Core performance and mix in direct-drive spherical implosions with high uniformity
The performance of gas-filled, plastic-shell implosions has significantly improved with advances in on-target uniformity on the 60-beam OMEGA laser system [T. R. Boehly, D. L. Brown, R. S. Craxton et al., Opt. Commun. 133, 495 (1997)]. Polarization smoothing (PS) with birefringent wedges and 1-THz-b...
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creator | Meyerhofer, D. D. Delettrez, J. A. Epstein, R. Glebov, V. Yu Goncharov, V. N. Keck, R. L. McCrory, R. L. McKenty, P. W. Marshall, F. J. Radha, P. B. Regan, S. P. Roberts, S. Seka, W. Skupsky, S. Smalyuk, V. A. Sorce, C. Stoeckl, C. Soures, J. M. Town, R. P. J. Yaakobi, B. Zuegel, J. D. Frenje, J. Li, C. K. Petrasso, R. D. Séguin, F. H. Fletcher, K. Padalino, S. Freeman, C. Izumi, N. Lerche, R. Phillips, T. W. Sangster, T. C. |
description | The performance of gas-filled, plastic-shell implosions has significantly improved with advances in on-target uniformity on the 60-beam OMEGA laser system [T. R. Boehly, D. L. Brown, R. S. Craxton et al., Opt. Commun. 133, 495 (1997)]. Polarization smoothing (PS) with birefringent wedges and 1-THz-bandwidth smoothing by spectral dispersion (SSD) have been installed on OMEGA. The beam-to-beam power imbalance is
⩽5%
rms. Implosions of 20-μm-thick CH shells (15 atm fill) using full beam smoothing (1-THz SSD and PS) have primary neutron yields and fuel areal densities that are
∼70%
larger than those driven with 0.35-THz SSD without PS. They also produce
∼35%
of the predicted one-dimensional neutron yield. The results described here suggest that individual-beam nonuniformity is no longer the primary cause of nonideal target performance. A highly constrained model of the core conditions and fuel–shell mix has been developed. It suggests that there is a “clean” fuel region, surrounded by a mixed region, that accounts for half of the fuel areal density. |
doi_str_mv | 10.1063/1.1350964 |
format | Article |
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⩽5%
rms. Implosions of 20-μm-thick CH shells (15 atm fill) using full beam smoothing (1-THz SSD and PS) have primary neutron yields and fuel areal densities that are
∼70%
larger than those driven with 0.35-THz SSD without PS. They also produce
∼35%
of the predicted one-dimensional neutron yield. The results described here suggest that individual-beam nonuniformity is no longer the primary cause of nonideal target performance. A highly constrained model of the core conditions and fuel–shell mix has been developed. It suggests that there is a “clean” fuel region, surrounded by a mixed region, that accounts for half of the fuel areal density.</description><identifier>ISSN: 1070-664X</identifier><identifier>EISSN: 1089-7674</identifier><identifier>DOI: 10.1063/1.1350964</identifier><identifier>CODEN: PHPAEN</identifier><language>eng</language><ispartof>Physics of Plasmas, 2001-05, Vol.8 (5), p.2251-2256</ispartof><rights>American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c297t-43ce04c7c60987c0b36cb76c979b33ed62f2801421422d653d1ad4602090bfdf3</citedby><cites>FETCH-LOGICAL-c297t-43ce04c7c60987c0b36cb76c979b33ed62f2801421422d653d1ad4602090bfdf3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/pop/article-lookup/doi/10.1063/1.1350964$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>309,310,314,778,782,787,788,792,1556,4500,23919,23920,25129,27913,27914,76143,76149</link.rule.ids></links><search><creatorcontrib>Meyerhofer, D. D.</creatorcontrib><creatorcontrib>Delettrez, J. A.</creatorcontrib><creatorcontrib>Epstein, R.</creatorcontrib><creatorcontrib>Glebov, V. Yu</creatorcontrib><creatorcontrib>Goncharov, V. N.</creatorcontrib><creatorcontrib>Keck, R. L.</creatorcontrib><creatorcontrib>McCrory, R. L.</creatorcontrib><creatorcontrib>McKenty, P. W.</creatorcontrib><creatorcontrib>Marshall, F. J.</creatorcontrib><creatorcontrib>Radha, P. B.</creatorcontrib><creatorcontrib>Regan, S. P.</creatorcontrib><creatorcontrib>Roberts, S.</creatorcontrib><creatorcontrib>Seka, W.</creatorcontrib><creatorcontrib>Skupsky, S.</creatorcontrib><creatorcontrib>Smalyuk, V. A.</creatorcontrib><creatorcontrib>Sorce, C.</creatorcontrib><creatorcontrib>Stoeckl, C.</creatorcontrib><creatorcontrib>Soures, J. M.</creatorcontrib><creatorcontrib>Town, R. P. J.</creatorcontrib><creatorcontrib>Yaakobi, B.</creatorcontrib><creatorcontrib>Zuegel, J. D.</creatorcontrib><creatorcontrib>Frenje, J.</creatorcontrib><creatorcontrib>Li, C. K.</creatorcontrib><creatorcontrib>Petrasso, R. D.</creatorcontrib><creatorcontrib>Séguin, F. H.</creatorcontrib><creatorcontrib>Fletcher, K.</creatorcontrib><creatorcontrib>Padalino, S.</creatorcontrib><creatorcontrib>Freeman, C.</creatorcontrib><creatorcontrib>Izumi, N.</creatorcontrib><creatorcontrib>Lerche, R.</creatorcontrib><creatorcontrib>Phillips, T. W.</creatorcontrib><creatorcontrib>Sangster, T. C.</creatorcontrib><title>Core performance and mix in direct-drive spherical implosions with high uniformity</title><title>Physics of Plasmas</title><description>The performance of gas-filled, plastic-shell implosions has significantly improved with advances in on-target uniformity on the 60-beam OMEGA laser system [T. R. Boehly, D. L. Brown, R. S. Craxton et al., Opt. Commun. 133, 495 (1997)]. Polarization smoothing (PS) with birefringent wedges and 1-THz-bandwidth smoothing by spectral dispersion (SSD) have been installed on OMEGA. The beam-to-beam power imbalance is
⩽5%
rms. Implosions of 20-μm-thick CH shells (15 atm fill) using full beam smoothing (1-THz SSD and PS) have primary neutron yields and fuel areal densities that are
∼70%
larger than those driven with 0.35-THz SSD without PS. They also produce
∼35%
of the predicted one-dimensional neutron yield. The results described here suggest that individual-beam nonuniformity is no longer the primary cause of nonideal target performance. A highly constrained model of the core conditions and fuel–shell mix has been developed. 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D.</au><au>Frenje, J.</au><au>Li, C. K.</au><au>Petrasso, R. D.</au><au>Séguin, F. H.</au><au>Fletcher, K.</au><au>Padalino, S.</au><au>Freeman, C.</au><au>Izumi, N.</au><au>Lerche, R.</au><au>Phillips, T. W.</au><au>Sangster, T. C.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Core performance and mix in direct-drive spherical implosions with high uniformity</atitle><jtitle>Physics of Plasmas</jtitle><date>2001-05</date><risdate>2001</risdate><volume>8</volume><issue>5</issue><spage>2251</spage><epage>2256</epage><pages>2251-2256</pages><issn>1070-664X</issn><eissn>1089-7674</eissn><coden>PHPAEN</coden><abstract>The performance of gas-filled, plastic-shell implosions has significantly improved with advances in on-target uniformity on the 60-beam OMEGA laser system [T. R. Boehly, D. L. Brown, R. S. Craxton et al., Opt. Commun. 133, 495 (1997)]. Polarization smoothing (PS) with birefringent wedges and 1-THz-bandwidth smoothing by spectral dispersion (SSD) have been installed on OMEGA. The beam-to-beam power imbalance is
⩽5%
rms. Implosions of 20-μm-thick CH shells (15 atm fill) using full beam smoothing (1-THz SSD and PS) have primary neutron yields and fuel areal densities that are
∼70%
larger than those driven with 0.35-THz SSD without PS. They also produce
∼35%
of the predicted one-dimensional neutron yield. The results described here suggest that individual-beam nonuniformity is no longer the primary cause of nonideal target performance. A highly constrained model of the core conditions and fuel–shell mix has been developed. It suggests that there is a “clean” fuel region, surrounded by a mixed region, that accounts for half of the fuel areal density.</abstract><doi>10.1063/1.1350964</doi><tpages>6</tpages></addata></record> |
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title | Core performance and mix in direct-drive spherical implosions with high uniformity |
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