The impact of low-mode symmetry on inertial fusion energy output in the burning plasma state
Abstract Indirect Drive Inertial Confinement Fusion Experiments on the National Ignition Facility (NIF) have achieved a burning plasma state with neutron yields exceeding 170 kJ, roughly 3 times the prior record and a necessary stage for igniting plasmas. The results are achieved despite multiple so...
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| Format: | Article |
| Language: | English |
| Published: |
Nature Portfolio
2024-04-01
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| Series: | Nature Communications |
| Online Access: | https://doi.org/10.1038/s41467-024-47302-8 |
| _version_ | 1797219716157145088 |
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| author | J. E. Ralph J. S. Ross A. B. Zylstra A. L. Kritcher H. F. Robey C. V. Young O. A. Hurricane A. Pak D. A. Callahan K. L. Baker D. T. Casey T. Döppner L. Divol M. Hohenberger S. Le Pape P. K. Patel R. Tommasini S. J. Ali P. A. Amendt L. J. Atherton B. Bachmann D. Bailey L. R. Benedetti L. Berzak Hopkins R. Betti S. D. Bhandarkar J. Biener R. M. Bionta N. W. Birge E. J. Bond D. K. Bradley T. Braun T. M. Briggs M. W. Bruhn P. M. Celliers B. Chang T. Chapman H. Chen C. Choate A. R. Christopherson D. S. Clark J. W. Crippen E. L. Dewald T. R. Dittrich M. J. Edwards W. A. Farmer J. E. Field D. Fittinghoff J. Frenje J. Gaffney M. Gatu Johnson S. H. Glenzer G. P. Grim S. Haan K. D. Hahn G. N. Hall B. A. Hammel J. Harte E. Hartouni J. E. Heebner V. J. Hernandez H. W. Herrmann M. C. Herrmann D. E. Hinkel D. D. Ho J. P. Holder W. W. Hsing H. Huang K. D. Humbird N. Izumi L. C. Jarrott J. Jeet O. Jones G. D. Kerbel S. M. Kerr S. F. Khan J. Kilkenny Y. Kim H. Geppert-Kleinrath V. Geppert-Kleinrath C. Kong J. M. Koning J. J. Kroll M. K. G. Kruse B. Kustowski O. L. Landen S. Langer D. Larson N. C. Lemos J. D. Lindl T. Ma M. J. MacDonald B. J. MacGowan A. J. Mackinnon S. A. MacLaren A. G. MacPhee M. M. Marinak D. A. Mariscal E. V. Marley L. Masse K. D. Meaney N. B. Meezan P. A. Michel M. Millot J. L. Milovich J. D. Moody A. S. Moore J. W. Morton T. J. Murphy K. Newman J.-M. G. Di Nicola A. Nikroo R. Nora M. V. Patel L. J. Pelz J. L. Peterson Y. Ping B. B. Pollock M. Ratledge N. G. Rice H. G. Rinderknecht M. Rosen M. S. Rubery J. D. Salmonson J. Sater S. Schiaffino D. J. Schlossberg M. B. Schneider C. R. Schroeder H. A. Scott S. M. Sepke K. Sequoia M. W. Sherlock S. Shin V. A. Smalyuk B. K. Spears P. T. Springer M. Stadermann S. Stoupin D. J. Strozzi L. J. Suter C. A. Thomas R. P. J. Town C. Trosseille E. R. Tubman P. L. Volegov C. R. Weber K. Widmann C. Wild C. H. Wilde B. M. Van Wonterghem D. T. Woods B. N. Woodworth M. Yamaguchi S. T. Yang G. B. Zimmerman |
| author_facet | J. E. Ralph J. S. Ross A. B. Zylstra A. L. Kritcher H. F. Robey C. V. Young O. A. Hurricane A. Pak D. A. Callahan K. L. Baker D. T. Casey T. Döppner L. Divol M. Hohenberger S. Le Pape P. K. Patel R. Tommasini S. J. Ali P. A. Amendt L. J. Atherton B. Bachmann D. Bailey L. R. Benedetti L. Berzak Hopkins R. Betti S. D. Bhandarkar J. Biener R. M. Bionta N. W. Birge E. J. Bond D. K. Bradley T. Braun T. M. Briggs M. W. Bruhn P. M. Celliers B. Chang T. Chapman H. Chen C. Choate A. R. Christopherson D. S. Clark J. W. Crippen E. L. Dewald T. R. Dittrich M. J. Edwards W. A. Farmer J. E. Field D. Fittinghoff J. Frenje J. Gaffney M. Gatu Johnson S. H. Glenzer G. P. Grim S. Haan K. D. Hahn G. N. Hall B. A. Hammel J. Harte E. Hartouni J. E. Heebner V. J. Hernandez H. W. Herrmann M. C. Herrmann D. E. Hinkel D. D. Ho J. P. Holder W. W. Hsing H. Huang K. D. Humbird N. Izumi L. C. Jarrott J. Jeet O. Jones G. D. Kerbel S. M. Kerr S. F. Khan J. Kilkenny Y. Kim H. Geppert-Kleinrath V. Geppert-Kleinrath C. Kong J. M. Koning J. J. Kroll M. K. G. Kruse B. Kustowski O. L. Landen S. Langer D. Larson N. C. Lemos J. D. Lindl T. Ma M. J. MacDonald B. J. MacGowan A. J. Mackinnon S. A. MacLaren A. G. MacPhee M. M. Marinak D. A. Mariscal E. V. Marley L. Masse K. D. Meaney N. B. Meezan P. A. Michel M. Millot J. L. Milovich J. D. Moody A. S. Moore J. W. Morton T. J. Murphy K. Newman J.-M. G. Di Nicola A. Nikroo R. Nora M. V. Patel L. J. Pelz J. L. Peterson Y. Ping B. B. Pollock M. Ratledge N. G. Rice H. G. Rinderknecht M. Rosen M. S. Rubery J. D. Salmonson J. Sater S. Schiaffino D. J. Schlossberg M. B. Schneider C. R. Schroeder H. A. Scott S. M. Sepke K. Sequoia M. W. Sherlock S. Shin V. A. Smalyuk B. K. Spears P. T. Springer M. Stadermann S. Stoupin D. J. Strozzi L. J. Suter C. A. Thomas R. P. J. Town C. Trosseille E. R. Tubman P. L. Volegov C. R. Weber K. Widmann C. Wild C. H. Wilde B. M. Van Wonterghem D. T. Woods B. N. Woodworth M. Yamaguchi S. T. Yang G. B. Zimmerman |
| author_sort | J. E. Ralph |
| collection | DOAJ |
| description | Abstract Indirect Drive Inertial Confinement Fusion Experiments on the National Ignition Facility (NIF) have achieved a burning plasma state with neutron yields exceeding 170 kJ, roughly 3 times the prior record and a necessary stage for igniting plasmas. The results are achieved despite multiple sources of degradations that lead to high variability in performance. Results shown here, for the first time, include an empirical correction factor for mode-2 asymmetry in the burning plasma regime in addition to previously determined corrections for radiative mix and mode-1. Analysis shows that including these three corrections alone accounts for the measured fusion performance variability in the two highest performing experimental campaigns on the NIF to within error. Here we quantify the performance sensitivity to mode-2 symmetry in the burning plasma regime and apply the results, in the form of an empirical correction to a 1D performance model. Furthermore, we find the sensitivity to mode-2 determined through a series of integrated 2D radiation hydrodynamic simulations to be consistent with the experimentally determined sensitivity only when including alpha-heating. |
| first_indexed | 2024-04-24T12:38:04Z |
| format | Article |
| id | doaj.art-269b30b0fbbf4e519e1e759f9f698844 |
| institution | Directory Open Access Journal |
| issn | 2041-1723 |
| language | English |
| last_indexed | 2024-04-24T12:38:04Z |
| publishDate | 2024-04-01 |
| publisher | Nature Portfolio |
| record_format | Article |
| series | Nature Communications |
| spelling | doaj.art-269b30b0fbbf4e519e1e759f9f6988442024-04-07T11:23:49ZengNature PortfolioNature Communications2041-17232024-04-0115111410.1038/s41467-024-47302-8The impact of low-mode symmetry on inertial fusion energy output in the burning plasma stateJ. E. Ralph0J. S. Ross1A. B. Zylstra2A. L. Kritcher3H. F. Robey4C. V. Young5O. A. Hurricane6A. Pak7D. A. Callahan8K. L. Baker9D. T. Casey10T. Döppner11L. Divol12M. Hohenberger13S. Le Pape14P. K. Patel15R. Tommasini16S. J. Ali17P. A. Amendt18L. J. Atherton19B. Bachmann20D. Bailey21L. R. Benedetti22L. Berzak Hopkins23R. Betti24S. D. Bhandarkar25J. Biener26R. M. Bionta27N. W. Birge28E. J. Bond29D. K. Bradley30T. Braun31T. M. Briggs32M. W. Bruhn33P. M. Celliers34B. Chang35T. Chapman36H. Chen37C. Choate38A. R. Christopherson39D. S. Clark40J. W. Crippen41E. L. Dewald42T. R. Dittrich43M. J. Edwards44W. A. Farmer45J. E. Field46D. Fittinghoff47J. Frenje48J. Gaffney49M. Gatu Johnson50S. H. Glenzer51G. P. Grim52S. Haan53K. D. Hahn54G. N. Hall55B. A. Hammel56J. Harte57E. Hartouni58J. E. Heebner59V. J. Hernandez60H. W. Herrmann61M. C. Herrmann62D. E. Hinkel63D. D. Ho64J. P. Holder65W. W. Hsing66H. Huang67K. D. Humbird68N. Izumi69L. C. Jarrott70J. Jeet71O. Jones72G. D. Kerbel73S. M. Kerr74S. F. Khan75J. Kilkenny76Y. Kim77H. Geppert-Kleinrath78V. Geppert-Kleinrath79C. Kong80J. M. Koning81J. J. Kroll82M. K. G. Kruse83B. Kustowski84O. L. Landen85S. Langer86D. Larson87N. C. Lemos88J. D. Lindl89T. Ma90M. J. MacDonald91B. J. MacGowan92A. J. Mackinnon93S. A. MacLaren94A. G. MacPhee95M. M. Marinak96D. A. Mariscal97E. V. Marley98L. Masse99K. D. Meaney100N. B. Meezan101P. A. Michel102M. Millot103J. L. Milovich104J. D. Moody105A. S. Moore106J. W. Morton107T. J. Murphy108K. Newman109J.-M. G. Di Nicola110A. Nikroo111R. Nora112M. V. Patel113L. J. Pelz114J. L. Peterson115Y. Ping116B. B. Pollock117M. Ratledge118N. G. Rice119H. G. Rinderknecht120M. Rosen121M. S. Rubery122J. D. Salmonson123J. Sater124S. Schiaffino125D. J. Schlossberg126M. B. Schneider127C. R. Schroeder128H. A. Scott129S. M. Sepke130K. Sequoia131M. W. Sherlock132S. Shin133V. A. Smalyuk134B. K. Spears135P. T. Springer136M. Stadermann137S. Stoupin138D. J. Strozzi139L. J. Suter140C. A. Thomas141R. P. J. Town142C. Trosseille143E. R. Tubman144P. L. Volegov145C. R. Weber146K. Widmann147C. Wild148C. H. Wilde149B. M. Van Wonterghem150D. T. Woods151B. N. Woodworth152M. Yamaguchi153S. T. Yang154G. B. Zimmerman155Lawrence Livermore National LaboratoryLawrence Livermore National LaboratoryPacific FusionLawrence Livermore National LaboratoryLos Alamos National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryFocused EnergyLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLaboratoire pour l’utilisation des Lasers Intenses chez École PolytechniqueLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLaboratory for Laser Energetics, University of RochesterLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLos Alamos National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryGeneral AtomicsLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryMassachusetts Institute of TechnologyLawrence Livermore National LaboratoryMassachusetts Institute of TechnologySLAC National Accelerator LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLos Alamos National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryGeneral AtomicsLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryGeneral AtomicsLos Alamos National LaboratoryLos Alamos National LaboratoryLos Alamos National LaboratoryGeneral AtomicsLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLos Alamos National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryAtomic Weapons EstablishmentLos Alamos National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryGeneral AtomicsGeneral AtomicsLaboratory for Laser Energetics, University of RochesterLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryGeneral AtomicsLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLaboratory for Laser Energetics, University of RochesterLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLos Alamos National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryDiamond Materials GmbhPacific FusionLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryGeneral AtomicsLawrence Livermore National LaboratoryLawrence Livermore National LaboratoryAbstract Indirect Drive Inertial Confinement Fusion Experiments on the National Ignition Facility (NIF) have achieved a burning plasma state with neutron yields exceeding 170 kJ, roughly 3 times the prior record and a necessary stage for igniting plasmas. The results are achieved despite multiple sources of degradations that lead to high variability in performance. Results shown here, for the first time, include an empirical correction factor for mode-2 asymmetry in the burning plasma regime in addition to previously determined corrections for radiative mix and mode-1. Analysis shows that including these three corrections alone accounts for the measured fusion performance variability in the two highest performing experimental campaigns on the NIF to within error. Here we quantify the performance sensitivity to mode-2 symmetry in the burning plasma regime and apply the results, in the form of an empirical correction to a 1D performance model. Furthermore, we find the sensitivity to mode-2 determined through a series of integrated 2D radiation hydrodynamic simulations to be consistent with the experimentally determined sensitivity only when including alpha-heating.https://doi.org/10.1038/s41467-024-47302-8 |
| spellingShingle | J. E. Ralph J. S. Ross A. B. Zylstra A. L. Kritcher H. F. Robey C. V. Young O. A. Hurricane A. Pak D. A. Callahan K. L. Baker D. T. Casey T. Döppner L. Divol M. Hohenberger S. Le Pape P. K. Patel R. Tommasini S. J. Ali P. A. Amendt L. J. Atherton B. Bachmann D. Bailey L. R. Benedetti L. Berzak Hopkins R. Betti S. D. Bhandarkar J. Biener R. M. Bionta N. W. Birge E. J. Bond D. K. Bradley T. Braun T. M. Briggs M. W. Bruhn P. M. Celliers B. Chang T. Chapman H. Chen C. Choate A. R. Christopherson D. S. Clark J. W. Crippen E. L. Dewald T. R. Dittrich M. J. Edwards W. A. Farmer J. E. Field D. Fittinghoff J. Frenje J. Gaffney M. Gatu Johnson S. H. Glenzer G. P. Grim S. Haan K. D. Hahn G. N. Hall B. A. Hammel J. Harte E. Hartouni J. E. Heebner V. J. Hernandez H. W. Herrmann M. C. Herrmann D. E. Hinkel D. D. Ho J. P. Holder W. W. Hsing H. Huang K. D. Humbird N. Izumi L. C. Jarrott J. Jeet O. Jones G. D. Kerbel S. M. Kerr S. F. Khan J. Kilkenny Y. Kim H. Geppert-Kleinrath V. Geppert-Kleinrath C. Kong J. M. Koning J. J. Kroll M. K. G. Kruse B. Kustowski O. L. Landen S. Langer D. Larson N. C. Lemos J. D. Lindl T. Ma M. J. MacDonald B. J. MacGowan A. J. Mackinnon S. A. MacLaren A. G. MacPhee M. M. Marinak D. A. Mariscal E. V. Marley L. Masse K. D. Meaney N. B. Meezan P. A. Michel M. Millot J. L. Milovich J. D. Moody A. S. Moore J. W. Morton T. J. Murphy K. Newman J.-M. G. Di Nicola A. Nikroo R. Nora M. V. Patel L. J. Pelz J. L. Peterson Y. Ping B. B. Pollock M. Ratledge N. G. Rice H. G. Rinderknecht M. Rosen M. S. Rubery J. D. Salmonson J. Sater S. Schiaffino D. J. Schlossberg M. B. Schneider C. R. Schroeder H. A. Scott S. M. Sepke K. Sequoia M. W. Sherlock S. Shin V. A. Smalyuk B. K. Spears P. T. Springer M. Stadermann S. Stoupin D. J. Strozzi L. J. Suter C. A. Thomas R. P. J. Town C. Trosseille E. R. Tubman P. L. Volegov C. R. Weber K. Widmann C. Wild C. H. Wilde B. M. Van Wonterghem D. T. Woods B. N. Woodworth M. Yamaguchi S. T. Yang G. B. Zimmerman The impact of low-mode symmetry on inertial fusion energy output in the burning plasma state Nature Communications |
| title | The impact of low-mode symmetry on inertial fusion energy output in the burning plasma state |
| title_full | The impact of low-mode symmetry on inertial fusion energy output in the burning plasma state |
| title_fullStr | The impact of low-mode symmetry on inertial fusion energy output in the burning plasma state |
| title_full_unstemmed | The impact of low-mode symmetry on inertial fusion energy output in the burning plasma state |
| title_short | The impact of low-mode symmetry on inertial fusion energy output in the burning plasma state |
| title_sort | impact of low mode symmetry on inertial fusion energy output in the burning plasma state |
| url | https://doi.org/10.1038/s41467-024-47302-8 |
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