[go: up one dir, main page]

CN107565381B - Distributed feedback semiconductor laser device and photonic integrated emission chip module - Google Patents

Distributed feedback semiconductor laser device and photonic integrated emission chip module Download PDF

Info

Publication number
CN107565381B
CN107565381B CN201710827089.2A CN201710827089A CN107565381B CN 107565381 B CN107565381 B CN 107565381B CN 201710827089 A CN201710827089 A CN 201710827089A CN 107565381 B CN107565381 B CN 107565381B
Authority
CN
China
Prior art keywords
grating
chirped
electrodes
distributed feedback
semiconductor laser
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201710827089.2A
Other languages
Chinese (zh)
Other versions
CN107565381A (en
Inventor
周亚亭
茆锐
沈玉乔
肖虹
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Changzhou Institute of Technology
Original Assignee
Changzhou Institute of Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Changzhou Institute of Technology filed Critical Changzhou Institute of Technology
Priority to CN201710827089.2A priority Critical patent/CN107565381B/en
Publication of CN107565381A publication Critical patent/CN107565381A/en
Application granted granted Critical
Publication of CN107565381B publication Critical patent/CN107565381B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Semiconductor Lasers (AREA)

Abstract

the invention discloses a distributed feedback type semiconductor laser device and a photon integrated emission chip module. The grating of the device is formed by connecting two chirped gratings in series through a gain area without grating, or formed by connecting sampling gratings with chirped sampling periods in series through a gain area without grating; wherein, the electrode of the first chirp grating is composed of three electrodes which are mutually electrically isolated, the corresponding part of the middle electrode of the grating is a phase shift adjusting area, and the corresponding parts of the electrodes at two sides of the grating are side areas; the corresponding portion of the second chirped grating is either a passive region without gain or an active region controlled by one or more electrodes. The invention can continuously adjust the lasing wavelength of the laser to meet the requirements of ITU-T standard by changing the injection current or the proportion of the injection current of the side area and the phase shift adjusting area; when the second chirped grating structure is identical to the first grating structure, the laser has better single-mode characteristics and narrower line width.

Description

分布反馈式半导体激光器装置及光子集成发射芯片模块Distributed feedback semiconductor laser device and photonic integrated emission chip module

技术领域technical field

本发明属于光电子技术领域,涉及光纤通信、光子集成、光电传感以及其他光电信息处理。本发明是一种波长可在一定范围内精细可调的分布反馈式半导体激光器装置及其制造方法。The invention belongs to the technical field of optoelectronics, and relates to optical fiber communication, photon integration, photoelectric sensing and other photoelectric information processing. The invention relates to a distributed feedback type semiconductor laser device whose wavelength can be finely adjusted within a certain range and a manufacturing method thereof.

背景技术Background technique

作为光纤通信系统的核心器件,分布反馈式(Distributed Feedback,DFB)半导体激光器由于体积小、结构简单而受到世人关注。普通的均匀光栅半导体激光器,其折射率是被周期性地均匀调制的。这种激光器在布拉格波长两侧,对称地存在两个谐振腔损耗相同并且最低的模式,称之为两种模式简并。为获得良好的单模特性,可以在均匀光栅的中心引入一个四分之一波长(λ/4)的真实相移,以消除模式简并,使激光器在其布拉格波长发生激射。As the core device of optical fiber communication system, distributed feedback (Distributed Feedback, DFB) semiconductor laser has attracted worldwide attention due to its small size and simple structure. The refractive index of ordinary uniform grating semiconductor laser is modulated periodically and uniformly. On both sides of the Bragg wavelength of this laser, there are two modes with the same resonator loss and the lowest symmetrically, which is called the degeneracy of the two modes. To obtain good single-mode behavior, a quarter-wavelength (λ/4) true phase shift can be introduced at the center of the uniform grating to eliminate mode degeneracy and allow the laser to lase at its Bragg wavelength.

要加工这种真实相移DFB半导体激光器,其光栅的刻制需要纳米精度的控制,目前只有经过特殊处理的高精度电子刻写设备能够达到这样的加工精度。这种高精度电子刻写设备价格昂贵,需要耗费大量的时间才能加工生产这种真实相移均匀光栅,因而真实相移DFB半导体激光器的制作成本高昂,目前还不具备大规模产业化应用的能力。To process this real phase-shifted DFB semiconductor laser, the engraving of the grating needs to be controlled with nanometer precision. At present, only high-precision electronic writing equipment that has undergone special treatment can achieve such processing accuracy. This kind of high-precision electronic writing equipment is expensive, and it takes a lot of time to process and produce this kind of real phase-shifted uniform grating. Therefore, the production cost of real phase-shifted DFB semiconductor lasers is high, and it is not yet capable of large-scale industrial application.

为克服这种缺点,南京大学陈向飞教授提出了用带有等效相移的均匀取样光栅来代替真实相移均匀光栅的方法,来制作光纤通信系统所用的分布反馈式半导体激光器。这种做法的好处是能获得与真实相移光栅半导体激光器相同激射性能的等效相移取样光栅半导体激光器,但后者要求的加工精度比前者要低一到两个数量级,因而能大大降低加工的难度和成本。In order to overcome this shortcoming, Professor Chen Xiangfei of Nanjing University proposed the method of replacing the real phase-shifted uniform grating with a uniformly sampled grating with equivalent phase shift to make distributed feedback semiconductor lasers used in optical fiber communication systems. The advantage of this method is that the equivalent phase-shifted sampling grating semiconductor laser with the same lasing performance as the real phase-shifted grating semiconductor laser can be obtained, but the processing accuracy required by the latter is one to two orders of magnitude lower than the former, so it can be greatly reduced. Difficulty and cost of processing.

但无论是等效相移取样光栅半导体激光器还是真实相移光栅半导体激光器,由于在制作过程中总是存在着各种偶然因素,会使得激光器的激射波长偏离设计的ITU-T标准。因而实际的分布反馈式半导体激光器,需要特殊的调谐装置,如电加热装置或改变注入电流等,来调节激光器的激射波长对准ITU-T标准。这些特殊的调谐装置会使得激光器的结构变得复杂,性能下降。However, whether it is an equivalent phase-shift sampling grating semiconductor laser or a real phase-shift grating semiconductor laser, due to various accidental factors in the production process, the lasing wavelength of the laser will deviate from the designed ITU-T standard. Therefore, the actual distributed feedback semiconductor laser requires a special tuning device, such as an electric heating device or changing the injection current, to adjust the lasing wavelength of the laser to the ITU-T standard. These special tuning devices will complicate the structure of the laser and degrade its performance.

另一方面,由于对光通信网络传输容量的需求急剧增长,波分复用(Wavelengthdivision multiplexing,WDM)系统复用的信道数越来越多,这种通信系统需要用不同激射波长的激光器作光源。为减少由此带来的能耗和维护成本急剧上升问题,光子集成(Photonic integration circuit,PIC)是必然的选择。如果仍然采用电加热装置或改变注入电流的方式来来调节各单元激光器的激射波长对准ITU-T标准,那么除会导致各单元激光器输出激光功率严重不均衡外,还会造成激光器阵列结构异常复杂的问题。On the other hand, due to the sharp increase in the demand for the transmission capacity of the optical communication network, the number of channels multiplexed by the Wavelength Division Multiplexing (WDM) system is increasing. This communication system needs to use lasers with different lasing wavelengths as light source. In order to reduce the resulting sharp rise in energy consumption and maintenance costs, photonic integration circuit (PIC) is an inevitable choice. If the electric heating device or the way of changing the injection current is still used to adjust the lasing wavelength of each unit laser to align with the ITU-T standard, then in addition to causing a serious imbalance in the output laser power of each unit laser, it will also cause the laser array structure Extraordinarily complex issue.

实际上,利用等效相移取样光栅技术制成的多波长半导体激光器阵列,其各单元激光器的激射波长的单模成品率可以通过引入等效相移来保证,而其激射波长的整体漂移可以通过为激光器阵列芯片整体外加电辅热装置来完成。但研究发现在这样的激光器阵列芯片中,各单元激光器的激射波长对ITU-T标准的上下波动,一般情况下仍然经常会达到零点几个纳米范围,远超过密集波分复用通信系统中ITU-T规定的要求。这会导致多波长半导体激光器阵列芯片成品率严重下降的问题。In fact, for the multi-wavelength semiconductor laser array made by the equivalent phase-shift sampling grating technology, the single-mode yield of the lasing wavelength of each unit laser can be guaranteed by introducing an equivalent phase shift, while the overall lasing wavelength The drift can be accomplished by adding an electric auxiliary heating device to the laser array chip as a whole. However, the study found that in such a laser array chip, the lasing wavelength of each unit laser fluctuates up and down with the ITU-T standard. Generally, it still often reaches the range of a few tenths of a nanometer, far exceeding that in dense wavelength division multiplexing communication systems. The requirements stipulated by ITU-T. This will lead to a serious drop in the yield of multi-wavelength semiconductor laser array chips.

发明内容Contents of the invention

针对现有技术中半导体激光器存在的上述不足,本发明提出了一种新的分布反馈式半导体激光器结构。Aiming at the above-mentioned shortcomings of semiconductor lasers in the prior art, the present invention proposes a new distributed feedback semiconductor laser structure.

本发明的技术方案是:Technical scheme of the present invention is:

一种分布反馈式半导体激光器装置,所述分布反馈式半导体激光器装置的光栅是由两个啁啾光栅通过无光栅的增益区串联而成,或者由取样周期啁啾的取样光栅(其选作激射信道的±1级子光栅仍是线性啁啾光栅)通过无光栅的增益区串联而成;其中第一个啁啾光栅的电极由三个相互电隔离的电极组成,这个光栅中间电极所对应部分为相移调整区,它的两侧电极对应部分为侧边区;第二个啁啾光栅所对应部分是无增益的无源区,或者是由一个或多个电极控制的有源区;A distributed feedback semiconductor laser device, the grating of the distributed feedback semiconductor laser device is formed by two chirped gratings connected in series through a gain region without a grating, or a sampling grating chirped by a sampling period (which is selected as the excitation The ±1-level sub-grating of the radiation channel is still a linear chirped grating) connected in series through the gain region without grating; the electrode of the first chirped grating is composed of three mutually electrically isolated electrodes, and the middle electrode of the grating corresponds to Part of it is a phase shift adjustment area, and the corresponding part of the electrodes on both sides is a side area; the corresponding part of the second chirped grating is a passive area without gain, or an active area controlled by one or more electrodes;

作为本发明的进一步改进,第一个啁啾光栅的两个侧边区长度相同;As a further improvement of the present invention, the two side regions of the first chirped grating have the same length;

作为本发明的进一步改进,第一个啁啾光栅的两个侧边区电极可以用导线连接在一起,形成同一个侧边区电极;As a further improvement of the present invention, the two side region electrodes of the first chirped grating can be connected together with wires to form the same side region electrode;

作为本发明的进一步改进,第二个啁啾光栅与第一个啁啾光栅可以是完全相同的啁啾光栅;As a further improvement of the present invention, the second chirped grating can be exactly the same chirped grating as the first chirped grating;

作为本发明的另一种改进,第二个啁啾光栅所对应部分可以是由三个相互电隔离的电极控制的有源区,即两个侧边区和中间相移调整区组成;As another improvement of the present invention, the corresponding part of the second chirped grating can be composed of three active regions controlled by mutually electrically isolated electrodes, that is, two side regions and an intermediate phase shift adjustment region;

作为本发明的进一步改进,第二个啁啾光栅所对应的两个侧边区和中间相移调整区,与第一个啁啾光栅完全相同;As a further improvement of the present invention, the two side regions and the middle phase shift adjustment region corresponding to the second chirped grating are exactly the same as the first chirped grating;

作为本发明的进一步改进,第二个啁啾光栅所对应的两个侧边区可以用导线连接在一起,形成同一个侧边区电极;As a further improvement of the present invention, the two side regions corresponding to the second chirped grating can be connected together with a wire to form the same side region electrode;

作为本发明的进一步改进,本发明激光器的四个侧边区电极和两个中间相移调整区的电极,可以分别用导线连接在一起形成总的侧边区电极和总的相移调整区电极;As a further improvement of the present invention, the electrodes of the four side region electrodes and the two intermediate phase shift adjustment regions of the laser of the present invention can be connected together with wires to form the total side region electrodes and the total phase shift adjustment region electrodes ;

本发明还提供一种分布反馈式半导体激光器单片集成阵列,所述分布反馈式半导体激光器单片集成阵列由上述分布反馈式半导体激光器装置构成。The present invention also provides a distributed feedback semiconductor laser monolithic integrated array, the distributed feedback semiconductor laser monolithic integrated array is composed of the above-mentioned distributed feedback semiconductor laser device.

本发明还提供一种光子集成发射芯片模块,由激光监测器阵列、上述半导体激光器单片集成阵列、调制器阵列、功率均衡器阵列和复用器,通过选择区外延生长或对接生长技术,依次生长集成到同一外延晶片上。The present invention also provides a photonic integrated emission chip module, which consists of a laser monitor array, the above-mentioned semiconductor laser monolithic integrated array, a modulator array, a power equalizer array and a multiplexer, through selective area epitaxial growth or docking growth technology, sequentially The growth is integrated on the same epitaxial wafer.

本发明的有益效果是:The beneficial effects of the present invention are:

本发明的激光器正常工作时,通过改变第一个啁啾光栅的侧边区和中间相移调整区注入电流,就可以连续调节激光器第一个啁啾光栅在不同的光栅周期处发生激射,从而可连续精细调节激光器的激射波长。如果激光器总的注入电流保持不变,只要通过改变侧边区、相移调整区注入电流的比例,就能够精细调控激光器的激射波长,且激光器保持相似的域值和激射输出功率。When the laser of the present invention is working normally, the first chirped grating of the laser can be continuously adjusted to lasing at different grating periods by changing the injection current in the side region and the intermediate phase shift adjustment region of the first chirped grating. Therefore, the lasing wavelength of the laser can be finely adjusted continuously. If the total injection current of the laser remains unchanged, the lasing wavelength of the laser can be finely regulated by changing the ratio of the injection current in the side region and the phase shift adjustment region, and the laser maintains a similar threshold value and lasing output power.

如果第二个啁啾光栅所对应的部分为无源反馈区或单电极控制的有源反馈区,那么第二个啁啾光栅作为宽谱的反射器,可以把这个激光器产生的激光,从第一个啁啾光栅的外端面反射出去,这就大大提高了激光器有效输出激光的效率。与此同时,如果激光器的两个啁啾光栅都是取样周期线性啁啾的取样光栅,与线性啁啾光栅相比,在获得相同的反射(或透射)性能的同时,大大降低了对光栅的加工精度要求,因而其制造成本能显著降低。If the part corresponding to the second chirped grating is a passive feedback area or an active feedback area controlled by a single electrode, then the second chirped grating acts as a wide-spectrum reflector, which can convert the laser generated by this laser from the first The outer end face of a chirped grating is reflected, which greatly improves the laser output efficiency of the laser. At the same time, if the two chirped gratings of the laser are sampling gratings whose sampling period is linearly chirped, compared with linearly chirped gratings, while obtaining the same reflective (or transmissive) performance, the impact on the gratings is greatly reduced. Machining accuracy is required, so its manufacturing cost can be significantly reduced.

如果第二个啁啾光栅与第一个啁啾光栅是完全相同的三电极光栅结构,在两个光栅的三个电极都通以相同的电流情况下,由于两个啁啾光栅对激光的选频和反馈作用完全相同,因此这样的光栅对产生激光的选频作用得到了进一步的强化,因而其输出的激光具有更好的单模特性,输出激光的线宽更窄。If the second chirped grating is the same three-electrode grating structure as the first chirped grating, when the three electrodes of the two gratings are all connected with the same current, due to the selection of the laser by the two chirped gratings The frequency and feedback functions are exactly the same, so the frequency selection effect of such a grating on the generated laser has been further strengthened, so the output laser has better single-mode characteristics, and the output laser has a narrower linewidth.

附图说明Description of drawings

图1是第二个啁啾光栅为无源光栅时本发明激光器的光栅结构示意图;Fig. 1 is the grating structure schematic diagram of the laser of the present invention when the second chirped grating is a passive grating;

图2是第二个啁啾光栅为单电极控制的有源光栅时本发明激光器的光栅结构示意图;Fig. 2 is the grating structure diagram of the laser of the present invention when the second chirped grating is an active grating controlled by a single electrode;

图3是第二个啁啾光栅为三电极控制的有源光栅时本发明激光器的光栅结构示意图;Fig. 3 is the grating structure diagram of the laser of the present invention when the second chirped grating is an active grating controlled by three electrodes;

图4是本发明分布反馈式半导体激光器第一个啁啾光栅的有源区结构示意图;Fig. 4 is a schematic diagram of the active region structure of the first chirped grating of the distributed feedback semiconductor laser of the present invention;

图中:1、P电极;2、欧姆接触层;3、P-InP层;4、光栅层;5、上限制层;6、有源层;7、下限制层;8、n-InP缓冲层;9、n-InP基底;10、n电极。In the figure: 1. P electrode; 2. Ohmic contact layer; 3. P-InP layer; 4. Grating layer; 5. Upper confinement layer; 6. Active layer; 7. Lower confinement layer; 8. n-InP buffer layer; 9, n-InP substrate; 10, n electrode.

图5是多波长光子集成发射芯片功能结构示意图。Fig. 5 is a schematic diagram of the functional structure of a multi-wavelength photonic integrated emission chip.

具体实施方式Detailed ways

下面结合附图对本发明作进一步详细说明。The present invention will be described in further detail below in conjunction with the accompanying drawings.

实施例一Embodiment one

本实施例提供一种分布反馈式半导体激光器装置,由两个啁啾光栅通过无光栅的增益区串联而成,或者是由两个取样周期啁啾的取样光栅通过无光栅的增益区串联而成;其中第一个啁啾光栅的电极由三个相互电隔离的电极组成,这个光栅中间电极所对应部分为相移调整区,它的两侧电极对应部分为侧边区;第二个啁啾光栅所对应部分是无增益的无源区(如图1所示),或者是由一个(如图2所示)或多个(如图3所示)电极控制的有源区。本发明分布反馈式半导体激光器第一个啁啾光栅的有源区的结构如图4所示。This embodiment provides a distributed feedback semiconductor laser device, which is formed by connecting two chirped gratings in series through a gain region without a grating, or by connecting two sampling gratings with a sampling period chirped in series through a gain region without a grating ; The electrode of the first chirped grating is composed of three electrodes electrically isolated from each other, the corresponding part of the middle electrode of the grating is the phase shift adjustment area, and the corresponding part of the electrodes on both sides of the grating is the side area; the second chirped grating The corresponding portion of the grating is a passive region with no gain (as shown in Figure 1), or an active region controlled by one (as shown in Figure 2) or multiple electrodes (as shown in Figure 3). The structure of the active region of the first chirped grating of the distributed feedback semiconductor laser of the present invention is shown in FIG. 4 .

本实施例中:第一个啁啾光栅的两个侧边区电极可以通过导线连接在一起,形成同一个侧边区电极;第一个啁啾光栅的两个侧边区可以长度相同。In this embodiment: the two side region electrodes of the first chirped grating can be connected together by wires to form the same side region electrode; the two side region electrodes of the first chirped grating can have the same length.

本实施例中,第二个啁啾光栅与第一个啁啾光栅可以是完全相同的啁啾光栅,其对应的电极和结构也相同,均由完全相同的两个侧边区和一个相移调整区组成;第二个啁啾光栅的两个侧边区电极,可以用导线连接在一起,形成同一个侧边区电极。In this embodiment, the second chirped grating and the first chirped grating can be exactly the same chirped grating, and the corresponding electrodes and structures are also the same, and both have the same two side regions and a phase shift The composition of the adjustment area; the two side area electrodes of the second chirped grating can be connected together by wires to form the same side area electrode.

本实施例中:两个啁啾光栅的四个侧边区电极,可以用导线连接在一起形成同一个侧边区电极,两个啁啾光栅的两个相移调整区电极,可以用导线连接在一起形成同一个相移调整区电极。In this embodiment: the four side region electrodes of the two chirped gratings can be connected together by wires to form the same side region electrodes, and the two phase shift adjustment region electrodes of the two chirped gratings can be connected by wires together to form the same phase shift adjustment region electrodes.

本实施例中,相邻的相移调整区、侧边区、增益区和第二个啁啾光栅的各电极间可以通过相距一定距离、或者通过注入氦离子、或者通过刻蚀电隔离沟等方式相电隔离。In this embodiment, the electrodes of the adjacent phase shift adjustment regions, side regions, gain regions, and the second chirped grating can be separated by a certain distance, or by implanting helium ions, or by etching electrical isolation grooves, etc. way of galvanic isolation.

本发明分布反馈式半导体激光器装置激射波长精细调节的实现原理如下:The realization principle of the fine adjustment of the lasing wavelength of the distributed feedback semiconductor laser device of the present invention is as follows:

这里以图2中第一个啁啾光栅对应长度相同的两个侧边区和中间相移调整区,第二个啁啾光栅对应位置为单电极控制的有源区,且相邻的中间相移调整区、侧边区、增益区电极都相互电隔离的情形,来说明本发明分布反馈式半导体激光器装置精细调节激射波长的原理。Here, the first chirped grating in Figure 2 corresponds to the two side regions and the middle phase shift adjustment region with the same length, and the corresponding position of the second chirped grating is the active region controlled by a single electrode, and the adjacent middle phase The principle of finely adjusting the lasing wavelength of the distributed feedback semiconductor laser device of the present invention will be described by using the case where the electrodes of the shift adjustment region, the side region and the gain region are electrically isolated from each other.

由于每一个线性啁啾光栅都可以看作光栅周期连续变化的均匀光栅叠加而成,当本发明激光器中注入电流高于阈值时,如果第一个啁啾光栅的侧边区和中间相移调整区电极注入不同大小电流,就能在不同周期的均匀光栅中引入不同的相移,这就使得在某一特定光栅周期位置其激射波长具有最低的阈值,因而这个激光器就能产生这个波长的激光。当改变激光器啁啾光栅的侧边区和中间相移调整区电极注入电流比例(大小)时,就能引发线性啁啾光栅在不同的光栅周期位置产生激射,进而精细调节激光器的激射波长。Since each linear chirped grating can be regarded as a superposition of uniform gratings with continuously changing grating periods, when the injection current in the laser of the present invention is higher than the threshold value, if the side region and the middle phase shift of the first chirped grating are adjusted By injecting currents of different magnitudes into the region electrodes, different phase shifts can be introduced into the uniform gratings of different periods, which makes the lasing wavelength have the lowest threshold value at a certain period position of the grating, so this laser can produce lasers of this wavelength. laser. When changing the electrode injection current ratio (size) of the side region of the laser chirped grating and the middle phase shift adjustment region, the linear chirped grating can be induced to generate lasing at different grating period positions, and then the lasing wavelength of the laser can be finely adjusted .

实施例二Embodiment two

本实施例提供一种分布反馈式半导体激光器单片集成阵列,该集成阵列由实施例一中所述的分布反馈式半导体激光器装置构成。This embodiment provides a monolithic integrated array of distributed feedback semiconductor lasers, which is composed of the distributed feedback semiconductor laser device described in Embodiment 1.

本实施例还提供一种光子集成发射芯片模块(如图5所示),该模块由激光监测器阵列、上述分布反馈式半导体激光器单片集成阵列、调制器阵列、功率均衡器阵列和复用器,通过选择区外延生长或对接生长技术,依次生长集成到同一外延晶片上构成。The present embodiment also provides a photonic integrated emission chip module (as shown in Figure 5), which consists of a laser monitor array, the above-mentioned distributed feedback semiconductor laser monolithic integrated array, modulator array, power equalizer array and multiplexing Devices are sequentially grown and integrated on the same epitaxial wafer through selective area epitaxial growth or butt growth technology.

实施例三Embodiment three

本实施例通过一种分布反馈式半导体激光器及其阵列的制作方法,其步骤如下:This embodiment adopts a manufacturing method of a distributed feedback semiconductor laser and an array thereof, the steps of which are as follows:

(1)在n型InP衬底材料上依次外延n型InP缓冲层、100nm厚的非掺杂晶格匹配InGaAsP下限制层、应变InGaAsP多量子阱和100nm厚的p型晶格匹配InGaAsP上限制层;(1) Epitaxial n-type InP buffer layer, 100nm thick undoped lattice-matched InGaAsP lower confinement layer, strained InGaAsP multiple quantum wells and 100nm thick p-type lattice-matched InGaAsP upper confinement layer on n-type InP substrate material Floor;

(2)光栅的制作方法:(2) The production method of the grating:

①线性啁啾取样光栅的制作方法,用双光束全息干涉透过取样光刻板进行曝光的方法,把啁啾取样光栅图案转移到上限制层上的光刻胶上,然后施以材料刻蚀,在上限制层上部形成所需的啁啾取样光栅结构。①The manufacturing method of the linear chirped sampling grating, using the method of double-beam holographic interference to expose through the sampling photoresist, transfer the chirped sampling grating pattern to the photoresist on the upper confinement layer, and then perform material etching, A required chirped sampling grating structure is formed on the upper part of the upper confinement layer.

②线性啁啾光栅的制作方法,用高精度电子束刻写的方法,把线性啁啾光栅刻录到上限制层上的光刻胶上,然后施以材料刻蚀,在上限制层上部形成所需的啁啾光栅结构。②The manufacturing method of the linear chirped grating, using the method of high-precision electron beam writing, the linear chirped grating is recorded on the photoresist on the upper confinement layer, and then the material is etched to form the required chirped grating structure.

(3)当光栅制作好后,再通过二次外延生长p型InP层和p型InGaAs欧姆接触层。在外延生长结束后,利用普通光刻结合化学湿法刻蚀,完成脊形波导的制作;(3) After the grating is fabricated, the p-type InP layer and the p-type InGaAs ohmic contact layer are grown by secondary epitaxy. After the epitaxial growth is completed, the fabrication of the ridge waveguide is completed by using ordinary photolithography combined with chemical wet etching;

(4)用等离子体增强化学气相沉积法工艺,在脊形波导周围沉积一层300nm厚的SiO2层或有机物BCB绝缘层;( 4 ) Deposit a layer of 300nm thick SiO layer or organic BCB insulating layer around the ridge waveguide with plasma enhanced chemical vapor deposition process;

(5)接着利用光刻和化学湿法刻蚀,去除激光器脊形波导上方的SiO2层或有机物BCB绝缘层,露出其InGaAs欧姆接触层;(5) Then use photolithography and chemical wet etching to remove the SiO2 layer or organic BCB insulating layer above the laser ridge waveguide to expose its InGaAs ohmic contact layer;

(6)用磁控溅射的方法,在整个激光器结构的上方分别镀上100nm厚的Ti和400nm厚的Au,结合光刻工艺和化学湿法刻蚀,在脊条上方露出InGaAs的欧姆接触层上形成Ti-Au金属P电极;(6) Using the method of magnetron sputtering, 100nm thick Ti and 400nm thick Au are respectively plated on the entire laser structure, combined with photolithography and chemical wet etching, the ohmic contact of InGaAs is exposed above the ridges A Ti-Au metal P electrode is formed on the layer;

(7)接着把整个激光器晶片减薄到150μm后,在基底材料的下方蒸镀上500nm厚的Au-Ge-Ni合金作为n电极;(7) After thinning the entire laser wafer to 150 μm, a 500 nm-thick Au-Ge-Ni alloy is evaporated below the base material as the n-electrode;

(8)接着把得到激光器芯片的侧边区、相移调整区、增益区和第二个啁啾光栅的各个P电极用金丝连接引出,形成各侧边区、相移调整区、增益区和第二个啁啾光栅的P电极;简化的方案是激光器芯片的所有侧边区的P电极用金丝连接在一起引出成为总的侧边区P电极,所有相移调整区的P电极用金丝连接在一起引出成为总的相移调整区P电极。(8) Then connect and lead each P electrode of the obtained laser chip side region, phase shift adjustment region, gain region and the second chirped grating with a gold wire to form each side region, phase shift adjustment region, and gain region and the P electrode of the second chirped grating; the simplified solution is that the P electrodes of all side regions of the laser chip are connected together with gold wires to become the total side region P electrodes, and the P electrodes of all phase shift adjustment regions are used The gold wires are connected together and lead out to become the P electrode of the overall phase shift adjustment area.

由本发明单元分布反馈式半导体激光器组成的多波长激光器阵列芯片的制作,与单一波长的分布反馈式半导体激光器相比,只需要为各个单元激光器制作不用的线性啁啾光栅,除此之外其余的制作过程是完全相同的。The manufacture of the multi-wavelength laser array chip composed of the unit distributed feedback semiconductor laser of the present invention, compared with the single wavelength distributed feedback semiconductor laser, only needs to make unused linear chirped gratings for each unit laser, and other The making process is exactly the same.

综上所述,本发明的分布反馈式半导体激光器装置的光栅由两个线性啁啾光栅(也可为取样周期线性啁啾的取样光栅,其选作激射信道的±1级子光栅也是线性啁啾光栅)通过无光栅的增益区串联而成;其中第一个光栅的电极由三个相互隔离的电极组成,这个光栅中间电极所对应部分为相移调整区,它的两侧电极对应部分为侧边区;第二个啁啾光栅所对应部分可以是无增益的无源区,也可以是由一个或三个电极控制的有源区;相邻的相移调整区、侧边区、增益区和第二个啁啾光栅的电极通过某种方式相电隔离。在第一个啁啾光栅的侧边区、相移调整区注入不同电流密度时,可在相应的啁啾光栅某特定周期处引入一个电流控制的真实相移(或等效相移)。通过改变侧边区、相移调整区注入电流,就可以连续调节激光器第一个啁啾光栅在不同的光栅周期处发生激射,从而可连续调节激光器的激射波长以满足ITU-T标准要求。在激光器总工作电流保持不变的条件下,只要通过改变侧边区、相移调整区注入电流的比例,就能够精细调控激光器的激射波长,且激光器保持相似的域值和激射输出功率。与此同时,第二个啁啾光栅作为宽谱反射器,可以把这个激光器产生的在大部分激光,从第一个光栅的外端面反射出去。或者,当第二个啁啾光栅结构是与第一个光栅完全相同的三电极光栅结时,在两个啁啾光栅的三个电极通以相同的电流情况下,这个激光器装置在激射时,激射的激光有更好的单模特性,且线宽更窄。In summary, the grating of the distributed feedback type semiconductor laser device of the present invention consists of two linear chirped gratings (also can be the sampling grating of sampling cycle linear chirp, and the ± 1st order sub-grating that it is selected as the lasing channel is also linear Chirped grating) is connected in series through the gain area without grating; the electrode of the first grating is composed of three mutually isolated electrodes, the corresponding part of the middle electrode of the grating is the phase shift adjustment area, and the corresponding part of the electrodes on both sides of the grating is is the side region; the corresponding part of the second chirped grating can be a passive region without gain, or an active region controlled by one or three electrodes; the adjacent phase shift adjustment region, side region, The electrodes of the gain region and the second chirped grating are electrically isolated in some way. When different current densities are injected into the side region and phase shift adjustment region of the first chirped grating, a current-controlled real phase shift (or equivalent phase shift) can be introduced at a specific period of the corresponding chirped grating. By changing the injection current in the side region and phase shift adjustment region, the first chirped grating of the laser can be continuously adjusted to lasing at different grating periods, so that the lasing wavelength of the laser can be continuously adjusted to meet the requirements of ITU-T standards . Under the condition that the total operating current of the laser remains constant, the lasing wavelength of the laser can be finely regulated by changing the injection current ratio of the side region and the phase shift adjustment region, and the laser maintains a similar threshold value and lasing output power . At the same time, the second chirped grating acts as a broad-spectrum reflector, which can reflect most of the laser light generated by this laser from the outer end face of the first grating. Or, when the second chirped grating structure is exactly the same three-electrode grating junction as the first grating, when the three electrodes of the two chirped gratings are connected with the same current, the laser device will , the lasing laser has better single-mode characteristics and narrower linewidth.

以上所述只是本发明的优选方式,应当指出:对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也应视为本发明的保护范围。The above is only the preferred mode of the present invention, it should be pointed out that for those of ordinary skill in the art, without departing from the principle of the present invention, some improvements and modifications can also be made, and these improvements and modifications should also be considered Be the protection scope of the present invention.

Claims (9)

1.分布反馈式半导体激光器装置,其特征在于:所述装置的光栅由两个啁啾光栅通过无光栅的增益区串联而成,或者是由两个取样周期啁啾的取样光栅通过无光栅的增益区串联而成;其中第一个啁啾光栅的电极由三个相互电隔离的电极组成,这个光栅中间电极所对应部分为相移调整区,它的两侧电极对应部分为侧边区;第二个啁啾光栅所对应部分是无增益的无源区,或者是由一个或多个电极控制的有源区;通过改变激光器啁啾光栅的侧边区和中间相移调整区电极注入电流比例,引发线性啁啾光栅在不同的光栅周期位置产生激射,进而精细调节激光器的激射波长。1. Distributed feedback type semiconductor laser device, it is characterized in that: the grating of described device is formed by two chirped gratings through the gain region without grating in series, or is by the sampling grating of two sampling period chirps through the gain region without grating The gain area is connected in series; the electrode of the first chirped grating is composed of three mutually electrically isolated electrodes, the corresponding part of the middle electrode of the grating is the phase shift adjustment area, and the corresponding part of the electrodes on both sides is the side area; The corresponding part of the second chirped grating is a passive area without gain, or an active area controlled by one or more electrodes; by changing the side area of the laser chirped grating and the middle phase shift adjustment area electrode injection current Ratio, triggering the linear chirped grating to generate lasing at different grating period positions, and then fine-tuning the lasing wavelength of the laser. 2.根据权利要求1所述的分布反馈式半导体激光器装置,其特征在于:第一个啁啾光栅的两个侧边区电极通过导线连接在一起,形成同一个侧边区电极。2. The distributed feedback semiconductor laser device according to claim 1, characterized in that: the two side region electrodes of the first chirped grating are connected together by wires to form the same side region electrode. 3.根据权利要求1所述的分布反馈式半导体激光器装置,其特征在于:第一个啁啾光栅的两个侧边区长度相同。3. The distributed feedback semiconductor laser device according to claim 1, characterized in that: the two side regions of the first chirped grating have the same length. 4.根据权利要求1所述的分布反馈式半导体激光器装置,其特征在于:第二个啁啾光栅与第一个啁啾光栅是完全相同的啁啾光栅,其对应的电极和结构也相同,均由完全相同的两个侧边区和一个相移调整区组成。4. The distributed feedback semiconductor laser device according to claim 1, characterized in that: the second chirped grating is the same chirped grating as the first chirped grating, and its corresponding electrodes and structures are also the same, Both are composed of identical two side regions and a phase shift adjustment region. 5.根据权利要求4所述的分布反馈式半导体激光器装置,其特征在于:第二个啁啾光栅的两个侧边区电极,用导线连接在一起,形成同一个侧边区电极。5. The distributed feedback semiconductor laser device according to claim 4, characterized in that: the two side region electrodes of the second chirped grating are connected together by wires to form the same side region electrode. 6.根据权利要求4所述的分布反馈式半导体激光器装置,其特征在于:两个啁啾光栅的四个侧边区电极,用导线连接在一起形成同一个侧边区电极,两个啁啾光栅的两个相移调整区电极,用导线连接在一起形成同一个相移调整区电极。6. The distributed feedback semiconductor laser device according to claim 4, characterized in that: four side region electrodes of two chirped gratings are connected together with wires to form the same side region electrodes, and two chirped gratings The two phase shift adjustment area electrodes of the grating are connected together by wires to form the same phase shift adjustment area electrode. 7.根据权利要求1所述的分布反馈式半导体激光器装置,其特征在于:相邻的相移调整区、侧边区、增益区和第二个啁啾光栅的各电极间通过相距一定距离、或者通过注入氦离子、或者通过刻蚀电隔离沟的方式相电隔离。7. The distributed feedback semiconductor laser device according to claim 1, characterized in that: each electrode of the adjacent phase shift adjustment region, side region, gain region and the second chirped grating passes through a certain distance, Either by implanting helium ions, or by etching an electrical isolation trench. 8.一种分布反馈式半导体激光器单片集成阵列,其特征在于:由权利要求1至7中任意一项所述的分布反馈式半导体激光器装置构成。8. A monolithic integrated array of distributed feedback semiconductor lasers, characterized in that it is composed of the distributed feedback semiconductor laser device according to any one of claims 1 to 7. 9.一种光子集成发射芯片模块,其特征在于:由激光监测器阵列、权利要求8所述的分布反馈式半导体激光器单片集成阵列、调制器阵列、功率均衡器阵列和复用器,通过选择区外延生长或对接生长技术,依次生长集成到同一外延晶片上构成。9. A photonic integrated emission chip module, characterized in that: by laser monitor array, distributed feedback type semiconductor laser monolithic integrated array, modulator array, power equalizer array and multiplexer according to claim 8, through Selected area epitaxial growth or docking growth technology, which is sequentially grown and integrated on the same epitaxial wafer.
CN201710827089.2A 2017-09-14 2017-09-14 Distributed feedback semiconductor laser device and photonic integrated emission chip module Active CN107565381B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710827089.2A CN107565381B (en) 2017-09-14 2017-09-14 Distributed feedback semiconductor laser device and photonic integrated emission chip module

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710827089.2A CN107565381B (en) 2017-09-14 2017-09-14 Distributed feedback semiconductor laser device and photonic integrated emission chip module

Publications (2)

Publication Number Publication Date
CN107565381A CN107565381A (en) 2018-01-09
CN107565381B true CN107565381B (en) 2019-12-06

Family

ID=60980899

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710827089.2A Active CN107565381B (en) 2017-09-14 2017-09-14 Distributed feedback semiconductor laser device and photonic integrated emission chip module

Country Status (1)

Country Link
CN (1) CN107565381B (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108649427B (en) * 2018-05-10 2020-09-01 常州工学院 High-efficiency lasing output DFB semiconductor laser device and photon integrated emission chip
CN109560459A (en) * 2018-12-03 2019-04-02 中国科学院半导体研究所 Low chirp distributed Blatt reflective tunable laser and preparation method thereof
CN113224638A (en) * 2021-04-08 2021-08-06 常州工学院 SBG semiconductor laser device for sampling by using electrode
CN114552390B (en) * 2022-02-25 2023-09-19 常州工学院 A semiconductor laser device that uses intermittent energization of ridges to control the lasing wavelength
CN114825037A (en) * 2022-04-08 2022-07-29 南京大学 Directly modulated multi-section tunable laser

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2378311A (en) * 2001-08-03 2003-02-05 Marconi Caswell Ltd Tunable Laser
CN100583579C (en) * 2008-10-06 2010-01-20 南京大学 Manufacture method and device of single-chip integrated semiconductor laser array
CN101750671B (en) * 2009-12-23 2012-09-26 南京大学 Planar waveguide Bragg grating and laser thereof based on reconstruction-equivalent chirp and equivalent apodization
CN102916340B (en) * 2012-02-08 2015-01-21 南京大学 Phase-shift electric-control sampling grating semiconductor laser and setting method therefor
CN105161977A (en) * 2015-10-08 2015-12-16 南京大学(苏州)高新技术研究院 Asymmetric phase shift and apodization sampling raster and DFB laser

Also Published As

Publication number Publication date
CN107565381A (en) 2018-01-09

Similar Documents

Publication Publication Date Title
CN107565381B (en) Distributed feedback semiconductor laser device and photonic integrated emission chip module
CN100444482C (en) Method and device for preparing semiconductor laser based on reconstruction-equivalent chirp technology
CN110401105B (en) Monolithically integrated narrow linewidth laser and method of fabrication
US20200335940A1 (en) High-order bragg grating single-mode laser array
CN101938083B (en) Manufacture method of bi-distributed feedback laser double-amplifier based on gamma waveguide
JP4954992B2 (en) Semiconductor light reflecting element, semiconductor laser using the semiconductor light reflecting element, and optical transponder using the semiconductor laser
CN103151702B (en) Phase shift electric control DFB semiconductor laser device and preparation method thereof
US7242699B2 (en) Wavelength tunable semiconductor laser apparatus
CN108649427B (en) High-efficiency lasing output DFB semiconductor laser device and photon integrated emission chip
JPH11251691A (en) Series coupled dfb laser
CN108471046B (en) Semiconductor laser and control method
US7177335B2 (en) Semiconductor laser array with a lattice structure
US20160336719A1 (en) Integrated semiconductor laser device and semiconductor laser module
WO2019072185A1 (en) SEMICONDUCTOR LASER HAVING A GAIN COUPLING DISTRIBUTED FEEDBACK AND METHOD OF MANUFACTURING THE SAME
JP6588859B2 (en) Semiconductor laser
CN105071219B (en) A kind of adjustable double Wavelength distribution feedback type semiconductor laser device
CN118825769B (en) Lateral amorphous silicon photonic crystal laser, laser array and preparation method
CN105140779A (en) Backup type semiconductor laser based on reconstructing-equivalent chirp technology
WO2020151290A1 (en) On-chip integrated semiconductor laser structure and manufacturing method thereof
US6432735B1 (en) High power single mode laser and method of fabrication
CN112928599B (en) Single-chip integrated mode-tunable chaotic laser and manufacturing and control method thereof
CN113991423A (en) Semiconductor laser based on distributed phase compensation technology
JP2014135351A (en) Semiconductor optical element, integrated type semiconductor optical element and method of manufacturing the same
Su et al. 48 channels 100-GHz tunable laser by integrating 16 DFB lasers with high wavelength-spacing uniformity
CN108493763B (en) A kind of semiconductor laser device and manufacturing method

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant