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Color switching of a terahertz quantum cascade laser
Author(s) -
Martin A. Kainz,
Sebastian Schönhuber,
Benedikt Limbacher,
A. M. Andrews,
Hermann Detz,
G. Strasser,
G. Bastard,
K. Unterrainer
Publication year - 2019
Publication title -
applied physics letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.182
H-Index - 442
eISSN - 1077-3118
pISSN - 0003-6951
DOI - 10.1063/1.5093901
Subject(s) - terahertz radiation , lasing threshold , laser , quantum cascade laser , cascade , far infrared laser , population , scattering , materials science , atomic physics , physics , optoelectronics , optics , chemistry , chromatography , demography , sociology
The mode formation of a terahertz Quantum Cascade laser with two optical transitions is studied experimentally. The emission spectrum shows two well separated frequency regions at 3.4 THz and 3.8 THz corresponding to two different upper laser states | 3 ⟩ and | 4 ⟩. From the relative strength of the two colors, population and electron scattering effects for the two states are investigated at different operating temperatures and in the presence of a strong magnetic field. At elevated temperatures, the population of state | 3 ⟩ is continuously reduced, resulting in only the 3.8 THz transition lasing at 140 K. For an applied magnetic field, the elastic scattering channel from | 4 ⟩ → | 3 ⟩ is progressively suppressed, resulting in laser emission switching from 3.4 THz to 3.8 THz.The mode formation of a terahertz Quantum Cascade laser with two optical transitions is studied experimentally. The emission spectrum shows two well separated frequency regions at 3.4 THz and 3.8 THz corresponding to two different upper laser states | 3 ⟩ and | 4 ⟩. From the relative strength of the two colors, population and electron scattering effects for the two states are investigated at different operating temperatures and in the presence of a strong magnetic field. At elevated temperatures, the population of state | 3 ⟩ is continuously reduced, resulting in only the 3.8 THz transition lasing at 140 K. For an applied magnetic field, the elastic scattering channel from | 4 ⟩ → | 3 ⟩ is progressively suppressed, resulting in laser emission switching from 3.4 THz to 3.8 THz.

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