Demonstration of 1.3um wavelength range super structure grating DBR laser with wide wavelength tuning range of over 30 nm by introducing carrier confinement layers

Author(s):  
Takahiko Shindo ◽  
Naoki Fujiwara ◽  
Yoshitaka Ohiso ◽  
Tomonari Sato ◽  
Hideaki Matsuzaki
2020 ◽  
Vol 12 (2) ◽  
pp. 1-10 ◽  
Author(s):  
Sani Mukhtar ◽  
Islam Ashry ◽  
Chao Shen ◽  
Tien K. Ng ◽  
Boon S. Ooi ◽  
...  

2017 ◽  
Vol 19 (27) ◽  
pp. 18068-18075 ◽  
Author(s):  
Kacper Parafiniuk ◽  
Lech Sznitko ◽  
Dominika Wawrzynczyk ◽  
Andrzej Miniewicz ◽  
Jaroslaw Mysliwiec

Broad range tunable DFB lasing was achieved by the utilization of two dyes forming molecular aggregates within the polymeric matrix.


1996 ◽  
Vol 32 (3) ◽  
pp. 433-441 ◽  
Author(s):  
H. Ishii ◽  
H. Tanobe ◽  
F. Kano ◽  
Y. Tohmori ◽  
Y. Kondo ◽  
...  

1999 ◽  
Vol 607 ◽  
Author(s):  
H. Q. Le ◽  
C.-H. Lin ◽  
S. J. Murry ◽  
J. Zheng ◽  
S.-S. Pei

AbstractSb mid-IR laser can be used in external configuration to achieve wide wavelength tuning range. At low temperature, gain media with band-edge wavelengths between 3.3 to 4 pm have been demonstrated with wavelength tuning up to ∼9% of the center wavelength. Power output from few tens of mW to 0.2-W peak, 20-mW average was achieved. Type-II Sb laser promises the possibility of such performance at higher temperature, e. g. 200 K. However, significant trade-off must be considered between tuning range and power and efficiency. Optimization requires consideration of both basic wafer design and cavity geometry.


1993 ◽  
Vol 5 (2) ◽  
pp. 126-129 ◽  
Author(s):  
Y. Tohmori ◽  
Y. Yoshikuni ◽  
T. Tamamura ◽  
H. Ishii ◽  
Y. Kondo ◽  
...  

1986 ◽  
Vol 6 (6) ◽  
pp. 361-371 ◽  
Author(s):  
Susan M. Grenci ◽  
George R. Bird ◽  
Brian W. Keelan ◽  
Ahmed H. Zewail

We have operated a dye laser over a broad wavelength range (593.8–667.0 nm) by shifting the dye emission profile with incremental changes of solvent composition. This was accomplished with the laser operating continuously, and only minor adjustment of the laser optics was required. Solvent tuning was facilitated by the critical dependence of the optimum laser wavelength on concentration of the second solvent. Using the known solvent-sensitive laser dye 9-diethylaminobenzo[a]phenoxaz-5-one (DBP), 87% of the tuning range from pure xylenes to pure methanol was covered by cumulative addition of 24 vol. % methanol to the starting xylenes solution. The optimum dye concentration was found to be independent of solvent composition, so that maximum laser power could be maintained by mixing equimolar dye solutions in the two solvents. These results establish the practicality of solvent-tuning as a method of conducting laser experiments over a broad wavelength range.


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