniform shape distribution along the longitudinal direction; preparation of electrodes on the dielectric film; Carry out cleavage, and prepare anti-reflection film and high-reflection film on the front and back ends of the cleavage surface respectively; from the anti-reflection film cavity surface to the high-reflection film cavity surface, carry out carrier injection of the semiconductor laser.
在一实施例中,所述将位于脊形结构脊面上的介质薄膜进行刻蚀处理,形成沿纵向方向的非均匀形状分布的介质薄膜的步骤,包括:获取半导体激光器均匀注入电极时载流子的非线性分布曲线;根据所述载流子的非线性分布曲线,将脊形结构的脊形结构脊面分沿纵向方向分割成多段区域,每段区域中非均匀形状分布的介质薄膜的面积占比,沿减反薄膜腔面到高反薄膜腔面的方向逐渐增加。In an embodiment, the step of etching the dielectric film on the ridge surface of the ridge structure to form a dielectric film with a non-uniform shape distribution along the longitudinal direction includes: obtaining a current carrier when the semiconductor laser is uniformly injected into the electrode According to the non-linear distribution curve of carriers, the ridge surface of the ridge structure is divided into multiple regions along the longitudinal direction, and the non-uniform shape distribution of the dielectric film in each region The area ratio gradually increases from the surface of the anti-reflective film cavity to the surface of the high-reflective film cavity.
在一实施例中,每段区域中非均匀形状分布的介质薄膜的面积不完全相同。In one embodiment, the area of the dielectric film with non-uniform shape distribution in each section of the region is not completely the same.
在一实施例中,靠近高反薄膜腔面的区域分割的长度比靠近减反薄膜腔面的区域分割的长度短。In one embodiment, the length of the division of the region close to the cavity surface of the high-reflective film is shorter than the length of the division of the region close to the cavity surface of the anti-reflective film.
在一实施例中,根据半导体激光器的腔长、减反薄膜腔面和高反薄膜腔面反射率、工作电流及载流子的非线性分布曲线确定每段区域中介质薄膜的长度。In an embodiment, the length of the dielectric film in each region is determined according to the cavity length of the semiconductor laser, the reflectivity of the anti-reflection film cavity surface and the high-reflection film cavity surface, the working current and the nonlinear distribution curve of carriers.
第二方面,本申请提供一种半导体激光器,包括:衬底;半导体激光器 外延结构,形成于所述衬底上;脊形结构,形成所述外延结构上;介质薄膜,形成于所述脊形结构上;纵向非均匀形状分布的介质薄膜,形成于脊形结构的脊面上方;电极,形成于所述介质薄膜上;减反膜和高反膜,形成于外延结构解理面的前后端面。In a second aspect, the present application provides a semiconductor laser, including: a substrate; a semiconductor laser epitaxial structure formed on the substrate; a ridge structure formed on the epitaxial structure; a dielectric film formed on the ridge Structurally; a dielectric film with a longitudinal non-uniform shape distribution is formed above the ridge surface of the ridge structure; an electrode is formed on the dielectric film; an anti-reflection film and a high-reflection film are formed on the front and rear surfaces of the cleavage surface of the epitaxial structure .
在一实施例中,所述纵向非均匀形状分布的介质薄膜的面积占比,沿减反薄膜腔面到高反薄膜腔面的方向逐渐增加。In an embodiment, the area ratio of the dielectric film distributed in a longitudinally non-uniform shape gradually increases from the cavity surface of the anti-reflection film to the cavity surface of the high-reflection film.
在一实施例中,所述纵向非均匀形状分布的介质薄膜的面积不完全相同。In one embodiment, the areas of the dielectric films with longitudinal non-uniform shape distribution are not completely the same.
在一实施例中,所述纵向非均匀形状分布的介质薄膜的形状为多边形、圆形或椭圆形。In an embodiment, the shape of the dielectric film with longitudinal non-uniform shape distribution is polygonal, circular or elliptical.
本申请技术方案,具有如下优点:The technical solution of this application has the following advantages:
本申请提供的半导体激光器其载流子注入方法,通过控制脊面上方介质薄膜的形状,控制实际电流注入的区域,实现电流沿脊形纵向的非均匀注入,从而抵消长腔长、两端腔面反射率差异引起的载流子非均匀分布,提升半导体激光器工作状态下增益沿纵向分布的均匀性,提高半导体激光器的光输出功率。The carrier injection method of the semiconductor laser provided by this application controls the actual current injection area by controlling the shape of the dielectric film above the ridge surface, and realizes the non-uniform injection of current along the longitudinal direction of the ridge, thereby offsetting the long cavity length and the cavity at both ends. The non-uniform distribution of carriers caused by the difference in surface reflectivity improves the uniformity of the longitudinal distribution of the gain in the working state of the semiconductor laser, and improves the optical output power of the semiconductor laser.
附图说明Description of the drawings
为了更清楚地说明本申请具体实施方式或现有技术中的技术方案,下面将对具体实施方式或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图是本申请的一些实施方式,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the specific embodiments of this application or the technical solutions in the prior art, the following will briefly introduce the drawings that need to be used in the specific embodiments or the description of the prior art. Obviously, the appendix in the following description The drawings are some embodiments of the application. For those of ordinary skill in the art, other drawings can be obtained based on these drawings without creative work.
图1为本申请实施例提供的半导体激光器的载流子注入方法一个示例 流程图;Fig. 1 is a flowchart of an example of a carrier injection method of a semiconductor laser provided by an embodiment of the application;
图2为本申请实施例提供的衬底及外延结构晶圆片的示意图;2 is a schematic diagram of a substrate and an epitaxial structure wafer provided by an embodiment of the application;
图3为本申请实施例提供的脊形结构的示意图;Figure 3 is a schematic diagram of a ridge structure provided by an embodiment of the application;
图4为本申请实施例提供的介质薄膜的示意图;4 is a schematic diagram of a dielectric film provided by an embodiment of the application;
图5为本申请实施例提供的非均匀形状分布的介质薄膜的示意图;5 is a schematic diagram of a dielectric film with a non-uniform shape distribution provided by an embodiment of the application;
图6为本申请实施例提供的电极结构的示意图;FIG. 6 is a schematic diagram of an electrode structure provided by an embodiment of the application;
图7为本申请实施例提供的AR腔面及HR腔面的示意图;FIG. 7 is a schematic diagram of an AR cavity surface and an HR cavity surface provided by an embodiment of the application;
图8为本申请实施例提供的形成非均匀形状分布的介质薄膜的一个示例流程图;FIG. 8 is an example flow chart of forming a dielectric film with a non-uniform shape distribution according to an embodiment of the application;
图9为本申请实施例提供的均匀注入电极时载流子的为非线性分布曲线图的示意图;FIG. 9 is a schematic diagram of a non-linear distribution curve diagram of carriers when the electrodes are uniformly injected according to an embodiment of the application; FIG.
图10为本申请实施例提供的非均匀形状分布的介质薄膜的剖视图;10 is a cross-sectional view of a dielectric film with a non-uniform shape distribution provided by an embodiment of the application;
图11为本申请实施例提供的将脊面进行等长度划分及非等长度划分载流子浓度的纵向分布的对比图;FIG. 11 is a comparison diagram of the longitudinal distribution of the carrier concentration of the ridges divided by equal length and unequal length according to the embodiment of the application;
图12为本申请实施例提供的半导体激光器的结构示意图。FIG. 12 is a schematic structural diagram of a semiconductor laser provided by an embodiment of the application.
具体实施方式detailed description
下面将结合附图对本申请的技术方案进行清楚、完整地描述,显然,所描述的实施例是本申请一部分实施例,而不是全部的实施例。基于本申请中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得 的所有其他实施例,都属于本申请保护的范围。The technical solution of the present application will be clearly and completely described below in conjunction with the accompanying drawings. Obviously, the described embodiments are part of the embodiments of the present application, rather than all of the embodiments. Based on the embodiments in this application, all other embodiments obtained by those of ordinary skill in the art without creative work shall fall within the protection scope of this application.
在本申请的描述中,需要说明的是,除非另有明确的规定和限定,术语“安装”、“相连”、“连接”应做广义理解,例如,可以是固定连接,也可以是可拆卸连接,或一体地连接;可以是机械连接,也可以是电连接;可以是直接相连,也可以通过中间媒介间接相连,还可以是两个元件内部的连通,可以是无线连接,也可以是有线连接。对于本领域的普通技术人员而言,可以具体情况理解上述术语在本申请中的具体含义。In the description of this application, it should be noted that the terms "installation", "connection", and "connection" should be understood in a broad sense, unless otherwise clearly specified and limited. For example, it can be a fixed connection or a detachable connection. Connected or integrally connected; it can be a mechanical connection or an electrical connection; it can be directly connected, or indirectly connected through an intermediate medium, or it can be the internal connection of the two components, it can be a wireless connection, or it can be a wired connection connection. For those of ordinary skill in the art, the specific meanings of the above-mentioned terms in this application can be understood under specific circumstances.
此外,下面所描述的本申请不同实施方式中所涉及的技术特征只要彼此之间未构成冲突就可以相互结合。In addition, the technical features involved in the different embodiments of the present application described below can be combined with each other as long as they do not conflict with each other.
实施例1Example 1
本申请实施例提供一种半导体激光器的载流子注入方法,如图1所示,包括:An embodiment of the present application provides a carrier injection method for a semiconductor laser, as shown in FIG. 1, including:
步骤S1:在衬底上制备半导体激光器外延结构,获取外延结构晶圆片。Step S1: Prepare a semiconductor laser epitaxial structure on a substrate to obtain an epitaxial structure wafer.
在本申请实施例中,可以使用现有的MOCVD、MBE等设备在衬底上生长半导体激光器外延结构,如图2所示,得到激光器外延结构晶圆片。In the embodiment of the present application, the existing MOCVD, MBE and other equipment can be used to grow the semiconductor laser epitaxial structure on the substrate, as shown in FIG. 2, to obtain the laser epitaxial structure wafer.
步骤S2:在晶圆片上制备半导体激光器的脊形结构。Step S2: preparing the ridge structure of the semiconductor laser on the wafer.
在本申请实施例中,通过光刻刻蚀在晶圆片上制备出脊形结构,如图3所示,脊形结构可以为中间部分高与两边的梯形结构,仅以此举例,不以此为限,在其他实施例中可以为其他形状的脊形结构。In the embodiment of the present application, a ridge structure is prepared on a wafer by photolithography. As shown in FIG. 3, the ridge structure can be a trapezoidal structure with a height in the middle part and two sides. For limitation, in other embodiments, it may be a ridge structure with other shapes.
步骤S3:在脊形结构上制备介质薄膜。Step S3: preparing a dielectric film on the ridge structure.
在本申请实施例中,介质薄膜的材料可以为SiO 2或SiN,如图4所示,制备的介质薄膜覆盖整个脊形结构表面。 In the embodiment of the present application, the material of the dielectric film may be SiO 2 or SiN. As shown in FIG. 4, the prepared dielectric film covers the entire surface of the ridge structure.
步骤S4:将位于脊形结构脊面上的介质薄膜进行刻蚀处理,形成沿纵向方向的非均匀形状分布的介质薄膜。Step S4: etching the dielectric film on the ridge surface of the ridge structure to form a dielectric film with a non-uniform shape distribution along the longitudinal direction.
在本申请实施例中,脊形结构脊面上对介质薄膜进行光刻刻蚀,使得位于脊面上介质薄膜非均匀形状分布,使得其在载流子注入时可以均分分布,在脊面上形成的非均匀形状分布的介质薄膜如图5所示。In the embodiment of the present application, the dielectric film is etched on the ridge surface of the ridge structure by photolithography, so that the dielectric film on the ridge surface has a non-uniform shape distribution, so that it can be evenly distributed during carrier injection. The non-uniform shape distribution of the dielectric film formed on it is shown in Figure 5.
步骤S5:在介质薄膜上制备电极。Step S5: preparing electrodes on the dielectric film.
本申请实施例中,如图6所示,通过沉积的方式在介质薄膜上生成金属电极形成的电极结构。In the embodiment of the present application, as shown in FIG. 6, an electrode structure formed by a metal electrode is formed on a dielectric thin film by deposition.
步骤S6:将晶圆片进行解理,并在解理面的前后两端分别制备减反薄膜及高反薄膜。Step S6: The wafer is cleaved, and anti-reflection films and high-reflection films are prepared on the front and back ends of the cleaved surface respectively.
本申请实施例中,如图7所示,将晶圆片进行解理后,可以通过蒸镀的方式在解理面的前后两端形成减反(AR)薄膜及高反(HR)薄膜,形成AR腔面及HR腔面。In the embodiment of the present application, as shown in FIG. 7, after the wafer is cleaved, an anti-reflection (AR) film and a high-reflection (HR) film can be formed on the front and rear ends of the cleavage surface by evaporation. Form AR cavity surface and HR cavity surface.
步骤S7:从减反薄膜腔面到高反薄膜腔面进行半导体激光器的载流子注入。Step S7: Perform carrier injection of the semiconductor laser from the surface of the anti-reflective film cavity to the surface of the high-reflective film cavity.
本申请提供的半导体激光器的载流子注入方法,通过对脊面上的介质薄膜部分被刻蚀,脊形上只有未覆盖介质薄膜的晶圆片表面才能同金属电极形成接触,从而沿纵向方向可以得到非均匀的载流子注入,利用图形化电极实现载流子的非均匀注入,从而抵消长腔长、两端腔面反射率差异引起的载流子非均匀分布,提升半导体激光器工作状态下增益沿纵向分布的均匀性,提高半导体激光器的光输出功率。The carrier injection method of a semiconductor laser provided in this application is to etch the dielectric film on the ridge surface. Only the surface of the wafer that is not covered with the dielectric film on the ridge can contact the metal electrode, thus along the longitudinal direction. Non-uniform carrier injection can be obtained, and the patterned electrode is used to achieve non-uniform injection of carriers, thereby offsetting the non-uniform distribution of carriers caused by the long cavity length and the difference in the reflectivity of the cavity surfaces at both ends, and improving the working state of the semiconductor laser The uniformity of the lower gain along the longitudinal distribution improves the optical output power of the semiconductor laser.
在一实施例中,执行步骤S4的具体过程,如图8所示,包括:In an embodiment, the specific process of performing step S4, as shown in FIG. 8, includes:
步骤S41:获取半导体激光器均匀注入电极时载流子的非线性分布曲线。Step S41: Obtain a nonlinear distribution curve of carriers when the semiconductor laser is uniformly injected into the electrode.
实际中,当注入电流大于阈值电流时,激光器开始激射,谐振腔内的光子密度会随着注入电流的增加而逐渐增加,且激光器谐振腔内的光子密度沿纵向(AR腔面到HR腔面)呈现出逐渐减小的趋势,导致减反膜(AR)一侧的载流子浓度较低,而高反膜(HR)一侧的载流子浓度较高,如图9所示的均匀注入电极时载流子的为非线性分布曲线图。In practice, when the injection current is greater than the threshold current, the laser starts lasing. The photon density in the cavity will gradually increase with the increase of the injection current, and the photon density in the laser cavity is along the longitudinal direction (AR cavity surface to HR cavity The surface) shows a gradually decreasing trend, resulting in a lower carrier concentration on the AR side, and a higher carrier concentration on the high-reflective film (HR) side, as shown in Figure 9 When uniformly injected into the electrode, the carrier is a non-linear distribution curve.
步骤S42:根据所述载流子的非线性分布曲线,将脊形结构的脊形结构脊面分沿纵向方向分割成多段区域,每段区域中非均匀形状分布的介质薄膜的面积占比,沿减反薄膜腔面到高反薄膜腔面的方向逐渐增加。Step S42: According to the non-linear distribution curve of carriers, the ridge surface of the ridge structure is divided into multiple sections along the longitudinal direction, and the area of the non-uniformly distributed dielectric film in each section is It gradually increases from the surface of the anti-reflective film cavity to the surface of the high-reflective film cavity.
本申请实施例中,介质薄膜的面积占比为介质薄膜面积/小区域面积,如图10所示,以按从左至右将脊形结构分成三部分区域,中间部分即为脊面。在进行介质薄膜的光刻刻蚀时,脊面上方的介质薄膜并未完全去除,被分割成若干个区域,每段区域中非均匀形状分布的介质薄膜的面积不完全相同,且沿着AR腔面到HR腔面纵向方向线性增加,靠近高反薄膜腔面的区域分割的长度比靠近减反薄膜腔面的区域分割的长度短,要具体根据半导体激光器的腔长、减反薄膜腔面和高反薄膜腔面反射率、工作电流及载流子的非线性分布曲线确定每段区域中介质薄膜的长度。如图11所示,通过采用优化的非等长度划分的方式,本申请可以有效提升载流子浓度和增益沿纵向分布的均匀性,通过将半导体激光器的光输出功率提升10%。In the embodiment of the present application, the area ratio of the dielectric film is the area of the dielectric film/the area of the small area. As shown in FIG. 10, the ridge structure is divided into three parts from left to right, and the middle part is the ridge surface. During the photolithography of the dielectric film, the dielectric film above the ridge surface is not completely removed and is divided into several regions. The area of the dielectric film distributed in non-uniform shapes in each region is not exactly the same, and along the AR The longitudinal direction from the cavity surface to the HR cavity surface increases linearly. The length of the region division close to the high-reflection film cavity surface is shorter than the length of the region division close to the anti-reflection film cavity surface. It depends on the cavity length of the semiconductor laser and the anti-reflection film cavity surface. And the non-linear distribution curve of high reflection film cavity surface reflectance, working current and carrier determine the length of the dielectric film in each region. As shown in FIG. 11, by adopting an optimized non-equal length division method, the present application can effectively improve the uniformity of the carrier concentration and gain along the longitudinal distribution, by increasing the optical output power of the semiconductor laser by 10%.
实施例2Example 2
本申请实施例提供一种半导体激光器,如图12所示,包括:衬底;半导体激光器外延结构,形成于所述衬底上;脊形结构,形成所述外延结构上; 介质薄膜,形成于所述脊形结构上;纵向非均匀形状分布的介质薄膜,形成于脊形结构的脊面上方;电极,形成于所述介质薄膜上;减反膜和高反膜,形成于外延结构解理面的前后端面。An embodiment of the present application provides a semiconductor laser, as shown in FIG. 12, comprising: a substrate; a semiconductor laser epitaxial structure formed on the substrate; a ridge structure formed on the epitaxial structure; a dielectric film formed on the substrate On the ridge structure; a dielectric film with a longitudinal non-uniform shape distribution is formed above the ridge surface of the ridge structure; an electrode is formed on the dielectric film; an anti-reflection film and a high-reflection film are formed on the cleavage of the epitaxial structure The front and rear faces of the face.
在本申请实施例中,纵向非均匀形状分布的介质薄膜的面积占比,沿减反薄膜腔面到高反薄膜腔面的方向逐渐增加,所述纵向非均匀形状分布的介质薄膜的面积不完全相同,非均匀形状分布的介质薄膜的排布如图10所示,以按从左至右将脊形结构分成三部分区域,中间部分即为脊面,靠近HR腔面的区域,分割成长度较短的区域;靠近AR腔面的区域,分割成长度较长的区域,具体的长度应根据激光器腔长、两端腔面反射率、工作电流、载流子分布曲线而决定。图10中未被刻蚀的介质薄膜为长方形,仅以举例,不以此为限,在其他实施例中可以为椭圆形、圆形或其他多边形。In the embodiment of the present application, the area ratio of the dielectric film distributed in the longitudinal non-uniform shape gradually increases along the direction from the cavity surface of the anti-reflective film to the cavity surface of the high-reflection film, and the area of the dielectric film distributed in the longitudinal non-uniform shape is different. The arrangement of the dielectric film with exactly the same, non-uniform shape distribution is shown in Figure 10. The ridge structure is divided into three parts from left to right. The middle part is the ridge surface, and the area close to the HR cavity surface is divided into long sections. The region near the AR cavity surface is divided into longer length regions. The specific length should be determined according to the laser cavity length, the reflectivity of the cavity surfaces at both ends, the operating current, and the carrier distribution curve. The dielectric film that is not etched in FIG. 10 is rectangular, which is only an example, and is not limited to this. In other embodiments, it may be elliptical, circular, or other polygonal shapes.
本申请实施例提供的半导体激光器,通过在脊面上方设置非均匀分布的介质薄膜的形状,控制实际电流注入的区域,实现电流沿脊形纵向的非均匀注入,从而抵消长腔长、两端腔面反射率差异引起的载流子非均匀分布,提升半导体激光器工作状态下增益沿纵向分布的均匀性,提高半导体激光器的光输出功率。In the semiconductor laser provided by the embodiment of the present application, the shape of the non-uniformly distributed dielectric film is arranged above the ridge surface to control the actual current injection area, so as to realize the non-uniform injection of current along the longitudinal direction of the ridge, thereby offsetting the long cavity length and both ends. The non-uniform distribution of carriers caused by the difference in the reflectivity of the cavity surface improves the uniformity of the longitudinal distribution of the gain in the working state of the semiconductor laser, and improves the optical output power of the semiconductor laser.
显然,上述实施例仅仅是为清楚地说明所作的举例,而并非对实施方式的限定。对于所属领域的普通技术人员来说,在上述说明的基础上还可以做出其它不同形式的变化或变动。这里无需也无法对所有的实施方式予以穷举。而由此所引申出的显而易见的变化或变动仍处于本申请创造的保护范围之中。Obviously, the foregoing embodiments are merely examples for clear description, and are not intended to limit the implementation manner. For those of ordinary skill in the art, other changes or modifications in different forms can be made on the basis of the above description. It is unnecessary and impossible to list all the implementation methods here. The obvious changes or changes derived from this are still within the scope of protection created by this application.

Claims (9)

  1. 一种半导体激光器的载流子注入方法,其特征在于,包括:A carrier injection method for a semiconductor laser is characterized in that it comprises:
    在衬底上制备半导体激光器外延结构,获取外延结构晶圆片;Prepare the semiconductor laser epitaxial structure on the substrate to obtain the epitaxial structure wafer;
    在晶圆片上制备半导体激光器的脊形结构;Preparation of the ridge structure of the semiconductor laser on the wafer;
    在脊形结构上制备介质薄膜;Preparation of dielectric film on the ridge structure;
    将位于脊形结构脊面上的介质薄膜进行刻蚀处理,形成沿纵向方向的非均匀形状分布的介质薄膜;Etching the dielectric film on the ridge surface of the ridge structure to form a dielectric film with a non-uniform shape distribution along the longitudinal direction;
    在介质薄膜上制备电极;Preparation of electrodes on the dielectric film;
    将晶圆片进行解理,并在解理面的前后两端分别制备减反薄膜及高反薄膜;Cleavage the wafer, and prepare anti-reflection film and high-reflection film on the front and back ends of the cleavage surface;
    从减反薄膜腔面到高反薄膜腔面进行半导体激光器的载流子注入。Carrier injection of the semiconductor laser is performed from the surface of the anti-reflective film cavity to the surface of the high-reflective film cavity.
  2. 根据权利要求1所述的半导体激光器的载流子注入方法,其特征在于,所述将位于脊形结构脊面上的介质薄膜进行刻蚀处理,形成沿纵向方向的非均匀形状分布的介质薄膜的步骤,包括:The carrier injection method of a semiconductor laser according to claim 1, wherein the dielectric film on the ridge surface of the ridge structure is etched to form a dielectric film with a non-uniform shape distribution along the longitudinal direction The steps include:
    获取半导体激光器均匀注入电极时载流子的非线性分布曲线;Obtain the nonlinear distribution curve of carriers when the semiconductor laser is uniformly injected into the electrode;
    根据所述载流子的非线性分布曲线,将脊形结构的脊形结构脊面分沿纵向方向分割成多段区域,每段区域中非均匀形状分布的介质薄膜的面积占比,沿减反薄膜腔面到高反薄膜腔面的方向逐渐增加。According to the non-linear distribution curve of the carriers, the ridge structure of the ridge structure is divided into multiple regions along the longitudinal direction. The direction from the film cavity surface to the high reflection film cavity surface gradually increases.
  3. 根据权利要求2所述的半导体激光器的载流子注入方法,其特征在于,每段区域中非均匀形状分布的介质薄膜的面积不完全相同。The carrier injection method of a semiconductor laser according to claim 2, wherein the area of the dielectric thin film distributed in the non-uniform shape in each region is not completely the same.
  4. 根据权利要求3所述的半导体激光器的载流子注入方法,其特征在于,靠近高反薄膜腔面的区域分割的长度比靠近减反薄膜腔面的区域分割的长度短。The carrier injection method of a semiconductor laser according to claim 3, wherein the length of the region division close to the cavity surface of the high-reflective film is shorter than the length of the region division close to the cavity surface of the anti-reflective film.
  5. 根据权利要求3所述的半导体激光器的载流子注入方法,其特征在于,根据半导体激光器的腔长、减反薄膜腔面和高反薄膜腔面反射率、工作电流及载流子的非线性分布曲线确定每段区域中介质薄膜的长度。The carrier injection method of a semiconductor laser according to claim 3, characterized in that according to the cavity length of the semiconductor laser, the reflectivity of the anti-reflection film cavity surface and the high-reflection film cavity surface, the operating current and the nonlinearity of the carrier The distribution curve determines the length of the dielectric film in each area.
  6. 一种半导体激光器,其特征在于,包括:A semiconductor laser, characterized in that it comprises:
    衬底;Substrate
    半导体激光器外延结构,形成于所述衬底上;A semiconductor laser epitaxial structure formed on the substrate;
    脊形结构,形成所述外延结构上;A ridge structure formed on the epitaxial structure;
    介质薄膜,形成于所述脊形结构上;A dielectric film formed on the ridge structure;
    纵向非均匀形状分布的介质薄膜,形成于脊形结构的脊面上方;A dielectric film with longitudinal non-uniform shape distribution is formed above the ridge surface of the ridge structure;
    电极,形成于所述介质薄膜上;An electrode formed on the dielectric film;
    减反膜和高反膜,形成于外延结构解理面的前后端面。Anti-reflection film and high-reflection film are formed on the front and back ends of the cleavage surface of the epitaxial structure.
  7. 根据权利要求6所述的半导体激光器,其特征在于,所述纵向非均匀形状分布的介质薄膜的面积占比,沿减反薄膜腔面到高反薄膜腔面的方向逐渐增加。7. The semiconductor laser according to claim 6, wherein the area ratio of the dielectric film distributed in the longitudinal non-uniform shape gradually increases from the surface of the anti-reflection film cavity to the surface of the high-reflection film cavity.
  8. 根据权利要求6所述的半导体激光器,其特征在于,所述纵向非均匀形状分布的介质薄膜的面积不完全相同。7. The semiconductor laser according to claim 6, wherein the areas of the dielectric films distributed in the longitudinal non-uniform shape are not completely the same.
  9. 根据权利要求8所述的半导体激光器,其特征在于,所述纵向非均匀形状分布的介质薄膜的形状为多边形、圆形或椭圆形。8. The semiconductor laser according to claim 8, wherein the shape of the dielectric film with longitudinal non-uniform shape distribution is polygonal, circular or elliptical.
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