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Beam divergence and COD issues in double barrier separate confinement heterostructure laser diodes

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Wybrane pełne teksty z tego czasopisma
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Języki publikacji
EN
Abstrakty
EN
The double barrier separate confinement heterostructure (DBSCH) design aimed at reduction of vertical beam divergence and increase of catastrophic optical damage (COD) level for high power laser diodes (LDs) operation is presented. Insertion of thin, wide-gap barrier layers at the interfaces between waveguide and cladding layers of SCH gives an additional degree of freedom in design making possible more precise shaping of the optical field distribution in the laser cavity. By comparison with the large optical cavity (LOC) heterostructure design it has been shown that the low beam divergence emission, of DBSCH LDs can be attributed to the soft-profiled field distribution inside the cavity. This 'soft mode profile' seems to determine narrow laser beam emission rather than the field distribution width itself. The potential problem with the soft-profiled but relatively narrow (at half-maximum) mode distribution is a lower COD level. Widening of the mode profile by the heterostructure design corrections can increase it, but care must be taken to avoid excessive decrease of confinement factor (gamma). As a result it is shown that DBSCH design is possible, where the low be divergence and high COD level is achieved simultaneously. Wide stripe gain-guided LDs based on GaAsP / AIGaAs DBSCH SQW structures have been manufactured according to the design above. Gaussian-shaped narrow directional characteristics are in relatively good agreement with modelling predictions. Vertical beam divergences are 13-15° and 17-18° FWHM for design versions experimentally investigated. Threshold current densities of the order of 350-270 Acm-2 and slope efficiencies of 0.95 and 1.15 W / A have been recorded for these two versions, respectively. Optical power at the level of 1 W has been achieved. The version with lower beam divergence proves to be more durable. Higher optical power levels are to be obtained after heterostructure doping optimisation.
Rocznik
Strony
167--173
Opis fizyczny
Bibliogr. 22 poz., 6 rys.
Twórcy
autor
  • Institute of Electronic Electronic Materials Technology, 131 Wólczyńska Str., 01-919 Warsaw, Poland., amalag@time.edu.pl
Bibliografia
  • [1] S.J. Matthews, “(Beam characterization) Good fundamentals”, Laser Focus World 82–86, (October 2002).
  • [2] C.J. Chang-Hasnain et al., “Spatial mode structure of broad-area semiconductor quantum well lasers”, APL 54 (3), 205–207 (1989).
  • [3] D. Botez and M. Ettenberg, “Beamwidth approximations for fundamental mode in symmetric doubleheterojunction lasers”, IEEE JQE QE-14 (11), 827–830 (1978).
  • [4] A. Kozłowska and A. Malag, “ Far-field emission characteristics of high-power laser diodes”, Proc. SPIE 5120, 178–183 (2003).
  • [5] D. Botez, “High power, Al-free diode lasers”, Compound Semiconductors 5 (6), (1999).
  • [6] M.A. Emanuel et al., “High-efficiency AlGaAs-based laser diode at 808 nm with large transverse spot size”, IEEE PTL 8 (10), 1291–1293 (1996).
  • [7] A. Knauer et al., “Optimization of GaAsP/AlGaAs-based QW laser structures for high power 800 nm operation”, J. Electron. Mat. 29 (1), 53–56 (2000).
  • [8] J. Sebastian et al., “High power 810-nm GaAsP-AlGaAs diode lasers with narrow beam divergence”, IEEE JSTQE 7 (2), 334–339 (2001).
  • [9] N.A Pikhtin et al., “16 W continuous-wave output power from 100 ¹m-aperture laser with quantum well asymmetric heterostructure”, Electron. Lett. 40 (22), 1413–1414 (2004).
  • [10] B.S. Ryvkin and E.A. Avrutin, “Improvement of differential quantum efficiency and power output by waveguide asymmetry in separate-confinement-structure diode lasers”, IEE Proc.-Optoelectron. 151 (4), 232–236 (2004).
  • [11] M. Buda et al., “Analysis of 6-nm AlGaAs SQW lowconfinement laser structures for very high power operation”, IEEE JST QE 3 (2), 173–179 (1997).
  • [12] G. Iordache et al., “High power CW output from low confinement asymmetric structure diode laser”, Electron. Lett. 35 (2), 148–149 (1999).
  • [13] G. Yang et al., “High performance 980-nm ridge waveguide laser with a nearly circular beam”, IEEE PTL 16 (4), 981–983 (2004).
  • [14] G. Lin et al., “Extremely small vertical far-field angle of InGaAs-AlGaAs quantum-well lasers with specially designed cladding structure”, IEEE PTL 8 (12), 1588–1590 (1996).
  • [15] G.W. Yang, J.Y. Xu, Z.T. Xu, J.M. Zhang, L.H. Hen, and Q.M. Wang, “Theoretical investigation on quantum well lasers with extremely low vertical beam divergence and low threshold current”, JAP 3 (1), 8–14 (1998).
  • [16] A. Malag and B. Mroziewicz, “Vertical beam divergence of double-barrier multiquantum well (DBMQW) (AlGa)As heterostructure lasers”, Journal of the Lightwave Technology 14 (6), 514–1518 (1996).
  • [17] A. Malag and W. Strupinski, “MOVPE-grown (AlGa)As double-barrier multiquantum well (DBMQW) laser diode with low vertical beam divergence”, J. Crystal Growth 170, 408–412 (1997).
  • [18] A. Malag, A. Kozłowska, and M. Wesołowski, “Effect of Al-content reduction in (AlGa)As cladding layers of MOVPE grown high-power laser diodes”, Booklet of Extended Abstracts Xth EW MOVPE, Lecce, Italy, 235–238 (June 8–11, 2003).
  • [19] K. Shigihara et al., “High-power 980-nm ridge waveguides laser diodes including an asymmetrically expanded optical field normal to active layer”, IEEE JQE 38 (8), 1081– 1088 (2002).
  • [20] Y.C. Chen, R.G. Waters, and R.J. Dalby, “Singlequantum- well laser with 11.2 degree transverse beam divergence”, Electron. Lett. 26, 1348–1350 (1990).
  • [21] G. Yang et al., “Highly reliable high-power 980-nm pump laser”, IEEE PTL 16 (11), 2403–2405 (2004).
  • [22] D. Botez, “Design considerations and analytical approximations for high continuous-wave power, broad waveguide diode lasers”, APL 74, 3102–3104 (1999).
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-article-BPG5-0005-0052
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