PACS numbers

52.57.−z Laser inertial confinement
  1. Celebrating the 65th anniversary of the Russian Federal Nuclear Center — All-Russian Research Institute of Experimental Physics (Scientific session of the Physical Sciences Division of the Russian Academy of Sciences, 6 October 2010)54 387–427 (2011)
    01.10.Fv, 01.65.+g, 05.70.Ce, 07.35.+k, 07.55.Db, 28.52.−s, 28.70.+y, 42.55.−f, 42.62.−b, 47.20.−k, 47.27.wj, 47.40.−x, 52.57.−z, 61.05.C−, 64.30.−t, 74.25.−q, 84.30.Ng, 84.70.+p, 85.70.−w (all)
  2. S.G. Garanin “High-power lasers and their applications in high-energy-density physics studies54 415–421 (2011)
    42.55.−f, 42.62.−b, 52.57.−z (all)
  3. V.B. Rozanov “Feasibility of spherical fusion target compression under two-beam laser irradiation47 359–370 (2004)
    28.52.Cx, 52.57.−z (all)
  4. O.N. Krokhin “Laser fusion: state of the art and prospects45 1305–1306 (2002)
    28.52.−s, 52.57.−z (all)
  5. A.F. Andreev, B.B. Kadomtsev et alNikolai Gennadievich Basov (on his seventieth birthday)36 (1) 32–33 (1993)
    01.60.+q, 01.10.Cr, 42.50.Gy, 42.55.Px, 42.60.By, 52.57.−z (all)
  6. O.N. Krokhin “Use of Lasers for Plasma Heating14 362–362 (1971)
    52.50.Jm, 52.57.−z, 42.60.Lh (all)
  7. I.I. Metelskii, V.F. Kovalev, V.Yu. Bychenkov “Relativistically nonlinear resonant absorption and harmonic generation of electromagnetic radiation in an inhomogeneous plasma”, accepted
    52.40.Db, 52.35.Hr, 52.38.−r, 42.65.Ky, 52.35.Fp, 52.50.Jm, 52.25.Os, 52.35.−g, 52.30.−q, 52.57.−z (all)
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