Self-consistent calculation of the lasing eigenmode of the dielectrically apertured Fabry-Perot microcavity with idealized or distributed Bragg reflectors

1997 ◽  
Vol 33 (12) ◽  
pp. 2319-2326 ◽  
Author(s):  
Q. Deng ◽  
D.G. Deppe
2010 ◽  
Vol 18 (2) ◽  
Author(s):  
M. Żujewski ◽  
W. Nakwaski

AbstractThe paper describes an impact of various possible inaccuracies in manufacturing of verticalcavity surface-emitting diode lasers (VCSELs), like thicknesses and compositions of their layers different from assumed ones, on VCSEL room-temperature (RT) continuous-wave (CW) threshold performance. To this end, the fully self-consistent comprehensive optical-electrical-thermal-recombination VCSEL model has been applied. While the analysis has been carried out for the 1.3-μm oxide-confined intra-cavity contacted GaInNAs/GaAs VCSEL, its conclusions are believed to be more general and concern most of modern VCSEL designs. As expected, the VCSEL active region has been found to require the most scrupulous care in its fabrication, any uncontrolled variation in compositions and/or thicknesses of its layers is followed by unaccepted RT CW lasing threshold increase. Also spacer thicknesses should be manufactured with care to ensure a proper overlapping of the optical standing wave and both the gain and lossy areas within the cavity. On the contrary, less than 5% thickness changes in distributed-Bragg-reflectors are followed by nearly insignificant changes in VCSEL RT CW threshold. However, exceeding the above limit causes a rapid increase in lasing thresholds. As expected, in all the above cases, VCSELs equipped with larger active regions have been confirmed to require more careful technology. The above results should enable easier organization of VCSEL manufacturing.


2005 ◽  
Vol 10 (1) ◽  
pp. 83-91 ◽  
Author(s):  
N. Samuolienė ◽  
E. Šatkovskis

Herein, the problem of nanocrystaline silicon laser and its importance in microelectronics are discussed upon. The features of vertical Fabry-Perot microcavities made on the base of porous silicon are described. The responses of the reflectivity of the distributed reflection Bragg mirrors and Fabry-Perot microcavities were found using transfer matrixes method for this purpose. Inherent optical parameters of porous silicon, deposited by electrochemical etch, were used in the calculations. The calculation of the reflectivity of the distributed reflection Bragg mirrors with front active layer of nanostructural porous silicon had been examined. In the second part, the features of Fabry-Perot microcavities on variation of the number of layers of the front or rear mirrors are described. The impact of the thickness of the active nanocrystaline silicon spacer between two distributed reflection Bragg mirrors upon the spectra of optical reflectivity of Fabry-Perot microcavities in the wavelength range of 0.4–0.9 µm had been examined as well. The made conclusions are important for improvement of the thickness of the active porous silicon spacer in front of Bragg mirror and the features of Fabry-Perot microcavities.


2012 ◽  
Vol 110 (1) ◽  
pp. 23-28 ◽  
Author(s):  
Jieying Kong ◽  
Sheng Chu ◽  
Jian Huang ◽  
Mario Olmedo ◽  
Weihang Zhou ◽  
...  

Author(s):  
J. Krupka ◽  
A. Cwikla ◽  
M. Mrozowski ◽  
R.N. Clarke ◽  
M.E. Tobar

2021 ◽  
Vol 21 (2) ◽  
pp. 2084-2091
Author(s):  
Ang Li ◽  
Zhenguo Jing ◽  
Yueying Liu ◽  
Qiang Liu ◽  
Zhiyuan Huang ◽  
...  

APL Photonics ◽  
2021 ◽  
Vol 6 (2) ◽  
pp. 026104
Author(s):  
Mirela Malekovic ◽  
Esteban Bermúdez-Ureña ◽  
Ullrich Steiner ◽  
Bodo D. Wilts

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