TY - JOUR
T1 - High-power, continuous-wave, current-tunable, single-mode quantum-cascade distributed-feedback lasers at λ ≅ 5.2 and λ ≅ 7.95 μm
AU - Gmachl, Claire
AU - Capasso, Federico
AU - Tredicucci, Alessandro
AU - Sivco, Deborah L.
AU - Baillargeon, James N.
AU - Hutchinson, Albert L.
AU - Cho, Alfred Y.
PY - 2000/2/15
Y1 - 2000/2/15
N2 - Quantum-cascade distributed-feedback lasers with high-power, continuous-wave (cw), tunable, single-mode emission are reported. The emission wavelengths are near 5.2 and 7.95 μm. The lasers are operated at liquid-nitrogen temperature and above. A maximum output power of >100 mW is obtained per facet at 80 K for both wavelengths, which is the result of careful positioning of the peak gain with respect to the Bragg wavelength. Continuous tuning with either heat-sink temperature or cw current is demonstrated. The tuning coefficients are 0.35 nm/K (5.2 μm) and 0.51 nm/K (7.95 μm) for thermal tuning and vary from 20 to 40 nm/A for tuning with current. The lasers are being used in high-resolution and high-sensitivity gas-sensing applications.
AB - Quantum-cascade distributed-feedback lasers with high-power, continuous-wave (cw), tunable, single-mode emission are reported. The emission wavelengths are near 5.2 and 7.95 μm. The lasers are operated at liquid-nitrogen temperature and above. A maximum output power of >100 mW is obtained per facet at 80 K for both wavelengths, which is the result of careful positioning of the peak gain with respect to the Bragg wavelength. Continuous tuning with either heat-sink temperature or cw current is demonstrated. The tuning coefficients are 0.35 nm/K (5.2 μm) and 0.51 nm/K (7.95 μm) for thermal tuning and vary from 20 to 40 nm/A for tuning with current. The lasers are being used in high-resolution and high-sensitivity gas-sensing applications.
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U2 - 10.1364/OL.25.000230
DO - 10.1364/OL.25.000230
M3 - Article
C2 - 18059838
AN - SCOPUS:0000605349
SN - 0146-9592
VL - 25
SP - 230
EP - 232
JO - Optics Letters
JF - Optics Letters
IS - 4
ER -