Picosecond two-beam coupling and polarization rotation by scalar gratings in undoped cadmium telluride at 1.064 μm
MS Petrovic, A Suchocki, RC Powell, GC Valley… - Physical Review B, 1991 - APS
We report on the observation of a photorefractive effect with picosecond pulses in a material
that has little or no midgap absorption (less than 0.1 cm− 1). We model our data using rate …
that has little or no midgap absorption (less than 0.1 cm− 1). We model our data using rate …
Frequency doubling and sum frequency generation in semiconductor optical waveguide devices
KA Shore, X Chen, P Blood - Progress in quantum electronics, 1996 - Elsevier
FREQUENCY DOUBLING AND SUM FREQUENCY GENERATION IN SEMICONDUCTOR
OPTICAL WAVEGUIDE DEVICES Page 1 Pergamon Pr0g. 0079-6727(95)00006-2 Quanr. E/em …
OPTICAL WAVEGUIDE DEVICES Page 1 Pergamon Pr0g. 0079-6727(95)00006-2 Quanr. E/em …
Two‐photon‐induced optical switching using a CdTe etalon
AY Hamad, JP Wicksted - Journal of applied physics, 1996 - pubs.aip.org
We report the observation of optical switching in a CdTe etalon at room temperature using
11 ns pulses at 1.064 m radiation. We have also observed optical limiting and pulse …
11 ns pulses at 1.064 m radiation. We have also observed optical limiting and pulse …
Spatial and temporal beam reshaping effects using bulk CdTe
AY Hamad, JP Wicksted, SY Wang… - Journal of applied …, 1995 - pubs.aip.org
Reshaping effects of ns pulses were theoretically and experimentally investigated using bulk
CdTe. The experiments were performed using a 1.064 μm Nd: YAG laser with pulse duration …
CdTe. The experiments were performed using a 1.064 μm Nd: YAG laser with pulse duration …
Transient Energy Transfer by ps‐Laser‐Induced Free‐Carrier and Photorefractive Gratings in CdTe at 1 μm
I Rückmann, J Kornack, J Kolenda… - … status solidi (b), 1992 - Wiley Online Library
Three‐beam mixing is investigated in ps‐transient grating experiments carried out on (110)
CdTe at 1 μm in the case of two‐photon absorption (TPA). The coupling of three transient …
CdTe at 1 μm in the case of two‐photon absorption (TPA). The coupling of three transient …
Transmission second harmonic generation in CdTe at 1.064 μm
MS Petrovic, A Suchocki, RC Powell, G Cantwell - Applied Physics A, 1991 - Springer
Transmission geometry measurements of the efficiency of second harmonic generation in
various thicknesses of CdTe samples were made to determine the conversion efficiency …
various thicknesses of CdTe samples were made to determine the conversion efficiency …
[PDF][PDF] Transmission SecondHarmonic Generation in CdMnTe at 1.064 µm
B Koziarska, L Kowalczyk, A Suchocki… - … Physica Polonica A, 1995 - bibliotekanauki.pl
Second harmonic generation, created by nanosecond Nd: YAG laser pulses at 1.064 µm
with relatively low intensity in Cd _1-x Mn _x Te bulk crystals and thin layers was measured …
with relatively low intensity in Cd _1-x Mn _x Te bulk crystals and thin layers was measured …
[图书][B] Picosecond nonlinear optical properties of undoped cadmium telluride
MS Petrovic - 1991 - search.proquest.com
Scope and method of study. Using near-infrared picosecond light pulses from a Y $\sb3 $ Al
$\sb5 $ O $\sb {12} $: Nd $\sp {3+} $(YAG: Nd) laser, the pulse-probe degenerate four-wave …
$\sb5 $ O $\sb {12} $: Nd $\sp {3+} $(YAG: Nd) laser, the pulse-probe degenerate four-wave …
[图书][B] Nonlinear optical properties of CdTe and laser induced grating in Eu (3+)-doped silicate glasses
AY Hamad - 1996 - search.proquest.com
Scope and method of study. Some of the nonlinear optical properties of CdTe were studied
via the pulse reshaping and optical switching techniques using nanosecond pulses at …
via the pulse reshaping and optical switching techniques using nanosecond pulses at …