TY - JOUR
T1 - Transversely superimposed gratings for narrow far-field terahertz surface emission of nonlinear quantum cascade lasers
AU - Demmerle, Frederic
AU - Oberhausen, Wolfhard
AU - Burghart, Dominik
AU - Wolf, Alexander
AU - Veerabathran, Ganpath Kumar
AU - Krakofsky, Jonas Heiko
AU - Schmeiduch, Hannes
AU - Böhm, Gerhard
AU - Amann, Markus Christian
N1 - Publisher Copyright:
© 2017 Society of Photo-Optical Instrumentation Engineers (SPIE).
PY - 2018/1/1
Y1 - 2018/1/1
N2 - We present terahertz (THz) surface emission by difference frequency generation in nonlinear quantum cascade lasers operating at room temperature. The device comprises two separate, transversely superimposed gratings, one for selective feedback for the midinfrared (MIR) modes and one for normal surface emission of the generated THz radiation. This allows for narrow far-field THz emission with an enhanced extraction over the entire device length with improved electrical and thermal properties compared to previous devices relying on Cherenkov phase matching. The MIR grating is realized as a higher order loss-coupled distributed feedback grating for single-mode emission at two distinct wavelengths. Its position determines the position of the standing wave pattern of the MIR modes and of the nonlinear polarization wave. This allows for a precise placement of the second-order top grating, which leads to perpendicular surface emission. The device emits in a single-lobed far-field with a full width half maximum of 3.5 deg in single-mode operation at room temperature.
AB - We present terahertz (THz) surface emission by difference frequency generation in nonlinear quantum cascade lasers operating at room temperature. The device comprises two separate, transversely superimposed gratings, one for selective feedback for the midinfrared (MIR) modes and one for normal surface emission of the generated THz radiation. This allows for narrow far-field THz emission with an enhanced extraction over the entire device length with improved electrical and thermal properties compared to previous devices relying on Cherenkov phase matching. The MIR grating is realized as a higher order loss-coupled distributed feedback grating for single-mode emission at two distinct wavelengths. Its position determines the position of the standing wave pattern of the MIR modes and of the nonlinear polarization wave. This allows for a precise placement of the second-order top grating, which leads to perpendicular surface emission. The device emits in a single-lobed far-field with a full width half maximum of 3.5 deg in single-mode operation at room temperature.
KW - gratings
KW - nonlinear optics
KW - semiconductor lasers
KW - terahertz
UR - http://www.scopus.com/inward/record.url?scp=85029782488&partnerID=8YFLogxK
U2 - 10.1117/1.OE.57.1.011007
DO - 10.1117/1.OE.57.1.011007
M3 - Article
AN - SCOPUS:85029782488
SN - 0091-3286
VL - 57
JO - Optical Engineering
JF - Optical Engineering
IS - 1
M1 - 011007
ER -