双波长外腔面发射激光器

邱小浪; 王爽爽; 张晓健; 朱仁江; 张鹏; 郭于鹤洋; 宋晏蓉

doi:10.7498/aps.68.20182261

摘要

双波长激光光源在干涉测量、非线性频率变换产生中红外及太赫兹波段相干辐射等方面有重要的应用. 外腔面发射激光器具有输出功率高、光束质量好、发射波长可设计等突出优势, 非常适合用于双波长的产生. 用有源区为In_0.185Ga_0.815As/GaAs应变多量子阱、设计波长为960 nm, 以及有源区为In_0.26Ga_0.74As/GaAsP_0.02应变多量子阱、设计波长为1080 nm的两块半导体增益芯片, 在一个共线Y型谐振腔中, 获得了激光波长分别为953 nm和1100 nm的双波长输出, 对应光谱线宽为1.1 nm和2.7 nm, 波长间隔147 nm. 室温下, 每块增益芯片的抽运吸收功率均为5.8 W时, 双波长激光器总的输出功率达到293 mW.

关键词:

Abstract

Dual-wavelength laser sources have important applications in the interferometry and the nonlinear-frequency-conversion generated mid-infrared or terahertz-band coherent radiation. Vertical-external-cavity surface-emitting lasers own outstanding advantages such as high output power, good beam quality and flexible emission wavelength, which make them very suitable for dual-wavelength running. In this paper, we employ a collinear Y-type cavity to produce a dual-wavelength laser. There are two semiconductor gain chips in the resonant cavity, one has an active region of In_0.185Ga_0.815As/GaAs strained multiple quantum wells and a designed wavelength of 960 nm, and the other has an active region of In_0.26Ga_0.74As/GaAsP_0.02 strained multiple quantum wells and a target wavelength of 1080 nm. The peak wavelength of the photoluminescence of chip 1 is 950 nm, which is 10 nm shorter than the designed wavelength under weak pump, and the peak wavelength of the photoluminescence of chip 2 is 1094 nm, which is 14 nm longer than the target wavelength under low pump. When the pump power is increased, the peak wavelengths of the photoluminescence of two gain chips are both red-shifted. The oscillating laser wavelengths are centered at 953 nm and 1100 nm, the corresponding full width at half maximum (FWHM) values of the laser spectra are 1.1 nm and 2.7 nm, respectively. The wavelength spacing of the dual-wavelength is 147 nm, and the related mid-infrared coherent radiation is about 7.1 μm on the assumption that the dual-wavelength laser is used for difference frequency generation. When the absorbed pump power of each gain chip is 5.8 W, the total output power of the dual-wavelength laser reaches 293 mW at room temperature.

Keywords:

external cavity surface emitting laser /
dual wavelength /
Y- cavity /
polarizing beam splitter

作者及机构信息

1.
重庆师范大学物理与电子工程学院, 重庆　401331

2.
北京工业大学应用数理学院, 北京　100124

通信作者: 朱仁江, 834083237@qq.com

基金项目: 重庆市基础研究与前沿探索项目(批准号: cstc2015jcyjBX0098, cstc2018jcyjAX0319)、国家自然科学基金(批准号: 61575011)、重庆市高校创新团队项目(批准号: CXTDX201601016)和教育部“蓝火计划”(惠州)产学研联合创新资金项目(批准号: CXZJHZ201728)资助的课题.

Authors and contacts

1.
College of Physics and Electronic Engineering, Chongqing Normal University, Chongqing 401331, China

2.
College of Applied Sciences, Beijing University of Technology, Beijing 100124, China

Corresponding author: Zhu Ren-Jiang, 834083237@qq.com

Funds: Project supported by the Chongqing Research Program of Basic Research and Frontier Technology, China (Grant Nos. cstc2015jcyjBX0098, cstc2018jcyjAX0319), the National Natural Science Foundation of China (Grant No. 61575011), the Foundation for the Creative Research Groups of Higher Education of Chongqing, China (Grant No. CXTDX201601016), and the Blue Fire Plan (Huizhou) of the Industry-University-Research Joint Innovation Project of Ministry of Education of China (Grant No. CXZJHZ201728).

文章全文

参考文献

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施引文献

图 1 双波长VECSEL实验装置示意图

Fig. 1. Schematic of the experimental setup of dual-wavelength VECSEL.

下载: 全尺寸图片幻灯片

图 2 只抽运增益芯片1时所得荧光和激光光谱

Fig. 2. Photoluminescence and laser spectra when gain chip 1 is pumped only.

下载: 全尺寸图片幻灯片

图 3 只抽运增益芯片2所得荧光和激光光谱

Fig. 3. Photoluminescence and laser spectra when gain chip 2 is pumped only.

下载: 全尺寸图片幻灯片

图 4 双波长VECSEL输出的激光光谱图

Fig. 4. Laser spectra of the dual-wavelength VECSEL.

下载: 全尺寸图片幻灯片

图 5 953 nm和1100 nm单独振荡以及双波长工作时VECSEL的输出功率

Fig. 5. Output powers of the VECSEL when only 953 nm or 1100 nm mode oscillating, and dual-wavelength operating.

下载: 全尺寸图片幻灯片

[1]	苏俊宏 2003 红外与激光工程 32 359 Google Scholar Su J 2003 Infrared Laser Eng. 32 359 Google Scholar
[2]	李践 2005 中国生物医学工程学报 24 237 Google Scholar Li J 2005 Chin. J. Biomed. Eng. 24 237 Google Scholar
[3]	Mao Q, Lit J W Y 2002 IEEE Photonic Tech. L. 14 1252 Google Scholar
[4]	Schlager J B, Kawanishi S, Saruwatari M 1991 Electron. Lett. 27 2072 Google Scholar
[5]	Kawase K, Mizuno M, Sohma S, Takahashi H, Taniuchi T, Urata Y, Wada S, Tashiro H, Ito H 1999 Opt. Lett. 24 1065 Google Scholar
[6]	Tittel F K, Richter D, Fried A 2003 Mid-infrared Laser Applications in Spectroscopy (Springer, Berlin, Heidelberg) pp458−529
[7]	Beck M, Hofstetter D, Aellen T, Faist J, Oesterle U, Ilegems M, Gini E, Melchior H 2002 Science 295 301 Google Scholar
[8]	Willer U, Saraji M, Khorsandi A, Geiser P, Schade W 2006 Opt. Laser Eng. 44 699 Google Scholar
[9]	Waynant R W, Ilev I K, Gannot I 2001 Phil. Trans. R. Soc. A 359 635 Google Scholar
[10]	Jeon M Y, Kim N, Shin J, Jeong J S, Han S P, Lee C W, Leem Y A, Yee D S, Chun H S, Park K H 2010 Opt. Express 18 12291 Google Scholar
[11]	Jackson S D 2012 Nat. Photonics 6 423 Google Scholar
[12]	Lee B G, Belkin M A , Audet R , MacArthur J, Diehl L, Pflügl C, Capasso F, Oakley D C, Chapman D, Napoleone A, Bour D, Corzine S, Höfler G, Faist J 2007 Appl. Phys. Lett. 91 231101 Google Scholar
[13]	Schiessl U P, Rohr J 1999 Infrared Phys. Tech. 40 325 Google Scholar
[14]	Budni P A, Pomeranz L A, Lemons M L, Miller C A, Mosto J R, Chicklis E P 2000 J. Opt. Soc. Am 17 723 Google Scholar
[15]	Hastie J E, Calvez S, Dawson M D, Leinonen T, Laakso A, Lyytikäinen J, Pessa M 2005 Opt. Express 13 77 Google Scholar
[16]	Fan L, Hader J, Schillgalies M, Fallahi M, Zakharian A R, Moloney J V, Bedford R, MurrayJ T, Koch S W, Stolz W 2005 IEEE Photonic Tech. L. 17 1764 Google Scholar
[17]	Fallahi M, Fan L, Kaneda Y, Hessenius C, Hader J, Li H, Moloney J V, Kunert B, Stolz W, Koch S W, Murray J, Bedford R 2008 IEEE Photonic Tech. L. 20 1700 Google Scholar
[18]	Maclean A J, Kemp A J, Calvez S, Kim J Y, Kim T, Dawson M D, Burns D 2008 IEEE J. Quantum Elect. 44 216 Google Scholar
[19]	Fallahi M, Hessenius C, Kaneda Y, Hader J, Moloney J V, Kunert B, Stolz W, Koch S W 2009 Nonlinear Optics: Materials, Fundamentals and Applications Honolulu, Hawaii, July 12−17, 2009 pNThC1
[20]	De Groot P J, McGarvey J A 1994 US Patent 5 371
[21]	Keller U, Tropper A C 2006 Phys. Rep. 429 67 Google Scholar
[22]	Zhu R, Wang S, Qiu X, Chen X, Jiang M, Guo-Yu H, Zhang P, Song Y 2018 J. Lumin. 204 663 Google Scholar
[23]	Abram R H, Gardner K S, Riis E, Ferguson A I 2004 Opt. Express 12 5434 Google Scholar
[24]	Alfieri C G, Waldburger D, Golling M, Keller U 2018 IEEE Photonic Tech. L. 30 525 Google Scholar
[25]	Jasik A, Sokół A K, Broda A, Sankowska I, Wójcik-Jedlinska A, Wasiak M, Kubacka-Traczyk J, Muszalski J 2016 Appl. Phys. B 122 23
[26]	Polanik M 2015 Annual Report, Institute of Optoelectronics, Ulm University 3
[27]	Leinonen T, Ranta S, Laakso A, Morozov Y, Saarinen M, Pessa M 2007 Opt. Express 15 13451 Google Scholar
[28]	Hessenius C, Lukowski M, Fallahi M 2012 Appl. Phys. Lett. 101 121110 Google Scholar
[29]	Lukowski M, Hessenius C, Bedford R, Fallagi M 2015 Opt. Lett. 40 4174 Google Scholar
[30]	Zhang F, Gaafar M, Möller C, Stolz W, Koch M, Rahimi-Iman A 2016 IEEE Photonic Tech. L. 28 927
[31]	Sandusky J V, Brueck S R J 1996 IEEE Photonic Tech. L. 8 313 Google Scholar

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