Chirped-Probe-Pulse Femtosecond Coherent Anti-Stokes Raman Scattering for Single-Laser-Pulse Flame Temperature Measurements

2010 ◽  
Author(s):  
Daniel R. Richardson ◽  
Robert P. Lucht ◽  
Waruna D. Kulatilaka ◽  
Sukesh Roy ◽  
James R. Gord
Keyword(s):  
Laser Pulse ◽  
Raman Scattering ◽  
Probe Pulse ◽  
Flame Temperature ◽  
Temperature Measurements ◽  
Single Laser Pulse ◽  
Single Laser ◽  
Anti Stokes

Theoretical modeling of single-laser-shot, chirped-probe-pulse femtosecond coherent anti-Stokes Raman scattering thermometry

2011 ◽  
Vol 104 (3) ◽  
pp. 699-714 ◽  
Author(s):  
D. R. Richardson ◽  
R. P. Lucht ◽  
W. D. Kulatilaka ◽  
S. Roy ◽  
J. R. Gord
Keyword(s):  
Raman Scattering ◽  
Probe Pulse ◽  
Theoretical Modeling ◽  
Laser Shot ◽  
Single Laser ◽  
Anti Stokes

Single laser pulse compression via strongly coupled stimulated Brillouin scattering in plasma

2016 ◽  
Vol 23 (7) ◽  
pp. 073516 ◽  
Author(s):  
H. Peng ◽  
Z. H. Wu ◽  
Y. L. Zuo ◽  
Z. M. Zhang ◽  
K. N. Zhou ◽  
...  
Keyword(s):  
Laser Pulse ◽  
Pulse Compression ◽  
Brillouin Scattering ◽  
Stimulated Brillouin Scattering ◽  
Single Laser Pulse ◽  
Strongly Coupled ◽  
Single Laser ◽  
Stimulated Brillouin

All-optical magnetic recording in garnets using a single laser pulse at L-band telecom wavelengths

2021 ◽  
Vol 118 (26) ◽  
pp. 262401
Author(s):  
Antoni Frej ◽  
Andrzej Maziewski ◽  
Andrzej Stupakiewicz
Keyword(s):  
Laser Pulse ◽  
Magnetic Recording ◽  
Single Laser Pulse ◽  
Single Laser ◽  
All Optical ◽  
L Band

scholarly journals Equation-of-state studies using a 10-Hz Nd:YAG laser oscillator

2003 ◽  
Vol 21 (4) ◽  
pp. 615-626 ◽  
Author(s):  
M. SHUKLA ◽  
A. UPADHYAY ◽  
V.K. SENECHA ◽  
P. KHARE ◽  
S. BANDYAOPADHYAY ◽  
...  
Keyword(s):  
Equation Of State ◽  
Laser Pulse ◽  
Beam Quality ◽  
Impedance Matching ◽  
Laser System ◽  
Control Unit ◽  
Aluminum Foil ◽  
Single Laser Pulse ◽  
High Contrast ◽  
Single Laser

A commercial mode locked cavity dumped Nd:YAG dye laser operating at 10 Hz repetition rate is modified to produce a high contrast (>5000:1) single laser pulse while maintaining the energy stability and high beam quality. A trigger generator biases the cavity dumping photodiode, which is triggered externally by a pulse from the microprocessor-based control unit controlling a ∼2 J/200 ps laser chain. In the laser chain, the high contrast (>5000:1) is achieved by an external pulse selector based on single Pockel's cell to select a single laser pulse of high contrast, which is a prerequisite for experimental study of the equation of state. Laser-induced shock velocity measurement in thin aluminum, gold on aluminum, and copper on aluminum foil targets using this modified laser system are also presented. The equation of state of Al, Au, and Cu obtained using an impedance matching technique are in agreement with the reported results of SESAME and simulation results.

Generation of a quasimonoenergetic electron beam using a single laser pulse

Laser Physics ◽  
2006 ◽  
Vol 16 (7) ◽  
pp. 1107-1110 ◽  
Author(s):  
H. Kotaki ◽  
A. Yamazaki ◽  
I. Daito ◽  
M. Kando ◽  
S. V. Bulanov ◽  
...  
Keyword(s):  
Electron Beam ◽  
Laser Pulse ◽  
Single Laser Pulse ◽  
Single Laser

The application of coherent anti-Stokes Raman scattering to temperature measurements in a pulsed high enthalpy supersonic flow

Shock Waves ◽  
1994 ◽  
Vol 4 (3) ◽  
pp. 119-125 ◽  
Author(s):  
D. R. N. Pulford ◽  
D. S. Newman ◽  
A. F. P. Houwing ◽  
R. J. Sandeman
Keyword(s):  
Supersonic Flow ◽  
Raman Scattering ◽  
Temperature Measurements ◽  
High Enthalpy ◽  
Anti Stokes

Crystallization of Amorphous 55wt%Cr-45wt%Ni Films Induced by 60 ns (0.694 μm) Single Laser Pulse

1986 ◽  
Vol 74 ◽  
Author(s):  
I. Ursu ◽  
M. I. Bîrjega ◽  
C. A. Constantin ◽  
M. Dinescu ◽  
I. N. Mihailescu ◽  
...  
Keyword(s):  
Liquid Phase ◽  
Laser Pulse ◽  
Ruby Laser ◽  
Amorphous Matrix ◽  
Normal Incidence ◽  
Single Laser Pulse ◽  
Thermal Gradients ◽  
Single Laser ◽  
Threshold Conditions ◽  
Phase Liquid

AbstractAmorphous 55wt%Cr-45wt%Ni films (60 nm thick) supported on EM copper grids were irradiated in air at normal incidence with a ruby laser (λ∼, 0.694 μm) through a ≈ 1.5 mm diameter diaphragm using one single laser pulse of 60 ns (FWHM) with fluences ranging from 120 to 540 J.m−2. The structure of the irradiated films is studied by TEM and TED. As a rule due to the appearance of thermal gradients between the centre and the mesh edge of the EM grid, the crystallization took place under various conditions of reaction from liquid phase, liquid melted layers , activated diffusion in solid state, to under threshold conditions for the development of the crystalline nuclei in the amorphous matrix. Periodic resonant and unreso-nant structures also developed in the liquid melted layers.

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