scholarly journals PULSED LASER EXCITATION AND OPTICAL DETECTION OF RAYLEIGH WAVES ON A METALLIC SPHERE

1992 ◽  
Vol 02 (C1) ◽  
pp. C1-789-C1-792 ◽  
Author(s):  
X. JIA ◽  
D. ROYER ◽  
G. QUENTIN
Keyword(s):  
Rayleigh Waves ◽  
Laser Excitation ◽  
Optical Detection ◽  
Pulsed Laser

Optical Detection of Rayleigh Waves

1969 ◽  
Vol 40 (8) ◽  
pp. 3408-3409 ◽  
Author(s):  
E. Salzmann ◽  
D. Weismann
Keyword(s):  
Rayleigh Waves ◽  
Optical Detection

scholarly journals Reactive quenching of electronically excited NO<sub>2</sub><sup>∗</sup> and NO<sub>3</sub><sup>∗</sup> by H<sub>2</sub>O as potential sources of atmospheric HO<sub><i>x</i></sub> radicals

2018 ◽  
Vol 18 (19) ◽  
pp. 14005-14015 ◽  
Author(s):  
Terry J. Dillon ◽  
John N. Crowley
Keyword(s):  
Gas Phase ◽  
Laser Excitation ◽  
Pulsed Laser ◽  
Work Rate ◽  
Rate Coefficients ◽  
Phase Reaction ◽  
Gas Phase Reaction ◽  
Upper Limit ◽  
Upper Limits ◽  
Electronically Excited

Abstract. Pulsed laser excitation of NO2 (532–647 nm) or NO3 (623–662 nm) in the presence of H2O was used to initiate the gas-phase reaction NO2∗+H2O → products (Reaction R5) and NO3∗+H2O → products (Reaction R12). No evidence for OH production in Reactions (R5) or (R12) was observed and upper limits for OH production of k5b/k5<1×10-5 and k12b/k12<0.03 were assigned. The upper limit for k5b∕k5 renders this reaction insignificant as a source of OH in the atmosphere and extends the studies (Crowley and Carl, 1997; Carr et al., 2009; Amedro et al., 2011) which demonstrate that the previously reported large OH yield by Li et al. (2008) was erroneous. The upper limit obtained for k12b∕k12 indicates that non-reactive energy transfer is the dominant mechanism for Reaction (R12), though generation of small but significant amounts of atmospheric HOx and HONO cannot be ruled out. In the course of this work, rate coefficients for overall removal of NO3∗ by N2 (Reaction R10) and by H2O (Reaction R12) were determined: k10=(2.1±0.1)×10-11 cm3 molecule−1 s−1 and k12=(1.6±0.3)×10-10 cm3 molecule−1 s−1. Our value of k12 is more than a factor of 4 smaller than the single previously reported value.

Broadband Optical Limiting and CCD Sensor Protection From Nanosecond-Pulsed Laser Threat With Reverse Saturable Absorbers

1997 ◽  
Vol 479 ◽  
Author(s):  
V. Dentan ◽  
P. Feneyrou ◽  
F. Soyer ◽  
M. Vergnolle ◽  
P. Le Barny ◽  
...  
Keyword(s):  
Excited States ◽  
Nonlinear Optical ◽  
Laser Excitation ◽  
Pulsed Laser ◽  
Saturable Absorbers ◽  
Nanosecond Pulsed Laser ◽  
Optical Limiter ◽  
Linear And Nonlinear ◽  
Ccd Arrays ◽  
Pulsed Laser Irradiation

AbstractWe study in detail the linear and nonlinear optical properties of a heavy metal substituted naphthalocyanine reverse saturable absorber (RSA). The excited states involved in the RSA process under nanosecond pulsed laser excitation in the visible are fully characterized. We then demonstrate that this material can be used as an efficient optical limiter for protecting silicium CCD arrays from destruction due to nanosecond-pulsed laser irradiation in the visible.

Time-resolved luminescence of CdGaInS4 under pulsed laser excitation at 30 K

1986 ◽  
Vol 133 (1) ◽  
pp. 379-388 ◽  
Author(s):  
M. Colocci ◽  
F. Fermi ◽  
R. Querzoli ◽  
A. Vinattieri
Keyword(s):  
Laser Excitation ◽  
Pulsed Laser ◽  
Time Resolved

Lasing efficiency of krypton ions in the (8–14)-nm band upon pulsed laser excitation

2020 ◽  
Vol 50 (4) ◽  
pp. 408-413
Author(s):  
A N Nechay ◽  
S A Garakhin ◽  
A Ya Lopatin ◽  
V N Polkovnikov ◽  
D G Reunov ◽  
...  
Keyword(s):  
Laser Excitation ◽  
Pulsed Laser ◽  
Lasing Efficiency
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