Detailed study on optical properties of Li2B4O7 for down conversion to millimeter waves |
344 |
398 |
56 |
High-resolution terahertz spectrometer with up to 110 m single-pass base |
1934 |
2130 |
222 |
Millimetre-wave range optical properties of BIBO |
1853 |
1926 |
80 |
Detailed study on optical properties of Li2B4O7 for down-conversion to millimeter waves |
306 |
389 |
87 |
Snapshots of Dirac fermions near the Dirac point in topological insulators |
7150 |
7123 |
6 |
The efficiency of THz wave generation in β-BBO under visible and IR FS pulse pump |
272 |
331 |
66 |
Temperature phase-matching tuning of nonlinear ZnGeP2 crystal for frequency conversion under noncritical spectral phase-matching |
1145 |
1143 |
2 |
Birefringence of GaSe1-xSx, x = 0 - 0.44, crystals at mid-IR and THz range |
1253 |
1479 |
242 |
Physical origins of double peak phase matching in GaSe |
804 |
1029 |
234 |
Optical properties of Te-doped GaSe cristal |
2715 |
2708 |
4 |
Phase matching in RT KTP crystal for down-conversion into the THz range |
2777 |
2750 |
3 |
Phase-matching in KTP crystal for THz wave generation at room temperature and 81 K |
1376 |
1370 |
3 |
Numerical study of multiline CO laser frequency conversion in a ZnGeP2 crystal to the THz range |
592 |
795 |
219 |
Using oxide nonlinear crystals to convert frequencies to the THz range |
306 |
307 |
2 |
Doping as a mean to improve mechanical properties for GaSe |
1751 |
2004 |
311 |
Optical properties and terahertz radiation generation in a Li2B4O7 crystal |
1121 |
1117 |
2 |
Optical properties of β-BBO and potential for THz applications |
2660 |
2803 |
160 |
Optimization on the frequency conversion of LiGaS2 crystal |
1019 |
1012 |
2 |
Modification and AB-initio spectroscopic application of modified commerce terahertz spectrometer by using homemade parts |
740 |
917 |
187 |
Nonlinear absorption in GaSe1-xSx crystals in the range of 680-1080 nm |
761 |
913 |
164 |
Perspective material and applications of uncooled metal bolometers |
376 |
380 |
4 |
CO laser frequency mixing in nonlinear crystals ZnGeP2 and GaSe |
3413 |
3403 |
3 |
Growth of GaSe and GaS single crystals |
1731 |
1718 |
9 |
Observation of a different birefringence order at optical and THz frequencies in LBO crystal |
2189 |
2169 |
4 |
Doubling of THz radiation frequency in nonlinear borate crystals |
385 |
385 |
2 |
GaSe:Er3+ crystals for SHG in the infrared spectral range |
3744 |
3723 |
7 |
The dielectric tensor rotation angle and optical properties of a nonlinear crystal of bismuth triborate in the millimeter wave range |
1072 |
1140 |
77 |
Impact of fs and ns pulses on indium and sulfur doped gallium selenide crystals |
5445 |
5375 |
7 |
Prototype of topographical-target trace gas analyzer operating at THz range |
816 |
981 |
182 |
Sum and difference frequency generation in a PIT crystal |
481 |
482 |
2 |
Modification and ab-initio spectroscopic application of modified commerce terahertz spectrometer by using homemade parts |
2442 |
2705 |
287 |
Intensive terahertz emission from GaSe0.91S0.09 under collinear difference frequency generation |
2565 |
2558 |
3 |
The multi-photon induced Fano effect |
702 |
772 |
73 |
Down-conversion in doped GaSe for spectroscopic applications |
1746 |
2045 |
337 |
The dielectric tensor rotation angle and optical properties of a nonlinear crystal of bismuth triborate in the millimeter-wave range |
989 |
989 |
2 |
Model studies of THz-range generation by down-conversion in GaSe and GaSeS crystals |
1300 |
1586 |
298 |
Single and double-element doped GaSe for nonlinear applications |
667 |
876 |
219 |
Dispersion properties of sulfur doped gallium selenide crystals studied by THz TDS |
2729 |
2704 |
5 |
Potential of sub-THz-wave generation in Li2B4O7 nonlinear crystal at room and cryogenic temperatures |
2230 |
2290 |
80 |
Generating femtosecond pulses in the mid-IR and THz ranges in GaSe1-xTex crystals |
1269 |
1259 |
4 |
Temperature dependence of terahertz optical properties of LBO and perspectives of applications in down-converters |
1152 |
1280 |
142 |
Comment on “GaSe1-xSx and GaSe1-xTex thick crystals for broadband terahertz pulses generation” [Appl. Phys. Lett. 99, 081105 (2011)] |
991 |
990 |
2 |
SHG in γ-Ga2S3 powder |
1040 |
1367 |
341 |
Characterization of Bridgman grown GaSe:Al crystals |
4921 |
4900 |
5 |
Verification of an integral figure of merit for mid-IR nonlinear crystals |
718 |
714 |
3 |
Optical properties of vanadium and nitrogen doped 4H and 6H-SiC |
1501 |
1782 |
319 |
Optical properties and potential of LB4 for THz wave generation |
767 |
836 |
80 |
Optical rectification and down-conversion of FS pulses into mid-IR and THz range in GaSe1-xSx |
577 |
719 |
152 |
Frequency conversion of mode-locked and Q-switched CO laser radiation with efficiency up to 37% |
1039 |
1038 |
4 |
Dielectric properties of BiB3O6 crystal in the sub-THz range |
590 |
634 |
52 |
Algorithm for estimating the efficiency of uncooled bolometers based on metals and their alloys |
1163 |
1163 |
4 |
Optical rectification in β-BBO |
1838 |
2047 |
252 |
Comparative studies of terahertz-based optical properties in transmission/reflection modes of GaSe: S and measurement of its scattering losses due to surface roughness for efficient terahertz generation |
295 |
296 |
1 |
Physical origins of double peak phase matcing in GaSe |
625 |
800 |
184 |
Prospects of controlling the propagation of high-power THz radiation by passive optical elements including 3D printed |
286 |
339 |
61 |
Widely linear and non-phase-matched optical-to-terahertz conversion on GaSe:Te crystals |
2200 |
2191 |
6 |
Optical rectification and down-conversion of fs pulses into mid-IR and THz range in GaSe1-xSx |
1183 |
1476 |
316 |
Remote imaging by nanosecond terahertz spectrometer with standoff detector |
1941 |
1890 |
3 |
Prospects of controlling the propagation of high power THz radiation by passive optical elements including 3D printed |
416 |
459 |
46 |
Growth and optical properties of solid solution crystals GaSe1-xSx |
2519 |
2507 |
7 |
Optimal Te-doping in GaSe for non-linear applications |
2589 |
2579 |
5 |
Three-stage frequency conversion of sub-microsecond multiline CO laser pulse in a single ZnGeP2 crystal |
551 |
552 |
3 |
Properties of oxide nonlinear crystals in the wavelength range over 600 μm |
132 |
154 |
26 |
Difference frequency generation of CO and CO2 lasers in PbIn6Te10 crystal |
1522 |
1843 |
337 |
Doped GaSe crystals for laser frequency conversion |
4511 |
4890 |
425 |
Optical properties of non-linear crystal grown from the melt GaSe–AgGaSe2 |
4317 |
5004 |
745 |
Optical properties of KTP crystals and their potential for terahertz generation |
912 |
1122 |
217 |
THz pulse generation in ZnGeP2 with near-IR pumping |
329 |
372 |
47 |
Terahertz birefringence and dichroism of KTA crystal |
1721 |
1923 |
220 |
Characterization of optical quality of GaSe:Al crystals by exciton absorption peak parameters |
2680 |
2669 |
8 |
Optical properties and application of GaSe: AgGaSe2 crystal |
3395 |
3525 |
184 |
IR-to-THz down conversion in nonlinear Gase:Al crystals |
1307 |
1475 |
180 |
LBO: optical properties and potential for THz application |
2861 |
2836 |
13 |
Laser-induced damage threshold of ZnGeP2 crystal for (sub)picosecond 1-μm laser pulse |
410 |
410 |
1 |
CO laser sum-frequency comb for atmosphere sensing |
696 |
696 |
3 |
Tellurium and sulfur doped GaSe for mid-IR applications |
3198 |
3193 |
6 |
Aspects for efficient wide spectral band THz generation via CO2 laser down conversion |
1391 |
1709 |
326 |
Model studies of THz-range generation by down-conversion in GaSe and GaSes crystals |
731 |
897 |
174 |
New nonlinear crystal Ga2S3 for IR applications |
1290 |
1503 |
248 |