Reliable polarization control of VCSELs through monolithically integrated surface gratings: A comparative theoretical and experimental study

被引:77
作者
Debernardi, P [1 ]
Ostermann, JM
Feneberg, M
Jalics, C
Michalzik, R
机构
[1] Politecn Torino, CNR, IEIIT, I-10129 Turin, Italy
[2] Univ Ulm, Optoelect Dept, D-89069 Ulm, Germany
关键词
polarization control; semiconductor laser modeling; surface grating; vertical. cavity surface-emitting laser (VCSEL);
D O I
10.1109/JSTQE.2004.841712
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Vertical cavity surface-emitting lasers (VCSELs) with a well-defined and predictable polarization of the emitted light are sought for a number of applications. In this paper, we show that one can define and stabilize the polarization of single- and multimode oxide-confined VCSELs with a monolithically integrated dielectric surface grating. In recent years, we have developed a three-dimensional, fully vectorial model for VCSELs, which proved to nicely reproduce the experimental results of quite complex structures, such as noncircular devices and phase-coupled VCSEL arrays. This software allows for the first time to analyze the effects of a dielectric grating in the output facet cap layer and its capability to fix the polarization of the emitted light. It is here employed as a design tool, yielding excellent agreement with the experimental data. Since the simulations predict the polarization behavior to be sensitively dependent on the grating parameters, hundreds of VCSELs with 99 different parameter sets, two grating orientations and active diameters of 4 and 7 mum have been analyzed. Even VCSELs with eight or more coexisting modes turned out to be linearly, polarized with an orthogonal polarization suppression ratio in excess of 15 dB. Theoretical and experimental emission far-fields are compared, and it is shown that diffraction side lobes can be prevented with properly chosen grating parameters which simultaneously ensure full polarization stability.
引用
收藏
页码:107 / 116
页数:10
相关论文
共 33 条
[1]   Characteristics of polarization switching from the low to the high frequency mode in vertical-cavity surface-emitting lasers [J].
Ackemann, T ;
Sondermann, M .
APPLIED PHYSICS LETTERS, 2001, 78 (23) :3574-3576
[2]  
BAVA GP, 2001, PHYS REV A, V63
[3]   Vertical cavity surface emitting lasers incorporating structured mirrors patterned by electron-beam lithography [J].
Berseth, CA ;
Dwir, B ;
Utke, I ;
Pier, H ;
Rudra, A ;
Iakovlev, VP ;
Kapon, E ;
Moser, M .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 1999, 17 (06) :3222-3225
[4]   POLARIZATION CHARACTERISTICS OF QUANTUM-WELL VERTICAL CAVITY SURFACE EMITTING LASERS [J].
CHANGHASNAIN, CJ ;
HARBISON, JP ;
FLOREZ, LT ;
STOFFEL, NG .
ELECTRONICS LETTERS, 1991, 27 (02) :163-165
[5]   CONTROL OF VERTICAL-CAVITY LASER POLARIZATION WITH ANISOTROPIC TRANSVERSE CAVITY GEOMETRIES [J].
CHOQUETTE, KD ;
LEIBENGUTH, RE .
IEEE PHOTONICS TECHNOLOGY LETTERS, 1994, 6 (01) :40-42
[6]   Single-mode, single-polarization VCSELs via elliptical surface etching: Experiments and theory [J].
Debernardi, P ;
Unold, HJ ;
Maehnss, J ;
Michalzik, R ;
Bava, GP ;
Ebeling, KJ .
IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS, 2003, 9 (05) :1394-1405
[7]   Coupled mode theory: A powerful tool for analyzing complex VCSELs and designing advanced device features [J].
Debernardi, P ;
Bava, GP .
IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS, 2003, 9 (03) :905-917
[8]   Features of vectorial modes in phase-coupled VCSEL arrays: Experiments and theory [J].
Debernardi, P ;
Bava, GP ;
di Sopra, FM ;
Willemsen, MB .
IEEE JOURNAL OF QUANTUM ELECTRONICS, 2003, 39 (01) :109-119
[9]   Influence of anisotropies on transverse modes in oxide-confined VCSELs [J].
Debernardi, P ;
Bava, GP ;
Degen, C ;
Fischer, I ;
Elsässer, W .
IEEE JOURNAL OF QUANTUM ELECTRONICS, 2002, 38 (01) :73-84
[10]   Two-variable reduction of the San Miguel-Feng-Moloney model for vertical-cavity surface-emitting lasers [J].
Erneux, T ;
Danckaert, J ;
Panajotov, K ;
Veretennicoff, I .
PHYSICAL REVIEW A, 1999, 59 (06) :4660-4667