Polarization beam smoothing for inertial confinement fusion

For both direct and indirect drive approaches to inertial confinement fusion (ICF) it is imperative to obtain the best possible drive beam uniformity. The approach chosen for the National Ignition Facility uses a random-phase plate to generate a speckle pattern with a precisely controlled envelope on target. A number of temporal smoothing techniques can then be employed to utilize bandwidth to rapidly change the speckle pattern, and thus average out the small-scale speckle structure. One technique which generally can supplement other smoothing methods is polarization smoothing (PS): the illumination of the target with two distinct and orthogonally polarized speckle patterns. Since these two polarizations do not interfere, the intensity patterns add incoherently, and the rms nonuniformity can be reduced by a factor of √. A number of PS schemes are described and compared on the basis of the aggregate rms and the spatial spectrum of the focused illumination distribution. The √ rms nonuniformity reduction of ...

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

[2]  J. D. Moody,et al.  Laser–plasma interactions in ignition‐scale hohlraum plasmas , 1996 .

[3]  Joshua E. Rothenberg,et al.  Two-dimensional beam smoothing by spectral dispersion for direct-drive inertial confinement fusion , 1995, Other Conferences.

[4]  Koji Tsubakimoto,et al.  Suppression of interference speckles produced by a random phase plate, using a polarization control plate , 1992 .

[5]  S. P. Obenschain,et al.  Use of induced spatial incoherence for uniform illumination on laser fusion targets. Memorandum report , 1983 .

[6]  Joshua E. Rothenberg,et al.  Reduction of laser self-focusing in plasma by polarization smoothing , 1998 .

[7]  Koji Tsubakimoto,et al.  Suppression of speckle contrast by using polarization property on second harmonic generation , 1993 .

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

[9]  D. E. Gray,et al.  American Institute of Physics Handbook , 1957 .

[10]  M. Rostaing,et al.  Optical spatial smoothing of Nd-Glass laser beam , 1988 .

[11]  John Lindl,et al.  Hydrodynamic stability and the direct drive approach to laser fusion , 1990 .

[12]  Emil Wolf,et al.  Principles of Optics: Contents , 1999 .

[13]  S. Skupsky,et al.  Irradiation uniformity for high-compression laser-fusion experiments , 1999 .

[14]  S. N. Dixit,et al.  Electro-optic control of correlations in speckle statistics , 1994 .

[15]  Joshua E. Rothenberg,et al.  Comparison of beam-smoothing methods for direct-drive inertial confinement fusion , 1997 .

[16]  Koji Tsubakimoto,et al.  Partially coherent light generated by using single and multimode optical fibers in a high‐power Nd:glass laser system , 1993 .

[17]  Kunioki Mima,et al.  Random Phasing of High-Power Lasers for Uniform Target Acceleration and Plasma-Instability Suppression , 1984 .