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85033176527
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private communication
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W. Kruer (private communication, 1996).
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14
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85033166853
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Persistent anti-correlation of stimulated Raman scatter and stimulated Brillouin scatter in laser produced plasmas
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submitted to
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D. S. Montgomery, B. J. MacGowan, R. K. Kirkwood, J. D. Moody, C. A. Back, S. H. Glenzer, G. S. Stone, B. B. Afeyan, R. L. Berger, W. L. Kruer, B. F. Lasinski, D. H. Munro, E. A. Williams, D. Desenne, and C. Rous-seaux. "Persistent anti-correlation of stimulated Raman scatter and stimulated Brillouin scatter in laser produced plasmas," submitted to Phys. Rev. Lett. (1996).
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16
-
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85033173301
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-
note
-
Collisional absorption effects are ignored because for the particular examples considered, propagation lengths are speckle lengths and for plasma densities and temperatures of interest, these effects are a correction.
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-
-
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17
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0012623512
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1. In such models, however, density is not strictly conserved. Such a model is commonly used in studies of self focusing: A. J. Schmitt, Phys. Fluids 31, 3079 (1988); H. A. Rose and D. F. DuBois, Phys. Fluids B 5, 3337 (1993).
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Phys. Fluids
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Schmitt, A.J.1
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18
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36448999524
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1. In such models, however, density is not strictly conserved. Such a model is commonly used in studies of self focusing: A. J. Schmitt, Phys. Fluids 31, 3079 (1988); H. A. Rose and D. F. DuBois, Phys. Fluids B 5, 3337 (1993).
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Phys. Fluids B
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Rose, H.A.1
DuBois, D.F.2
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21
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85033176385
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The Landau damping term has been simplified by omitting a factor of 1/(1+ρ)
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The Landau damping term has been simplified by omitting a factor of 1/(1+ρ).
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-
-
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22
-
-
85033185238
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-
Spatial gain narrowing may cause the variation across a hot spot to occur on scales smaller than a speckle width
-
Spatial gain narrowing may cause the variation across a hot spot to occur on scales smaller than a speckle width.
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-
-
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23
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85033166766
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It is further assumed that the loss of coherence due to the various scattering processes is small, which is consistent with small reflectivities
-
It is further assumed that the loss of coherence due to the various scattering processes is small, which is consistent with small reflectivities.
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-
-
-
24
-
-
85033171324
-
-
Except for a divergence related to free electromagnetic transport
-
Except for a divergence related to free electromagnetic transport.
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-
-
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27
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0000028237
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P. Mounaix, D. Pesme, W. Rozmus, and M. Casanova, Phys. Fluids B 5, 3304 (1993).
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Mounaix, P.1
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31
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85033170849
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-
note
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0.7,.
-
-
-
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32
-
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85033165423
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This would be the reflectivity in the usual sense if the incident laser beam were spatially uniform rather than a hot spot
-
This would be the reflectivity in the usual sense if the incident laser beam were spatially uniform rather than a hot spot.
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-
-
-
33
-
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85033184772
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There is no qualitative change in the results as this parameter varies between l.E-8 and 1.E-4
-
There is no qualitative change in the results as this parameter varies between l.E-8 and 1.E-4.
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-
-
-
35
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0027559209
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T. Kolber, W. Rozmus, and V. T. Tikhonchuk, Phys. Rev. Lett. 70, 1810 (1993); Phys. Fluids B 5, 138 (1993); Phys. Plasmas 2, 256 (1995).
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Kolber, T.1
Rozmus, W.2
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36
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0000320428
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T. Kolber, W. Rozmus, and V. T. Tikhonchuk, Phys. Rev. Lett. 70, 1810 (1993); Phys. Fluids B 5, 138 (1993); Phys. Plasmas 2, 256 (1995).
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Phys. Fluids B
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37
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36449006171
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T. Kolber, W. Rozmus, and V. T. Tikhonchuk, Phys. Rev. Lett. 70, 1810 (1993); Phys. Fluids B 5, 138 (1993); Phys. Plasmas 2, 256 (1995).
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Phys. Plasmas
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41
-
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85033165623
-
-
note
-
If Landau damping dominates collisional damping, then Langmuir wave momentum is transferred to superthermal electrons which will take a significantly longer time to equilibrate with the ions. In such a regime there will be a nonlocal relationship between momentum injection due to the fundamental SRS process, and the transfer of this momentum to the ions.
-
-
-
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42
-
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85033174134
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-
note
-
SRS, which is simply related to the total Langmuir wave damping in the strongly damped regime.
-
-
-
-
44
-
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36549091865
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S. Skupsky, R. W. Short, T. Kessler, R. S. Craxton, S. Letzring, and J. M. Soures, J. Appl. Phys. 66, 3456 (1989).
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Letzring, S.5
Soures, J.M.6
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45
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36449007583
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-
A. J. Schmitt, Phys. Fluids B 3, 186 (1991); R. L. Berger, B. F. Lasinski, T. B. Kaiser, E. A. Williams, A. B. Langdon, and B. I. Cohen, Phys. Fluids B 5, 2243 (1993).
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Phys. Fluids B
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Schmitt, A.J.1
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46
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36449003771
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A. J. Schmitt, Phys. Fluids B 3, 186 (1991); R. L. Berger, B. F. Lasinski, T. B. Kaiser, E. A. Williams, A. B. Langdon, and B. I. Cohen, Phys. Fluids B 5, 2243 (1993).
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Phys. Fluids B
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Berger, R.L.1
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Williams, E.A.4
Langdon, A.B.5
Cohen, B.I.6
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47
-
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0029509340
-
-
Strictly speaking this is only true for ISI, since one-dimensional SSD has a preferred direction. Two-dimensional SSD, while still not isotropic, is closer to that ideal. See J. E. Rothenberg, Proc. SPIE 2633, 634 (1995).
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Proc. SPIE
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Rothenberg, J.E.1
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48
-
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85033186280
-
-
Since this is a higher order process, models which do not strictly conserve momentum may not accurately predict the altered plasma flow
-
Since this is a higher order process, models which do not strictly conserve momentum may not accurately predict the altered plasma flow.
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-
-
|