Large-scale high-resolution simulations of high gain direct-drive inertial confinement fusion targets
Phys. Plasmas 11, 2716 (2004); doi:10.1063/1.1667485
Published 23 April 2004
You are not logged in to this journal. Log in
Targets have been designed that produce moderate to high gain when directly driven by lasers. The intrinsic sensitivity of these targets to hydro instabilities is found using the FAST(2D) multidimensional radiation hydrocode [J. H. Gardner, A. J. Schmitt, J. P. Dahlburg et al., Phys. Plasmas 5, 1935 (1998)], which simulates the simultaneous behavior of a large bandwidth (e.g.,
= 2256) of perturbations from compression to acceleration, and then to stagnation and burn. The development of the structure in these multimode simulations is benchmarked to theoretical analysis and single-mode calculations, which reveals the need to "renormalize" the simulation after compression. The simulations predict that a direct drive point design is expected to degrade significantly from its one-dimensional clean yield, yet still ignite and give appreciable gain. Simulations of high-gain pellets using a spike prepulse to inhibit RichtmyerMeshkov growth show a considerable robustness, with high (>100) gains possible even with nominal surface finishes and laser imprint. ©2004 American Institute of Physics.
| History: | Received 30 October 2003; accepted 13 January 2004; published 23 April 2004 |
| Permalink: |
http://link.aip.org/link/?PHPAEN/11/2716/1 |
Supplemental Material
- IntensityNotes.NRLMemo.pdf (92 kB) 19-Apr-2001 17:5
- README.TXT (1 kB) 27-Apr-2001 18:30
KEYWORDS and PACS
- 52.57.Bc
Target design and fabrication for laser ICF - 52.50.Jm
Plasma production and heating by laser beams including laserfoil, lasercluster, etc - 52.35.Qz
Plasma microinstabilities including ion-acoustic, two-stream, loss-cone, beam-plasma, drift, ion- or electron-cyclotron instabilities, etc - 52.65.-y
Plasma simulation - 28.52.Fa
Fusion reactor materials - YEAR: 2004
RELATED DATABASES
PUBLICATION DATA
1070-664X (print)
1089-7674 (online)
REFERENCES (25)
For access to fully linked references, you need to log in.
For access to fully linked references, you need to Log in.
- J. H. Gardner, A. J. Schmitt, J. P. Dahlburg et al., Phys. Plasmas 5, 1935 (1998).
- V. N. Goncharov, Phys. Rev. Lett. 82, 2091 (1999);
- A. L. Velikovich, A. J. Schmitt, J. H. Gardner, and N. Metzler, Phys. Plasmas 8, 592 (2001);
- J. D. Lindl, Inertial Confinement Fusion (Springer-Verlag, New York, 1998).
- G. I. Bell, "Taylor instability on cylinders and spheres in small amplitude approximation," Los Alamos Scientific Laboratory Report No. LA-1321, 1951;
- R. Kishony and D. Shvarts, Phys. Plasmas 8, 4925 (2001).
- P. McKenty, V. N. Goncharov, R. P. J. Town, S. Skupsky, R. Betti, and R. L. McCrory, Phys. Plasmas 8, 2315 (2001).
- M. M. Marinak, R. E. Tipton, O. L. Landen et al., Phys. Plasmas 3, 2070 (1996).
- A. J. Schmitt, A. L. Velikovich, J. H. Gardner, S. P. Obenschain, Y. Aglitskiy, and Y. Chan, Phys. Plasmas 8, 2287 (2001).
- R. H. Lehmberg and S. P. Obenschain,
Opt. Commun. 46, 27 (1983) . - S. Skupsky, R. W. Short, T. Kessler et al., J. Appl. Phys. 66, 3456 (1989).
- See EPAPS Document No. E-PHPAEN-8-992105 for "Analysis of intensity structure of the ISI model in the FAST2D hydrocode," by A. J. Schmitt. 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. [EPAPS]
- C. P. Verdon, Bull. Am. Phys. Soc. 38, 2010 (1993);
- A. I. Nikitenko, S. M. Tolokonnikov, and R. Cook,
Fusion Technol. 31, 385 (1997) ;
R. C. Cook, R. L. McEachern, and R. B. Stephens, - It makes little difference if the initial conditions (surface perturbations) are replaced by local density perturbations that are parallel to the orthogonal mesh but give the same areal mass nonuniformity. In either case, the evolution of the mass quickly results in a sharp density gradient (the ablation surface) that is not aligned on the mesh, and thus sources for nonlinearity.
- R. Betti, V. N. Goncharov, R. L. McCrory, and C. P. Verdon, Phys. Plasmas 5, 1446 (1998).
- S. E. Bodner,
Phys. Rev. Lett. 33, 761 (1974) ;
H. Takabe, K. Mima, L. Montierth, and R. L. Morse, Phys. Fluids 28, 3676 (1985). - S. V. Weber, S. G. Glendinning, D. H. Kalantar, M. H. Key, B. A. Remington, J. E. Rothenberg, E. Wolfrum, C. P. Verdon, and J. P. Knauer, Phys. Plasmas 4, 1978 (1997).
- S. W. Haan, Phys. Rev. A 39, 5812 (1989).
- S. V. Weber, H. Dalhed, D. Eimerl et al., "Direct Drive Capsules for NIF," University of California Report No. UCRL-LR-105821-97-2, 1997.
- A. L. Velikovich, A. J. Schmitt, N. Metzler, and J. H. Gardner, Phys. Plasmas 10, 3270 (2003).
- V. N. Goncharov, J. P. Knauer, P. W. McKenty et al., Phys. Plasmas 10, 1906 (2003).
- K. Anderson and R. Betti, Phys. Plasmas 10, 4448 (2003).
- S. T. Zalesak, "The applicability of modern front-capturing methods to the modeling of small-amplitude instability growth," J. Comput. Phys. (submitted).
- S. K. Godunov, Mat. Sb. 47, 271 (1959).
R. Ishizaki and K. Nishihara, Phys. Rev. E 58, 3744 (1998).








