WO2021056617A1 - Semiconductor laser and carrier injection method therefor - Google Patents
Semiconductor laser and carrier injection method therefor Download PDFInfo
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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
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/06—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
- H01S5/0604—Arrangements 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
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/20—Structure 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
- H01S5/22—Structure 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
Definitions
- 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
Description
Claims (9)
- 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.
- 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.
- 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.
- 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.
- 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.
- 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.
- 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.
- 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.
- 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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CN114583556B (en) * | 2022-05-05 | 2022-07-15 | 苏州长光华芯光电技术股份有限公司 | Longitudinal carrier modulation high-power semiconductor light-emitting chip and preparation method thereof |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1574526A (en) * | 2003-05-22 | 2005-02-02 | 松下电器产业株式会社 | Semiconductor laser |
JP2005302843A (en) * | 2004-04-07 | 2005-10-27 | Matsushita Electric Ind Co Ltd | Semiconductor laser |
CN101938085A (en) * | 2009-06-29 | 2011-01-05 | 夏普株式会社 | Nitride semi-conductor laser and wafer |
CN107946901A (en) * | 2017-12-25 | 2018-04-20 | 苏州长光华芯光电技术有限公司 | A kind of semiconductor laser patterned electrodes method for implanting |
CN109923743A (en) * | 2016-11-01 | 2019-06-21 | 索尼半导体解决方案公司 | The method of semiconductor devices, semiconductor laser and manufacturing semiconductor devices |
Family Cites Families (3)
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CN1960091A (en) * | 2005-11-01 | 2007-05-09 | 中国科学院半导体研究所 | Tube core cell structure of gallium - arsenic based quanta cascaded laser, and fabricating method |
JP5005300B2 (en) * | 2006-09-07 | 2012-08-22 | パナソニック株式会社 | Semiconductor laser device |
JPWO2012101686A1 (en) * | 2011-01-26 | 2014-06-30 | パナソニック株式会社 | Semiconductor light emitting element and light emitting device |
-
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Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1574526A (en) * | 2003-05-22 | 2005-02-02 | 松下电器产业株式会社 | Semiconductor laser |
JP2005302843A (en) * | 2004-04-07 | 2005-10-27 | Matsushita Electric Ind Co Ltd | Semiconductor laser |
CN101938085A (en) * | 2009-06-29 | 2011-01-05 | 夏普株式会社 | Nitride semi-conductor laser and wafer |
CN109923743A (en) * | 2016-11-01 | 2019-06-21 | 索尼半导体解决方案公司 | The method of semiconductor devices, semiconductor laser and manufacturing semiconductor devices |
CN107946901A (en) * | 2017-12-25 | 2018-04-20 | 苏州长光华芯光电技术有限公司 | A kind of semiconductor laser patterned electrodes method for implanting |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20210384702A1 (en) * | 2020-06-09 | 2021-12-09 | Xiamen Sanan Optoelectronics Technology Co., Ltd | Laser diode and method for manufacturing the same |
US11870219B2 (en) * | 2020-06-09 | 2024-01-09 | Quanzhou San'an Semiconductor Technology Co., Ltd. | Laser diode and method for manufacturing the same |
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