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0038294750
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B. G. Logan, C. M. Celata, J. Kwan, E. P. Lee, M. Leitner, P. A. Seidl, S. S. Yu, J. J. Barnard, A. Friedman, W. R. Meier, and R. C. Davidson, Laser Part. Beams 20, 369 (2002); C. M. Celata, F. M. Bieniosek, E. Henestroza, J. W. Kwan, E. P. Lee, G. Logan, L. Prost, P. A. Seidl, J. L. Vay, W. L. Waldron, S. S. Yu, J. J. Barnard, D. A. Callahan, R. H. Cohen, A. Friedman, D. P. Grote, S. M. Lund, A. Molvik, W. M. Sharp, G. Westenskow, R. C. Davidson, P. Efthimion, E. Gilson, L. R. Grisham, I. Kaganovich, H. Qin, E. A. Startsev, S. Bernal, Y. Cui, D. Feldman, T. F. Godlove, I. Haber, J. Harris, R. A. Kishek, H. Li, P. G. O'Shea, B. Quinn, M. Reiser, A. Valfells, M. Walter, Y. Zou, D. V. Rose, and D. R. Welch, Phys. Plasmas 10, 2063 (2003); S. S. Yu, W. R. Meier, R. P. Abbott, J. J. Barnard, T. Brown, D. A. Callahan, C. Debonnel, P. Heitzenroeder, J. F. Latkowski, B. G. Logan, S. J. Pemberton, P. F. Peterson, D. V. Rose, G. L. Sabbi, W. M. Sharp, and D. R. Welch, Fusion Sci. Technol. 44, 266 (2003).
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Westenskow, G.20
Davidson, R.C.21
Efthimion, P.22
Gilson, E.23
Grisham, L.R.24
Kaganovich, I.25
Qin, H.26
Startsev, E.A.27
Bernal, S.28
Cui, Y.29
Feldman, D.30
Godlove, T.F.31
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Harris, J.33
Kishek, R.A.34
Li, H.35
O'Shea, P.G.36
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Latkowski, J.F.9
Logan, B.G.10
Pemberton, S.J.11
Peterson, P.F.12
Rose, D.V.13
Sabbi, G.L.14
Sharp, W.M.15
Welch, D.R.16
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12
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3142721671
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note
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e, = 4 eV). Therefore, the electron thermal velocity is 50 times smaller than the ion beam velocity, and unless the plasma density is 50 times larger than the ion beam density, the electron thermal velocity is much smaller than ion beam velocity.
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14
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0001231909
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D. R. Welch, D. V. Rose, B. V. Oliver, T. C. Genoni, R. E. Clark, C. L. Olson, and S. S. Yu, Phys. Plasmas 9, 2344 (2002); D. R. Welch, D. V. Rose, W. M. Sharp, C. L. Olson, and S. S. Yu, Laser Part. Beams 20, 621 (2002).
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0038359467
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16
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3142687998
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note
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b, and the skin depth is larger than the beam radius [for example, see Fig. 3(c)]. In this case the ion beam current is not neutralized: both the electron current and the displacement current are small compared to ion beam current and can be neglected. As a result, the displacement current can be neglected for all cases in Eq. (12).
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21
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0036478182
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3142696722
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See EPAPS Document No. E-PHPAEN-11-025407 for movies showing highly complex collective behavior of the electron motion during the entry of the intense beam into the background plasma. A direct link to this document may be found in the online article's HTML reference section. The document may also be reached via the EPAPS homepage (http://www.aip.org/pubservs/epaps.html) or from ftp.aip.org in the directory/epaps. See the EPAPS homepage for more information
-
See EPAPS Document No. E-PHPAEN-11-025407 for movies showing highly complex collective behavior of the electron motion during the entry of the intense beam into the background plasma. A direct link to this document may be found in the online article's HTML reference section. The document may also be reached via the EPAPS homepage (http://www.aip.org/pubservs/epaps.html) or from ftp.aip.org in the directory/epaps. See the EPAPS homepage for more information.
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