Measurements of the divergence of fast electrons in laser-irradiated spherical targets

In recent experiments using directly driven spherical targets on the OMEGA laser system, the energy in fast electrons was found to reach ∼1% of the laser energy at an irradiance of ∼1.1 × 1015 W/cm2. The fraction of these fast electrons absorbed in the compressed fuel shell depends on their angular divergence. This paper describes measurements of this divergence deduced from a series of shots where Mo-coated shells of increasing diameter (D) were suspended within an outer CH shell. The intensity of the Mo–Kα line and the hard x-ray radiation were found to increase approximately as ∼D2, indicating wide divergence of the fast electrons. Alternative interpretations of these results (electron scattering, radiation excitation of Kα, and an electric field due to return current) are shown to be unimportant.

[1]  H. Baldis,et al.  Growth and saturation of the two‐plasmon decay instability , 1983 .

[2]  P. B. Radha,et al.  Role of hot-electron preheating in the compression of direct-drive imploding targets with cryogenic D2 ablators. , 2008, Physical review letters.

[3]  J. Lindl,et al.  Inertial Confinement Fusion: The Quest for Ignition and Energy Gain Using Indirect Drive , 1998 .

[4]  U. Feldman,et al.  Hard x-ray transmission crystal spectrometer at the OMEGA-EP laser facility. , 2010, The Review of scientific instruments.

[5]  E. Williams,et al.  A variational approach to parametric instabilities in inhomogeneous plasmas III: Two-plasmon decay , 1997 .

[6]  Jonathan D. Zuegel,et al.  Hard x-ray detectors for OMEGA and NIF , 2001 .

[7]  Indrin J Chetty,et al.  Spiral computed tomography phase-space source model in the BEAMnrc/EGSnrc Monte Carlo system: implementation and validation. , 2013, Physics in medicine and biology.

[8]  L Maigne,et al.  Comparison of GATE/GEANT4 with EGSnrc and MCNP for electron dose calculations at energies between 15 keV and 20 MeV , 2011, Physics in medicine and biology.

[9]  G B Zimmerman,et al.  Direct measurement of energetic electrons coupling to an imploding low-adiabat inertial confinement fusion capsule. , 2012, Physical review letters.

[10]  S. Skupsky,et al.  Effects of non-Maxwellian electron populations in non-LTE simulations of laser-plasma thermal transport and implosion experiments , 1986 .

[11]  E. Moses,et al.  The National Ignition Facility , 2004 .

[12]  S. Skupsky,et al.  Reduction of laser imprinting using polarization smoothing on a solid-state fusion laser , 1999 .

[13]  Chihiro Yamanaka,et al.  Inertial confinement fusion: The quest for ignition and energy gain using indirect drive , 1999 .

[14]  M. Rosenbluth,et al.  Temporal evolution of a three-wave parametric instability , 1973 .

[15]  Samuel A. Letzring,et al.  Improved laser‐beam uniformity using the angular dispersion of frequency‐modulated light , 1989 .

[16]  I. Kawrakow Accurate condensed history Monte Carlo simulation of electron transport. I. EGSnrc, the new EGS4 version. , 2000, Medical physics.

[17]  Samuel A. Letzring,et al.  Initial performance results of the OMEGA laser system , 1997 .

[18]  S. Skupsky,et al.  Progress in direct-drive inertial confinement fusion , 2004 .

[19]  Y. Lin,et al.  Distributed phase plates for super-Gaussian focal-plane irradiance profiles. , 1995, Optics letters.

[20]  P. B. Radha,et al.  Demonstration of the highest deuterium-tritium areal density using multiple-picket cryogenic designs on OMEGA. , 2010, Physical review letters.

[21]  Measurement of preheat due to fast electrons in laser implosions of cryogenic deuterium targets , 2005 .

[22]  D. T. Michel,et al.  Laser–plasma interactions in direct-drive ignition plasmas , 2012 .

[23]  Barukh Yaakobi,et al.  Measured hot-electron intensity thresholds quantified by a two-plasmon-decay resonant common-wave gain in various experimental configurationsa) , 2013 .

[24]  H. Baldis,et al.  Hot Electron Generation by the Two-Plasmon Decay Instability in the Laser-Plasma Interaction at 10.6 μm , 1980 .

[25]  A. Maximov,et al.  Multibeam effects on fast-electron generation from two-plasmon-decay instability. , 2003, Physical review letters.

[26]  Stefano Atzeni,et al.  The Physics of Inertial Fusion: Beam Plasma Interaction, Hydrodynamics, Hot Dense Matter , 2004 .

[27]  P. Chang,et al.  Fast-electron generation in long-scale-length plasmas , 2012 .

[28]  D. T. Michel,et al.  Saturation of the two-plasmon decay instability in long-scale-length plasmas relevant to direct-drive inertial confinement fusion. , 2012, Physical review letters.

[29]  J. Meyer-ter-Vehn,et al.  The physics of inertial fusion - Hydrodynamics, dense plasma physics, beam-plasma interaction , 2004 .