The temperature dependence of 1.3-and 1.5-mu m compressively strained InGaAs(P) MQW semiconductor lasers

Citation
Af. Phillips et al., The temperature dependence of 1.3-and 1.5-mu m compressively strained InGaAs(P) MQW semiconductor lasers, IEEE S T QU, 5(3), 1999, pp. 401-412
Citations number
54
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Eletrical & Eletronics Engineeing
Journal title
IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS
ISSN journal
1077260X → ACNP
Volume
5
Issue
3
Year of publication
1999
Pages
401 - 412
Database
ISI
SICI code
1077-260X(199905/06)5:3<401:TTDO11>2.0.ZU;2-O
Abstract
We have studied experimentally and theoretically the spontaneous emission f rom 1,3- and 1.5-mu m compressively strained InCaAs(P) multiple-quantum-wel l lasers in the temperature range 90-400 K to determine the variation of ca rrier density n with current I up to threshold. We find that the current co ntributing to spontaneous emission at threshold I-Rad is always well behave d and has a characteristic temperature T-0 (I-Rad) approximate to T, as pre dicted by simple theory. This implies that the carrier density at threshold is also proportional to temperature. Below a breakpoint temperature T-B, w e find I proportional to n(Z), where Z = 2, and the total current at thresh old I-th also has a characteristic temperature T-0(I-th) approximate to T, showing that the current is dominated by radiative transitions right up to threshold, Above T-B, Z increases steadily to Z approximate to 3 and T-0 (I -th) decreases to a value less than T/3. This behavior is explained in term s of the onset of Auger recombination above T-B. a conclusion supported by measurements of the pressure dependence of I-th From our results, we estima te that, at 300 K, Auger recombination accounts for 50% of I-th in the 1.3- mu m laser and 80% of I-th, in the 1.5-mu m laser, Measurements of the spon taneous emission and differential efficiency indicate that a combination of increased optical losses and carrier overflow into the barrier and separat e confinement heterostructure regions may further degrade T-0 (I-th) above room temperature.