scholarly journals Saturation of cross-beam energy transfer for multispeckled laser beams involving both ion and electron dynamics

2019 ◽  
Vol 26 (8) ◽  
pp. 082708 ◽  
Author(s):  
L. Yin ◽  
B. J. Albright ◽  
D. J. Stark ◽  
W. D. Nystrom ◽  
R. F. Bird ◽  
...  
Author(s):  
Stefan Hüller ◽  
Gaurav Raj ◽  
Mufei Luo ◽  
Wojciech Rozmus ◽  
Denis Pesme

Crossed beam energy transfer, CBET, in high-intensity laser–plasma interaction is investigated for the case of optically smoothed laser beams. In the two approaches to laser-driven inertial confinement fusion experiments, the direct-drive and the indirect-drive, CBET is of great importance because it governs the coupling of laser energy to the plasma. We use the two-dimensional wave-coupling code H armony to simulate the transfer between two laser beams with speckle structure that overlap in a plasma with an inhomogeneous flow profile. We compare the CBET dynamics for laser beams with spatial incoherence and with spatio-temporal incoherence; in particular we apply the smoothing techniques using random phase plates (RPPs) and smoothing by spectral dispersion (SSD), respectively. It is found that for laser beams (wavelength λ 0 ) with intensities ( I L ) above I L  ∼ 2 × 10 15  W cm −2 ( λ 0 /0.35 µm) −2 ( T e /keV), both the so-called plasma-induced smoothing as well as self-focusing in intense laser speckles induce temporal incoherence; the latter affects the CBET and the angular distribution of the light transmitted behind the zone of beam overlap. For RPP-smoothed incident beams, the resulting band width of the transmitted light can already be of the same order as the effective band width of the SSD available at major laser facilities. We examine the conditions when spatio-temporal smoothing techniques become efficient for CBET. This article is part of a discussion meeting issue ‘Prospects for high gain inertial fusion energy (part 1)’.


2017 ◽  
Vol 24 (10) ◽  
pp. 103128 ◽  
Author(s):  
R. K. Follett ◽  
D. H. Edgell ◽  
D. H. Froula ◽  
V. N. Goncharov ◽  
I. V. Igumenshchev ◽  
...  

1977 ◽  
Vol 31 (4) ◽  
pp. 253-271 ◽  
Author(s):  
W. M. Tolles ◽  
J. W. Nibler ◽  
J. R. McDonald ◽  
A. B. Harvey

Coherent anti-Stokes Raman spectroscopy (CARS) is a relatively new kind of Raman spectroscopy which is based on a nonlinear conversion of two laser beams into a coherent, laser-like Raman beam of high intensity in the anti-Stokes region. The emission is often many orders of magnitude greater than normal Raman scattering and, because of the coherent and anti-Stokes character of radiation, the method is very useful for obtaining Raman spectra of fluorescing samples, gases in discharges, plasmas, combustion, atmospheric chemistry. In this paper we outline the basic theory behind CARS and describe its unusual effects and drawbacks. We review the research to date on various materials, and indicate the possible future direction, utility and applications of CARS such as surface studies, fluctuation phenomena, reaction dynamics, photochemistry, kinetics, relaxation, and energy transfer.


2006 ◽  
Vol 23 (10) ◽  
pp. 2113 ◽  
Author(s):  
Sarik R. Nersisyan ◽  
Nelson V. Tabiryan ◽  
C. Martin Stickley

2014 ◽  
Vol 47 (4) ◽  
pp. 1252-1260 ◽  
Author(s):  
Bertrand Clair ◽  
Aziza Ikni ◽  
Wenjing Li ◽  
Philippe Scouflaire ◽  
Vincent Quemener ◽  
...  

Non-photochemical laser-induced nucleation (NPLIN) has been a growing field of study since 1996, and more than 40 compounds including organics, inorganics and proteins have now been probed under various conditions (solvents, laser types, laser beamsetc.). The potential advantages of using this technique are significant, in particular polymorphic control. To realize these benefits, the objective is a carefully designed experimental setup and highly controlled parameters, for example temperature and energy density, in order to reduce the uncertainty regarding the origin of nucleation. In this paper, a new experimental setup designed to study NPLIN is reported. After a full technical description of the present setup, the different functionalities of this device will be illustrated through results on glycine. Glycine crystals obtained through NPLIN nucleate at the meniscus and exhibit different morphologies. The nucleation efficiency, as a function of the supersaturation of the solution used and the laser beam energy density, has also been established for a large number of samples, with all other parameters held constant.


2019 ◽  
Vol 399 ◽  
pp. 108916 ◽  
Author(s):  
Jason F. Myatt ◽  
John G. Shaw ◽  
Russell K. Follett ◽  
Dana H. Edgell ◽  
Dustin H. Froula ◽  
...  
Keyword(s):  

2011 ◽  
Vol 18 (2) ◽  
pp. 023108
Author(s):  
Deepak Tripathi ◽  
R. Uma ◽  
V. K. Tripathi

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