EXACT FORWARD SCATTERING OF A CO2-LASER BEAM FROM A RELATIVISTIC PLASMA-WAVE BY TIME-RESOLVED FREQUENCY MIXING IN AGGAS2

Citation
A. Lal et al., EXACT FORWARD SCATTERING OF A CO2-LASER BEAM FROM A RELATIVISTIC PLASMA-WAVE BY TIME-RESOLVED FREQUENCY MIXING IN AGGAS2, Review of scientific instruments, 68(1), 1997, pp. 690-693
Citations number
5
Categorie Soggetti
Physics, Applied","Instument & Instrumentation
ISSN journal
00346748
Volume
68
Issue
1
Year of publication
1997
Part
2
Pages
690 - 693
Database
ISI
SICI code
0034-6748(1997)68:1<690:EFSOAC>2.0.ZU;2-F
Abstract
In the UCLA plasma beat wave accelerator, a high intensity two frequen cy CO2 laser (lambda(1) = 10.6 mu m, lambda(1) = 10.3 mu m) is used to drive a large amplitude relativistic plasma wave. The plasma wave act s as a moving phase grating and scatters the incident pump waves into Stokes and anti-Stokes sidebands (omega(1)-omega(p), omega(2)+omega(p) ). The observation of these sidebands in the forward direction confirm s the presence of the relativistic plasmon, and also gives an estimate of the amplitude-length product (n(1)/n(0)xL) of the wave. Since the Stokes and anti-Stokes signals are picosecond pulses at 10.9 and 10.0 mu m, respectively, this Light cannot be time resolved directly on a c onventional detector or streak camera. The forward scattered light can be analyzed, however, by mixing the 10 mu m light with visible light from a laser diode (670 nm) in a nonlinear crystal (AgGaS2) to produce frequency shifted light at 630 nm. The intensity of the 630 nm light is proportional to the product of the intensities of the two incident laser pulses, and can be time resolved on a streak camera. Experimenta l results for the plasma wave amplitude, spatial length, and temporal length are shown. (C) 1997 American Institute of Physics.