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RLE Progress Report No - Research Laboratory of Electronics - MIT

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1<br />

0.1<br />

ne<br />

Te<br />

Ti<br />

0.01<br />

100 200 300 400<br />

Location from target (z) in µ m<br />

Figure 1: Laser produced plasma in TRIDENT; n e in units <strong>of</strong> n e /n cr ,<br />

T e and T i in keV (from Ref.1).<br />

The basic experimental setup is illustrated in Figure 13 <strong>of</strong> our last report 2 , where a laser beam is<br />

focused into a plasma that is created from a plastic foil. 1 The plasma is approximately<br />

homogeneous along the beam path, but changes its density and temperature as it flows away<br />

from the target. By focusing the laser at different positions from the target, experimentalists have<br />

studied the SRS backscattering for the different parameters shown in Figure 1.<br />

Considering a weak nonlinear interaction <strong>of</strong> the five waves, we express this as nonlinearly<br />

coupled field amplitudes that change slowly in time and space. The equations that describe the<br />

interaction between the slowly varying amplitudes ( a 1<br />

, a ,<br />

2<br />

a ,<br />

3<br />

a and<br />

4<br />

a , for the Laser, BEMW,<br />

5<br />

EPW, BEPW and IAW, respectively) are:<br />

( ∂ + v ∂ + γ ) a = −K<br />

a SRS<br />

a , (1)<br />

t g1<br />

x 1 1<br />

t<br />

+ vg2∂<br />

x<br />

+ 2<br />

)<br />

2 =<br />

2<br />

1<br />

3<br />

3<br />

( ∂ γ a K a SRS<br />

a , (2)<br />

( ∂ + v ∂ + γ ) a = K a a − K a a , (3)<br />

t<br />

g3<br />

x 3 3 SRS 1 2<br />

t<br />

+ vg4∂<br />

x<br />

+ 4)<br />

a4<br />

=<br />

LDI<br />

t<br />

+ vg5∂<br />

x<br />

+ 5)<br />

a5<br />

=<br />

LDI<br />

3<br />

LDI<br />

( ∂ γ K a a , (4)<br />

3<br />

5<br />

( ∂ γ K a a . (5)<br />

4<br />

4<br />

5<br />

2<br />

In Eqs. (1)–(5), a<br />

<br />

= W<br />

/ ω ,<br />

<br />

W ,<br />

<br />

v and<br />

g<br />

γ are the wave action density, wave energy density,<br />

<br />

group velocity and damping rate <strong>of</strong> mode . The nonlinear coupling coefficients are:<br />

K<br />

SRS<br />

≈<br />

2<br />

ε<br />

o<br />

1/ 2<br />

2<br />

e k ⎛ ω ⎞<br />

3 pe ,<br />

m<br />

e<br />

⎜ ⎟<br />

4<br />

⎝ω1ω<br />

2ω<br />

3 ⎠<br />

K<br />

LDI<br />

≈<br />

2<br />

ε<br />

o<br />

m e<br />

1/ 2<br />

e ω pe ⎛ ω ⎞<br />

5<br />

4v<br />

⎜<br />

⎟<br />

.<br />

Te ⎝ω3ω<br />

4 ⎠<br />

Such model equations have also been considered in the past 3 but their solution was not explored<br />

in much detail nor related to experiments in relatively homogeneous plasmas.<br />

2 R. J. Focia, A. Bers, and A. K. Ram., “Plasma Electrodynamics and Applications: Section 5 – Electromagnetic Decay<br />

Instability in Single Hot Spot Geometry”, <strong>Progress</strong> <strong>Report</strong> <strong>No</strong>. 142, <strong>MIT</strong> <strong>Research</strong> <strong>Laboratory</strong> <strong>of</strong> <strong>Electronics</strong>, Cambridge,<br />

2000 (http://rleweb.mit.edu/Publications/pr142/bers142.pdf).<br />

3 J. A. Heikkinen and S. J. Karttunen, “Intensity Saturation <strong>of</strong> Stimulated Raman Scattering by Ion-Wave Coupling,” Phys.<br />

Fluids, 29(4), 1291 (1986).

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