Spectra of mode loss in THz quantum cascade laser with double metal waveguide based on Au, Cu and Ag

Author(s):  
Rustam Khabibullin ◽  
Dmitriy Ushakov ◽  
Alexander Afonenko ◽  
Nikolai Shchavruk ◽  
Dmitriy Ponomarev ◽  
...  
Author(s):  
Rustam Khabibullin ◽  
Dmitriy Ushakov ◽  
Alexander Afonenko ◽  
Nikolay Shchavruk ◽  
Dmitriy Ponomarev ◽  
...  

2017 ◽  
Vol 111 (2) ◽  
pp. 021106 ◽  
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Markus Rösch ◽  
Ileana-Cristina Benea-Chelmus ◽  
Christopher Bonzon ◽  
Martin J. Süess ◽  
Mattias Beck ◽  
...  

2016 ◽  
Vol 50 (10) ◽  
pp. 1377-1382 ◽  
Author(s):  
R. A. Khabibullin ◽  
N. V. Shchavruk ◽  
A. Yu. Pavlov ◽  
D. S. Ponomarev ◽  
K. N. Tomosh ◽  
...  

2006 ◽  
Vol 14 (24) ◽  
pp. 11672 ◽  
Author(s):  
Jonathan A. Fan ◽  
Mikhail A. Belkin ◽  
Federico Capasso ◽  
Suraj Khanna ◽  
Mohamed Lachab ◽  
...  

2011 ◽  
Vol 19 (2) ◽  
pp. 733 ◽  
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Michael Martl ◽  
Juraj Darmo ◽  
Christoph Deutsch ◽  
Martin Brandstetter ◽  
Aaron Maxwell Andrews ◽  
...  

2003 ◽  
Vol 83 (11) ◽  
pp. 2124-2126 ◽  
Author(s):  
Benjamin S. Williams ◽  
Sushil Kumar ◽  
Hans Callebaut ◽  
Qing Hu ◽  
John L. Reno

Author(s):  
R A Khabibullin ◽  
N V Shchavruk ◽  
A Yu Pavlov ◽  
A N Klochkov ◽  
I A Glinskiy ◽  
...  

Author(s):  
Р.А. Хабибуллин ◽  
Н.В. Щаврук ◽  
Д.С. Пономарев ◽  
Д.В. Ушаков ◽  
А.А. Афоненко ◽  
...  

AbstractThe active region of a THz (terahertz) quantum-cascade laser based on three tunnel-coupled GaAs/Al_0.15Ga_0.85As quantum wells with a resonance-phonon depopulation scheme is designed. Energy levels, matrix elements of dipole transitions, and gain spectra are calculated as functions of the applied electric-field strength F and temperature. It is shown that the maximum gain is implemented at a frequency of 3.37 THz and F = 12.3 kV/cm. Based on the proposed design, a quantum-cascade laser emitting at ~3.3 THz with a double metal waveguide and T _max ~ 84 K is fabricated. The activation energy E _ a = 23 meV for longitudinal-optical (LO) phonon emission upon the stimulated recombination of hot electrons from the upper laser level to the lower one is determined from the Arrhenius temperature dependence of the output power.


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