Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility
The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As...
Ausführliche Beschreibung
Autor*in: |
Murphy, Thomas J. [verfasserIn] Albright, B.J. [verfasserIn] Douglas, M.R. [verfasserIn] Cardenas, T. [verfasserIn] Cooley, J.H. [verfasserIn] Day, T.H. [verfasserIn] Denissen, N.A. [verfasserIn] Gore, R.A. [verfasserIn] Gunderson, M.A. [verfasserIn] Haack, J.R. [verfasserIn] Haines, B.M. [verfasserIn] Hamilton, C.E. [verfasserIn] Hartouni, E.P. [verfasserIn] Kim, Y. [verfasserIn] Kozlowski, P.M. [verfasserIn] Lee, M.N. [verfasserIn] Oertel, J.A. [verfasserIn] Olson, R.E. [verfasserIn] Randolph, R.B. [verfasserIn] Shah, R.C. [verfasserIn] Smidt, J.M. [verfasserIn] Woods, D.N. [verfasserIn] Yin, L. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2021 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: High energy density physics - Amsterdam [u.a.] : Elsevier, 2005, 38 |
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Übergeordnetes Werk: |
volume:38 |
DOI / URN: |
10.1016/j.hedp.2021.100929 |
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Katalog-ID: |
ELV005690242 |
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100 | 1 | |a Murphy, Thomas J. |e verfasserin |0 (orcid)0000-0002-6137-9873 |4 aut | |
245 | 1 | 0 | |a Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility |
264 | 1 | |c 2021 | |
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520 | |a The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. | ||
650 | 4 | |a Heterogeneous mix | |
650 | 4 | |a Thermonuclear burn | |
650 | 4 | |a BHR | |
700 | 1 | |a Albright, B.J. |e verfasserin |4 aut | |
700 | 1 | |a Douglas, M.R. |e verfasserin |4 aut | |
700 | 1 | |a Cardenas, T. |e verfasserin |0 (orcid)0000-0002-3994-4194 |4 aut | |
700 | 1 | |a Cooley, J.H. |e verfasserin |4 aut | |
700 | 1 | |a Day, T.H. |e verfasserin |0 (orcid)0000-0001-7399-9175 |4 aut | |
700 | 1 | |a Denissen, N.A. |e verfasserin |0 (orcid)0000-0003-3972-8018 |4 aut | |
700 | 1 | |a Gore, R.A. |e verfasserin |4 aut | |
700 | 1 | |a Gunderson, M.A. |e verfasserin |4 aut | |
700 | 1 | |a Haack, J.R. |e verfasserin |0 (orcid)0000-0002-2044-0885 |4 aut | |
700 | 1 | |a Haines, B.M. |e verfasserin |4 aut | |
700 | 1 | |a Hamilton, C.E. |e verfasserin |0 (orcid)0000-0002-1605-5992 |4 aut | |
700 | 1 | |a Hartouni, E.P. |e verfasserin |4 aut | |
700 | 1 | |a Kim, Y. |e verfasserin |4 aut | |
700 | 1 | |a Kozlowski, P.M. |e verfasserin |0 (orcid)0000-0001-6849-3612 |4 aut | |
700 | 1 | |a Lee, M.N. |e verfasserin |0 (orcid)0000-0002-8259-8768 |4 aut | |
700 | 1 | |a Oertel, J.A. |e verfasserin |4 aut | |
700 | 1 | |a Olson, R.E. |e verfasserin |4 aut | |
700 | 1 | |a Randolph, R.B. |e verfasserin |4 aut | |
700 | 1 | |a Shah, R.C. |e verfasserin |4 aut | |
700 | 1 | |a Smidt, J.M. |e verfasserin |4 aut | |
700 | 1 | |a Woods, D.N. |e verfasserin |4 aut | |
700 | 1 | |a Yin, L. |e verfasserin |0 (orcid)0000-0002-8978-5320 |4 aut | |
773 | 0 | 8 | |i Enthalten in |t High energy density physics |d Amsterdam [u.a.] : Elsevier, 2005 |g 38 |h Online-Ressource |w (DE-627)504859358 |w (DE-600)2213634-4 |w (DE-576)259273430 |7 nnns |
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10.1016/j.hedp.2021.100929 doi (DE-627)ELV005690242 (ELSEVIER)S1574-1818(21)00006-9 DE-627 ger DE-627 rda eng 530 DE-600 33.09 bkl 33.40 bkl 33.50 bkl 33.80 bkl 39.22 bkl Murphy, Thomas J. verfasserin (orcid)0000-0002-6137-9873 aut Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. Heterogeneous mix Thermonuclear burn BHR Albright, B.J. verfasserin aut Douglas, M.R. verfasserin aut Cardenas, T. verfasserin (orcid)0000-0002-3994-4194 aut Cooley, J.H. verfasserin aut Day, T.H. verfasserin (orcid)0000-0001-7399-9175 aut Denissen, N.A. verfasserin (orcid)0000-0003-3972-8018 aut Gore, R.A. verfasserin aut Gunderson, M.A. verfasserin aut Haack, J.R. verfasserin (orcid)0000-0002-2044-0885 aut Haines, B.M. verfasserin aut Hamilton, C.E. verfasserin (orcid)0000-0002-1605-5992 aut Hartouni, E.P. verfasserin aut Kim, Y. verfasserin aut Kozlowski, P.M. verfasserin (orcid)0000-0001-6849-3612 aut Lee, M.N. verfasserin (orcid)0000-0002-8259-8768 aut Oertel, J.A. verfasserin aut Olson, R.E. verfasserin aut Randolph, R.B. verfasserin aut Shah, R.C. verfasserin aut Smidt, J.M. verfasserin aut Woods, D.N. verfasserin aut Yin, L. verfasserin (orcid)0000-0002-8978-5320 aut Enthalten in High energy density physics Amsterdam [u.a.] : Elsevier, 2005 38 Online-Ressource (DE-627)504859358 (DE-600)2213634-4 (DE-576)259273430 nnns volume:38 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.09 Physik unter besonderen Bedingungen 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.80 Plasmaphysik 39.22 Astrophysik AR 38 |
spelling |
10.1016/j.hedp.2021.100929 doi (DE-627)ELV005690242 (ELSEVIER)S1574-1818(21)00006-9 DE-627 ger DE-627 rda eng 530 DE-600 33.09 bkl 33.40 bkl 33.50 bkl 33.80 bkl 39.22 bkl Murphy, Thomas J. verfasserin (orcid)0000-0002-6137-9873 aut Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. Heterogeneous mix Thermonuclear burn BHR Albright, B.J. verfasserin aut Douglas, M.R. verfasserin aut Cardenas, T. verfasserin (orcid)0000-0002-3994-4194 aut Cooley, J.H. verfasserin aut Day, T.H. verfasserin (orcid)0000-0001-7399-9175 aut Denissen, N.A. verfasserin (orcid)0000-0003-3972-8018 aut Gore, R.A. verfasserin aut Gunderson, M.A. verfasserin aut Haack, J.R. verfasserin (orcid)0000-0002-2044-0885 aut Haines, B.M. verfasserin aut Hamilton, C.E. verfasserin (orcid)0000-0002-1605-5992 aut Hartouni, E.P. verfasserin aut Kim, Y. verfasserin aut Kozlowski, P.M. verfasserin (orcid)0000-0001-6849-3612 aut Lee, M.N. verfasserin (orcid)0000-0002-8259-8768 aut Oertel, J.A. verfasserin aut Olson, R.E. verfasserin aut Randolph, R.B. verfasserin aut Shah, R.C. verfasserin aut Smidt, J.M. verfasserin aut Woods, D.N. verfasserin aut Yin, L. verfasserin (orcid)0000-0002-8978-5320 aut Enthalten in High energy density physics Amsterdam [u.a.] : Elsevier, 2005 38 Online-Ressource (DE-627)504859358 (DE-600)2213634-4 (DE-576)259273430 nnns volume:38 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.09 Physik unter besonderen Bedingungen 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.80 Plasmaphysik 39.22 Astrophysik AR 38 |
allfields_unstemmed |
10.1016/j.hedp.2021.100929 doi (DE-627)ELV005690242 (ELSEVIER)S1574-1818(21)00006-9 DE-627 ger DE-627 rda eng 530 DE-600 33.09 bkl 33.40 bkl 33.50 bkl 33.80 bkl 39.22 bkl Murphy, Thomas J. verfasserin (orcid)0000-0002-6137-9873 aut Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. Heterogeneous mix Thermonuclear burn BHR Albright, B.J. verfasserin aut Douglas, M.R. verfasserin aut Cardenas, T. verfasserin (orcid)0000-0002-3994-4194 aut Cooley, J.H. verfasserin aut Day, T.H. verfasserin (orcid)0000-0001-7399-9175 aut Denissen, N.A. verfasserin (orcid)0000-0003-3972-8018 aut Gore, R.A. verfasserin aut Gunderson, M.A. verfasserin aut Haack, J.R. verfasserin (orcid)0000-0002-2044-0885 aut Haines, B.M. verfasserin aut Hamilton, C.E. verfasserin (orcid)0000-0002-1605-5992 aut Hartouni, E.P. verfasserin aut Kim, Y. verfasserin aut Kozlowski, P.M. verfasserin (orcid)0000-0001-6849-3612 aut Lee, M.N. verfasserin (orcid)0000-0002-8259-8768 aut Oertel, J.A. verfasserin aut Olson, R.E. verfasserin aut Randolph, R.B. verfasserin aut Shah, R.C. verfasserin aut Smidt, J.M. verfasserin aut Woods, D.N. verfasserin aut Yin, L. verfasserin (orcid)0000-0002-8978-5320 aut Enthalten in High energy density physics Amsterdam [u.a.] : Elsevier, 2005 38 Online-Ressource (DE-627)504859358 (DE-600)2213634-4 (DE-576)259273430 nnns volume:38 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.09 Physik unter besonderen Bedingungen 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.80 Plasmaphysik 39.22 Astrophysik AR 38 |
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10.1016/j.hedp.2021.100929 doi (DE-627)ELV005690242 (ELSEVIER)S1574-1818(21)00006-9 DE-627 ger DE-627 rda eng 530 DE-600 33.09 bkl 33.40 bkl 33.50 bkl 33.80 bkl 39.22 bkl Murphy, Thomas J. verfasserin (orcid)0000-0002-6137-9873 aut Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. Heterogeneous mix Thermonuclear burn BHR Albright, B.J. verfasserin aut Douglas, M.R. verfasserin aut Cardenas, T. verfasserin (orcid)0000-0002-3994-4194 aut Cooley, J.H. verfasserin aut Day, T.H. verfasserin (orcid)0000-0001-7399-9175 aut Denissen, N.A. verfasserin (orcid)0000-0003-3972-8018 aut Gore, R.A. verfasserin aut Gunderson, M.A. verfasserin aut Haack, J.R. verfasserin (orcid)0000-0002-2044-0885 aut Haines, B.M. verfasserin aut Hamilton, C.E. verfasserin (orcid)0000-0002-1605-5992 aut Hartouni, E.P. verfasserin aut Kim, Y. verfasserin aut Kozlowski, P.M. verfasserin (orcid)0000-0001-6849-3612 aut Lee, M.N. verfasserin (orcid)0000-0002-8259-8768 aut Oertel, J.A. verfasserin aut Olson, R.E. verfasserin aut Randolph, R.B. verfasserin aut Shah, R.C. verfasserin aut Smidt, J.M. verfasserin aut Woods, D.N. verfasserin aut Yin, L. verfasserin (orcid)0000-0002-8978-5320 aut Enthalten in High energy density physics Amsterdam [u.a.] : Elsevier, 2005 38 Online-Ressource (DE-627)504859358 (DE-600)2213634-4 (DE-576)259273430 nnns volume:38 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.09 Physik unter besonderen Bedingungen 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.80 Plasmaphysik 39.22 Astrophysik AR 38 |
allfieldsSound |
10.1016/j.hedp.2021.100929 doi (DE-627)ELV005690242 (ELSEVIER)S1574-1818(21)00006-9 DE-627 ger DE-627 rda eng 530 DE-600 33.09 bkl 33.40 bkl 33.50 bkl 33.80 bkl 39.22 bkl Murphy, Thomas J. verfasserin (orcid)0000-0002-6137-9873 aut Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. Heterogeneous mix Thermonuclear burn BHR Albright, B.J. verfasserin aut Douglas, M.R. verfasserin aut Cardenas, T. verfasserin (orcid)0000-0002-3994-4194 aut Cooley, J.H. verfasserin aut Day, T.H. verfasserin (orcid)0000-0001-7399-9175 aut Denissen, N.A. verfasserin (orcid)0000-0003-3972-8018 aut Gore, R.A. verfasserin aut Gunderson, M.A. verfasserin aut Haack, J.R. verfasserin (orcid)0000-0002-2044-0885 aut Haines, B.M. verfasserin aut Hamilton, C.E. verfasserin (orcid)0000-0002-1605-5992 aut Hartouni, E.P. verfasserin aut Kim, Y. verfasserin aut Kozlowski, P.M. verfasserin (orcid)0000-0001-6849-3612 aut Lee, M.N. verfasserin (orcid)0000-0002-8259-8768 aut Oertel, J.A. verfasserin aut Olson, R.E. verfasserin aut Randolph, R.B. verfasserin aut Shah, R.C. verfasserin aut Smidt, J.M. verfasserin aut Woods, D.N. verfasserin aut Yin, L. verfasserin (orcid)0000-0002-8978-5320 aut Enthalten in High energy density physics Amsterdam [u.a.] : Elsevier, 2005 38 Online-Ressource (DE-627)504859358 (DE-600)2213634-4 (DE-576)259273430 nnns volume:38 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.09 Physik unter besonderen Bedingungen 33.40 Kernphysik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.80 Plasmaphysik 39.22 Astrophysik AR 38 |
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Murphy, Thomas J. @@aut@@ Albright, B.J. @@aut@@ Douglas, M.R. @@aut@@ Cardenas, T. @@aut@@ Cooley, J.H. @@aut@@ Day, T.H. @@aut@@ Denissen, N.A. @@aut@@ Gore, R.A. @@aut@@ Gunderson, M.A. @@aut@@ Haack, J.R. @@aut@@ Haines, B.M. @@aut@@ Hamilton, C.E. @@aut@@ Hartouni, E.P. @@aut@@ Kim, Y. @@aut@@ Kozlowski, P.M. @@aut@@ Lee, M.N. @@aut@@ Oertel, J.A. @@aut@@ Olson, R.E. @@aut@@ Randolph, R.B. @@aut@@ Shah, R.C. @@aut@@ Smidt, J.M. @@aut@@ Woods, D.N. @@aut@@ Yin, L. @@aut@@ |
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Murphy, Thomas J. |
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Murphy, Thomas J. ddc 530 bkl 33.09 bkl 33.40 bkl 33.50 bkl 33.80 bkl 39.22 misc Heterogeneous mix misc Thermonuclear burn misc BHR Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility |
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530 DE-600 33.09 bkl 33.40 bkl 33.50 bkl 33.80 bkl 39.22 bkl Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility Heterogeneous mix Thermonuclear burn BHR |
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results from single-shock marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the national ignition facility |
title_auth |
Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility |
abstract |
The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. |
abstractGer |
The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. |
abstract_unstemmed |
The Marble campaign on the National Ignition Facility investigates the effect of heterogeneous mix on thermonuclear burn for comparison to a probability distribution function (PDF) burn model. Marble utilizes plastic capsules filled with deuterated plastic foam and a fill gas containing tritium. As the capsules implode, the deuterium in the foam mixes with the tritium gas, and DT neutrons are produced as the shocks compress and heat the mixture. The yield of DT neutrons is dependent on the uniformity of the mix, with more heterogeneous mix producing fewer neutrons. In Marble, the heterogeneity of the mix is controlled by varying the diameter of voids introduced into the foam. The first NIF Marble campaign has been executed in which the Marble capsules were indirectly driven with a single strong shock using NIF hohlraums. The experiments produce a low-convergence, high-ion-temperature implosion. The ratio of DT to DD neutron yield is largely consistent with uniform atomic mix for fine-pore foam, and increases slightly with void diameter, contrary to 1D simulations using the PDF burn model. Recent 3D high-resolution simulations of similar experiments performed on the Omega Laser Facility suggest an explanation. |
collection_details |
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title_short |
Results from single-shock Marble experiments studying thermonuclear burn in the presence of heterogeneous mix on the National Ignition Facility |
remote_bool |
true |
author2 |
Albright, B.J. Douglas, M.R. Cardenas, T. Cooley, J.H. Day, T.H. Denissen, N.A. Gore, R.A. Gunderson, M.A. Haack, J.R. Haines, B.M. Hamilton, C.E. Hartouni, E.P. Kim, Y. Kozlowski, P.M. Lee, M.N. Oertel, J.A. Olson, R.E. Randolph, R.B. Shah, R.C. Smidt, J.M. Woods, D.N. Yin, L. |
author2Str |
Albright, B.J. Douglas, M.R. Cardenas, T. Cooley, J.H. Day, T.H. Denissen, N.A. Gore, R.A. Gunderson, M.A. Haack, J.R. Haines, B.M. Hamilton, C.E. Hartouni, E.P. Kim, Y. Kozlowski, P.M. Lee, M.N. Oertel, J.A. Olson, R.E. Randolph, R.B. Shah, R.C. Smidt, J.M. Woods, D.N. Yin, L. |
ppnlink |
504859358 |
mediatype_str_mv |
c |
isOA_txt |
false |
hochschulschrift_bool |
false |
doi_str |
10.1016/j.hedp.2021.100929 |
up_date |
2024-07-06T18:49:40.984Z |
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1803856674539175936 |
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|
score |
7.397663 |