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Article ; Online: Using x-rays to test chemical vapor deposited diamond detectors for areal density measurement at the National Ignition Facility.

Dauffy, L S / Koch, J A / Tommasini, R / Izumi, N

2008 Volume 79, Issue 10, Page(s) 10E931

Abstract: At the National Ignition Facility (NIF), 192 laser beams will compress a target containing a mixture of deuterium and tritium that will release fusion neutrons, photons, and other radiation. Diagnostics are being designed to measure this emitted ... ...

Abstract	At the National Ignition Facility (NIF), 192 laser beams will compress a target containing a mixture of deuterium and tritium that will release fusion neutrons, photons, and other radiation. Diagnostics are being designed to measure this emitted radiation to infer crucial parameters of an ignition shot. Chemical vapor deposited (CVD) diamond is one of the ignition diagnostics that will be used as a neutron time-of-flight detector for measuring primary (14.1 MeV) neutron yield, ion temperature, and plasma areal density. This last quantity is the subject of this study and is inferred from the number of downscattered neutrons arriving late in time, divided by the number of primary neutrons. We determine in this study the accuracy with which this detector can measure areal density when the limiting factor is detector and electronics saturation. We used laser-produced x-rays to reproduce NIF signals in terms of charge carrier density, time between pulses, and amplitude contrast and found that the effect of the large pulse on the small pulse is at most 8.4%, which is less than the NIF accuracy requirement of +/-10%.
Language	English
Publishing date	2008-10
Publishing country	United States
Document type	Journal Article
ZDB-ID	209865-9
ISSN	1089-7623 ; 0034-6748
ISSN (online)	1089-7623
ISSN	0034-6748
DOI	10.1063/1.2955705
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Article ; Online: Diagnosing inertial confinement fusion gamma ray physics (invited).

Herrmann, H W / Hoffman, N / Wilson, D C / Stoeffl, W / Dauffy, L / Kim, Y H / McEvoy, A / Young, C S / Mack, J M / Horsfield, C J / Rubery, M / Miller, E K / Ali, Z A

The Review of scientific instruments

2010 Volume 81, Issue 10, Page(s) 10D333

Abstract: The gamma reaction history (GRH) diagnostic is a multichannel, time-resolved, energy-thresholded γ-ray spectrometer that provides a high-bandwidth, direct-measurement of fusion reaction history in inertial confinement fusion implosion experiments. 16.75 ... ...

Abstract	The gamma reaction history (GRH) diagnostic is a multichannel, time-resolved, energy-thresholded γ-ray spectrometer that provides a high-bandwidth, direct-measurement of fusion reaction history in inertial confinement fusion implosion experiments. 16.75 MeV deuterium+tritium (DT) fusion γ-rays, with a branching ratio of the order of 10(-5)γ/(14 MeV n), are detected to determine fundamental burn parameters, such as nuclear bang time and burn width, critical to achieving ignition at the National Ignition Facility. During the tritium/hydrogen/deuterium ignition tuning campaign, an additional γ-ray line at 19.8 MeV, produced by hydrogen+tritium fusion with a branching ratio of unity, will increase the available γ-ray signal and may allow measurement of reacting fuel composition or ion temperature. Ablator areal density measurements with the GRH are also made possible by detection of 4.43 MeV γ-rays produced by inelastic scatter of DT fusion neutrons on (12)C nuclei in the ablating plastic capsule material.
Language	English
Publishing date	2010-10
Publishing country	United States
Document type	Journal Article
ZDB-ID	209865-9
ISSN	1089-7623 ; 0034-6748
ISSN (online)	1089-7623
ISSN	0034-6748
DOI	10.1063/1.3495770
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Article ; Online: Tests and calibration of NIF neutron time of flight detectors.

Ali, Z A / Glebov, V Yu / Cruz, M / Duffy, T / Stoeckl, C / Roberts, S / Sangster, T C / Tommasini, R / Throop, A / Moran, M / Dauffy, L / Horsefield, C

The Review of scientific instruments

2008 Volume 79, Issue 10, Page(s) 10E527

Abstract: The National Ignition Facility (NIF) neutron time of flight (NTOF) diagnostic will measure neutron yield and ion temperature in all NIF campaigns in DD, DT, and THD(*) implosions. The NIF NTOF diagnostic is designed to measure neutron yield from 1x10(9) ... ...

Abstract	The National Ignition Facility (NIF) neutron time of flight (NTOF) diagnostic will measure neutron yield and ion temperature in all NIF campaigns in DD, DT, and THD(*) implosions. The NIF NTOF diagnostic is designed to measure neutron yield from 1x10(9) to 2x10(19). The NTOF consists of several detectors of varying sensitivity located on the NIF at about 5 and 20 m from the target. Production, testing, and calibration of the NIF NTOF detectors have begun at the Laboratory for Laser Energetics (LLE). Operational tests of the NTOF detectors were performed on several facilities including the OMEGA laser at LLE and the Titan laser at Lawrence Livermore National Laboratory. Neutron calibrations were carried out on the OMEGA laser. Results of the NTOF detector tests and calibration will be presented.
Language	English
Publishing date	2008-10
Publishing country	United States
Document type	Journal Article
ZDB-ID	209865-9
ISSN	1089-7623 ; 0034-6748
ISSN (online)	1089-7623
ISSN	0034-6748
DOI	10.1063/1.2969289
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Article ; Online: Analysis of decay dose rates and dose management in the National Ignition Facility.

Khater, Hesham / Brereton, Sandra / Dauffy, Lucile / Hall, Jim / Hansen, Luisa / Kim, Soon / Kohut, Tom / Pohl, Bertram / Sitaraman, Shiva / Verbeke, Jerome / Young, Mitchell

Health physics

2013 Volume 104, Issue 6, Page(s) 580–588

Abstract: A detailed model of the Target Bay (TB) at the National Ignition Facility (NIF) has been developed to estimate the post-shot radiation environment inside the facility. The model includes the large number of structures and diagnostic instruments present ... ...

Abstract	A detailed model of the Target Bay (TB) at the National Ignition Facility (NIF) has been developed to estimate the post-shot radiation environment inside the facility. The model includes the large number of structures and diagnostic instruments present inside the TB. These structures and instruments are activated by neutrons generated during a shot, and the resultant gamma dose rates are estimated at various decay times following the shot. A set of computational tools was developed to help in estimating potential radiation exposure to TB workers. The results presented in this paper describe the expected radiation environment inside the TB following a low-yield DT shot of 10(16) neutrons. General environment dose rates drop below 30 μSv h(-1) within 3 h following a shot, with higher dose rates observed in the vicinity (~30 cm) of few components. The dose rates drop by more than a factor of two at 1 d following the shot. Dose rate maps of the different TB levels were generated to aid in estimating worker stay-out times following a shot before entry is permitted into the TB. Primary components, including the Target Chamber and diagnostic and beam line components, are constructed of aluminum. Near-term TB accessibility is driven by the decay of the aluminum activation product, 24Na. Worker dose is managed using electronic dosimeters (EDs) self-issued at kiosks using commercial dose management software. The software programs the ED dose and dose rate alarms based on the Radiological Work Permit (RWP) and tracks dose by individual, task, and work group.
MeSH term(s)	Facility Design and Construction ; Gamma Rays ; Humans ; Neutrons ; Nuclear Fusion ; Radiation Dosage ; Radiation Monitoring/methods ; Radiation Monitoring/standards ; Radiation Protection/methods ; Software
Language	English
Publishing date	2013-06
Publishing country	United States
Document type	Journal Article ; Research Support, U.S. Gov't, Non-P.H.S.
ZDB-ID	2406-5
ISSN	1538-5159 ; 0017-9078
ISSN (online)	1538-5159
ISSN	0017-9078
DOI	10.1097/HP.0b013e31828d0134
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Article: Application of MINERVA Monte Carlo simulations to targeted radionuclide therapy.

Descalle, Marie-Anne / Hartmann Siantar, Christine L / Dauffy, Lucile / Nigg, David W / Wemple, Charles A / Yuan, Aina / DeNardo, Gerald L

Cancer biotherapy & radiopharmaceuticals

2003 Volume 18, Issue 1, Page(s) 71–79

Abstract: Recent clinical results have demonstrated the promise of targeted radionuclide therapy for advanced cancer. As the success of this emerging form of radiation therapy grows, accurate treatment planning and radiation dose simulations are likely to become ... ...

Abstract	Recent clinical results have demonstrated the promise of targeted radionuclide therapy for advanced cancer. As the success of this emerging form of radiation therapy grows, accurate treatment planning and radiation dose simulations are likely to become increasingly important. To address this need, we have initiated the development of a new, Monte Carlo transport-based treatment planning system for molecular targeted radiation therapy as part of the MINERVA system. The goal of the MINERVA dose calculation system is to provide 3-D Monte Carlo simulation-based dosimetry for radiation therapy, focusing on experimental and emerging applications. For molecular targeted radionuclide therapy applications, MINERVA calculates patient-specific radiation dose estimates using computed tomography to describe the patient anatomy, combined with a user-defined 3-D radiation source. This paper describes the validation of the 3-D Monte Carlo transport methods to be used in MINERVA for molecular targeted radionuclide dosimetry. It reports comparisons of MINERVA dose simulations with published absorbed fraction data for distributed, monoenergetic photon and electron sources, and for radioisotope photon emission. MINERVA simulations are generally within 2% of EGS4 results and 10% of MCNP results, but differ by up to 40% from the recommendations given in MIRD Pamphlets 3 and 8 for identical medium composition and density. For several representative source and target organs in the abdomen and thorax, specific absorbed fractions calculated with the MINERVA system are generally within 5% of those published in the revised MIRD Pamphlet 5 for 100 keV photons. However, results differ by up to 23% for the adrenal glands, the smallest of our target organs. Finally, we show examples of Monte Carlo simulations in a patient-like geometry for a source of uniform activity located in the kidney.
MeSH term(s)	Algorithms ; Humans ; Monte Carlo Method ; Neoplasms/radiotherapy ; Radioisotopes/therapeutic use ; Radiotherapy Dosage ; Radiotherapy Planning, Computer-Assisted
Chemical Substances	Radioisotopes
Language	English
Publishing date	2003-02
Publishing country	United States
Document type	Journal Article ; Research Support, Non-U.S. Gov't ; Research Support, U.S. Gov't, Non-P.H.S. ; Research Support, U.S. Gov't, P.H.S.
ZDB-ID	1315649-4
ISSN	1084-9785
ISSN	1084-9785
DOI	10.1089/108497803321269340
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Article ; Online: Achievement of Target Gain Larger than Unity in an Inertial Fusion Experiment.

Abu-Shawareb, H / Acree, R / Adams, P / Adams, J / Addis, B / Aden, R / Adrian, P / Afeyan, B B / Aggleton, M / Aghaian, L / Aguirre, A / Aikens, D / Akre, J / Albert, F / Albrecht, M / Albright, B J / Albritton, J / Alcala, J / Alday, C /

Alessi, D A / Alexander, N / Alfonso, J / Alfonso, N / Alger, E / Ali, S J / Ali, Z A / Allen, A / Alley, W E / Amala, P / Amendt, P A / Amick, P / Ammula, S / Amorin, C / Ampleford, D J / Anderson, R W / Anklam, T / Antipa, N / Appelbe, B / Aracne-Ruddle, C / Araya, E / Archuleta, T N / Arend, M / Arnold, P / Arnold, T / Arsenlis, A / Asay, J / Atherton, L J / Atkinson, D / Atkinson, R / Auerbach, J M / Austin, B / Auyang, L / Awwal, A A S / Aybar, N / Ayers, J / Ayers, S / Ayers, T / Azevedo, S / Bachmann, B / Back, C A / Bae, J / Bailey, D S / Bailey, J / Baisden, T / Baker, K L / Baldis, H / Barber, D / Barberis, M / Barker, D / Barnes, A / Barnes, C W / Barrios, M A / Barty, C / Bass, I / Batha, S H / Baxamusa, S H / Bazan, G / Beagle, J K / Beale, R / Beck, B R / Beck, J B / Bedzyk, M / Beeler, R G / Behrendt, W / Belk, L / Bell, P / Belyaev, M / Benage, J F / Bennett, G / Benedetti, L R / Benedict, L X / Berger, R L / Bernat, T / Bernstein, L A / Berry, B / Bertolini, L / Besenbruch, G / Betcher, J / Bettenhausen, R / Betti, R / Bezzerides, B / Bhandarkar, S D / Bickel, R / Biener, J / Biesiada, T / Bigelow, K / Bigelow-Granillo, J / Bigman, V / Bionta, R M / Birge, N W / Bitter, M / Black, A C / Bleile, R / Bleuel, D L / Bliss, E / Blue, B / Boehly, T / Boehm, K / Boley, C D / Bonanno, R / Bond, E J / Bond, T / Bonino, M J / Borden, M / Bourgade, J-L / Bousquet, J / Bowers, J / Bowers, M / Boyd, R / Boyle, D / Bozek, A / Bradley, D K / Bradley, K S / Bradley, P A / Bradley, L / Brannon, L / Brantley, P S / Braun, D / Braun, T / Brienza-Larsen, K / Briggs, R / Briggs, T M / Britten, J / Brooks, E D / Browning, D / Bruhn, M W / Brunner, T A / Bruns, H / Brunton, G / Bryant, B / Buczek, T / Bude, J / Buitano, L / Burkhart, S / Burmark, J / Burnham, A / Burr, R / Busby, L E / Butlin, B / Cabeltis, R / Cable, M / Cabot, W H / Cagadas, B / Caggiano, J / Cahayag, R / Caldwell, S E / Calkins, S / Callahan, D A / Calleja-Aguirre, J / Camara, L / Camp, D / Campbell, E M / Campbell, J H / Carey, B / Carey, R / Carlisle, K / Carlson, L / Carman, L / Carmichael, J / Carpenter, A / Carr, C / Carrera, J A / Casavant, D / Casey, A / Casey, D T / Castillo, A / Castillo, E / Castor, J I / Castro, C / Caughey, W / Cavitt, R / Celeste, J / Celliers, P M / Cerjan, C / Chandler, G / Chang, B / Chang, C / Chang, J / Chang, L / Chapman, R / Chapman, T D / Chase, L / Chen, H / Chen, K / Chen, L-Y / Cheng, B / Chittenden, J / Choate, C / Chou, J / Chrien, R E / Chrisp, M / Christensen, K / Christensen, M / Christiansen, N S / Christopherson, A R / Chung, M / Church, J A / Clark, A / Clark, D S / Clark, K / Clark, R / Claus, L / Cline, B / Cline, J A / Cobble, J A / Cochrane, K / Cohen, B / Cohen, S / Collette, M R / Collins, G W / Collins, L A / Collins, T J B / Conder, A / Conrad, B / Conyers, M / Cook, A W / Cook, D / Cook, R / Cooley, J C / Cooper, G / Cope, T / Copeland, S R / Coppari, F / Cortez, J / Cox, J / Crandall, D H / Crane, J / Craxton, R S / Cray, M / Crilly, A / Crippen, J W / Cross, D / Cuneo, M / Cuotts, G / Czajka, C E / Czechowicz, D / Daly, T / Danforth, P / Danly, C / Darbee, R / Darlington, B / Datte, P / Dauffy, L / Davalos, G / Davidovits, S / Davis, P / Davis, J / Dawson, S / Day, R D / Day, T H / Dayton, M / Deck, C / Decker, C / Deeney, C / DeFriend, K A / Deis, G / Delamater, N D / Delettrez, J A / Demaret, R / Demos, S / Dempsey, S M / Desjardin, R / Desjardins, T / Desjarlais, M P / Dewald, E L / DeYoreo, J / Diaz, S / Dimonte, G / Dittrich, T R / Divol, L / Dixit, S N / Dixon, J / Do, A / Dodd, E S / Dolan, D / Donovan, A / Donovan, M / Döppner, T / Dorrer, C / Dorsano, N / Douglas, M R / Dow, D / Downie, J / Downing, E / Dozieres, M / Draggoo, V / Drake, D / Drake, R P / Drake, T / Dreifuerst, G / Drury, O / DuBois, D F / DuBois, P F / Dunham, G / Durocher, M / Dylla-Spears, R / Dymoke-Bradshaw, A K L / Dzenitis, B / Ebbers, C / Eckart, M / Eddinger, S / Eder, D / Edgell, D / Edwards, M J / Efthimion, P / Eggert, J H / Ehrlich, B / Ehrmann, P / Elhadj, S / Ellerbee, C / Elliott, N S / Ellison, C L / Elsner, F / Emerich, M / Engelhorn, K / England, T / English, E / Epperson, P / Epstein, R / Erbert, G / Erickson, M A / Erskine, D J / Erlandson, A / Espinosa, R J / Estes, C / Estabrook, K G / Evans, S / Fabyan, A / Fair, J / Fallejo, R / Farmer, N / Farmer, W A / Farrell, M / Fatherley, V E / Fedorov, M / Feigenbaum, E / Fehrenbach, T / Feit, M / Felker, B / Ferguson, W / Fernandez, J C / Fernandez-Panella, A / Fess, S / Field, J E / Filip, C V / Fincke, J R / Finn, T / Finnegan, S M / Finucane, R G / Fischer, M / Fisher, A / Fisher, J / Fishler, B / Fittinghoff, D / Fitzsimmons, P / Flegel, M / Flippo, K A / Florio, J / Folta, J / Folta, P / Foreman, L R / Forrest, C / Forsman, A / Fooks, J / Foord, M / Fortner, R / Fournier, K / Fratanduono, D E / Frazier, N / Frazier, T / Frederick, C / Freeman, M S / Frenje, J / Frey, D / Frieders, G / Friedrich, S / Froula, D H / Fry, J / Fuller, T / Gaffney, J / Gales, S / Le Galloudec, B / Le Galloudec, K K / Gambhir, A / Gao, L / Garbett, W J / Garcia, A / Gates, C / Gaut, E / Gauthier, P / Gavin, Z / Gaylord, J / Geddes, C G R / Geissel, M / Génin, F / Georgeson, J / Geppert-Kleinrath, H / Geppert-Kleinrath, V / Gharibyan, N / Gibson, J / Gibson, C / Giraldez, E / Glebov, V / Glendinning, S G / Glenn, S / Glenzer, S H / Goade, S / Gobby, P L / Goldman, S R / Golick, B / Gomez, M / Goncharov, V / Goodin, D / Grabowski, P / Grafil, E / Graham, P / Grandy, J / Grasz, E / Graziani, F R / Greenman, G / Greenough, J A / Greenwood, A / Gregori, G / Green, T / Griego, J R / Grim, G P / Grondalski, J / Gross, S / Guckian, J / Guler, N / Gunney, B / Guss, G / Haan, S / Hackbarth, J / Hackel, L / Hackel, R / Haefner, C / Hagmann, C / Hahn, K D / Hahn, S / Haid, B J / Haines, B M / Hall, B M / Hall, C / Hall, G N / Hamamoto, M / Hamel, S / Hamilton, C E / Hammel, B A / Hammer, J H / Hampton, G / Hamza, A / Handler, A / Hansen, S / Hanson, D / Haque, R / Harding, D / Harding, E / Hares, J D / Harris, D B / Harte, J A / Hartouni, E P / Hatarik, R / Hatchett, S / Hauer, A A / Havre, M / Hawley, R / Hayes, J / Hayes, S / Hayes-Sterbenz, A / Haynam, C A / Haynes, D A / Headley, D / Heal, A / Heebner, J E / Heerey, S / Heestand, G M / Heeter, R / Hein, N / Heinbockel, C / Hendricks, C / Henesian, M / Heninger, J / Henrikson, J / Henry, E A / Herbold, E B / Hermann, M R / Hermes, G / Hernandez, J E / Hernandez, V J / Herrmann, M C / Herrmann, H W / Herrera, O D / Hewett, D / Hibbard, R / Hicks, D G / Higginson, D P / Hill, D / Hill, K / Hilsabeck, T / Hinkel, D E / Ho, D D / Ho, V K / Hoffer, J K / Hoffman, N M / Hohenberger, M / Hohensee, M / Hoke, W / Holdener, D / Holdener, F / Holder, J P / Holko, B / Holunga, D / Holzrichter, J F / Honig, J / Hoover, D / Hopkins, D / Berzak Hopkins, L F / Hoppe, M / Hoppe, M L / Horner, J / Hornung, R / Horsfield, C J / Horvath, J / Hotaling, D / House, R / Howell, L / Hsing, W W / Hu, S X / Huang, H / Huckins, J / Hui, H / Humbird, K D / Hund, J / Hunt, J / Hurricane, O A / Hutton, M / Huynh, K H-K / Inandan, L / Iglesias, C / Igumenshchev, I V / Ivanovich, I / Izumi, N / Jackson, M / Jackson, J / Jacobs, S D / James, G / Jancaitis, K / Jarboe, J / Jarrott, L C / Jasion, D / Jaquez, J / Jeet, J / Jenei, A E / Jensen, J / Jimenez, J / Jimenez, R / Jobe, D / Johal, Z / Johns, H M / Johnson, D / Johnson, M A / Gatu Johnson, M / Johnson, R J / Johnson, S / Johnson, S A / Johnson, T / Jones, K / Jones, O / Jones, M / Jorge, R / Jorgenson, H J / Julian, M / Jun, B I / Jungquist, R / Kaae, J / Kabadi, N / Kaczala, D / Kalantar, D / Kangas, K / Karasiev, V V / Karasik, M / Karpenko, V / Kasarky, A / Kasper, K / Kauffman, R / Kaufman, M I / Keane, C / Keaty, L / Kegelmeyer, L / Keiter, P A / Kellett, P A / Kellogg, J / Kelly, J H / Kemic, S / Kemp, A J / Kemp, G E / Kerbel, G D / Kershaw, D / Kerr, S M / Kessler, T J / Key, M H / Khan, S F / Khater, H / Kiikka, C / Kilkenny, J / Kim, Y / Kim, Y-J / Kimko, J / Kimmel, M / Kindel, J M / King, J / Kirkwood, R K / Klaus, L / Klem, D / Kline, J L / Klingmann, J / Kluth, G / Knapp, P / Knauer, J / Knipping, J / Knudson, M / Kobs, D / Koch, J / Kohut, T / Kong, C / Koning, J M / Koning, P / Konior, S / Kornblum, H / Kot, L B / Kozioziemski, B / Kozlowski, M / Kozlowski, P M / Krammen, J / Krasheninnikova, N S / Krauland, C M / Kraus, B / Krauser, W / Kress, J D / Kritcher, A L / Krieger, E / Kroll, J J / Kruer, W L / Kruse, M K G / Kucheyev, S / Kumbera, M / Kumpan, S / Kunimune, J / Kur, E / Kustowski, B / Kwan, T J T / Kyrala, G A / Laffite, S / Lafon, M / LaFortune, K / Lagin, L / Lahmann, B / Lairson, B / Landen, O L / Land, T / Lane, M / Laney, D / Langdon, A B / Langenbrunner, J / Langer, S H / Langro, A / Lanier, N E / Lanier, T E / Larson, D / Lasinski, B F / Lassle, D / LaTray, D / Lau, G / Lau, N / Laumann, C / Laurence, A / Laurence, T A / Lawson, J / Le, H P / Leach, R R / Leal, L / Leatherland, A / LeChien, K / Lechleiter, B / Lee, A / Lee, M / Lee, T / Leeper, R J / Lefebvre, E / Leidinger, J-P / LeMire, B / Lemke, R W / Lemos, N C / Le Pape, S / Lerche, R / Lerner, S / Letts, S / Levedahl, K / Lewis, T / Li, C K / Li, H / Li, J / Liao, W / Liao, Z M / Liedahl, D / Liebman, J / Lindford, G / Lindman, E L / Lindl, J D / Loey, H / London, R A / Long, F / Loomis, E N / Lopez, F E / Lopez, H / Losbanos, E / Loucks, S / Lowe-Webb, R / Lundgren, E / Ludwigsen, A P / Luo, R / Lusk, J / Lyons, R / Ma, T / Macallop, Y / MacDonald, M J / MacGowan, B J / Mack, J M / Mackinnon, A J / MacLaren, S A / MacPhee, A G / Magelssen, G R / Magoon, J / Malone, R M / Malsbury, T / Managan, R / Mancini, R / Manes, K / Maney, D / Manha, D / Mannion, O M / Manuel, A M / Manuel, M J-E / Mapoles, E / Mara, G / Marcotte, T / Marin, E / Marinak, M M / Mariscal, D A / Mariscal, E F / Marley, E V / Marozas, J A / Marquez, R / Marshall, C D / Marshall, F J / Marshall, M / Marshall, S / Marticorena, J / Martinez, J I / Martinez, D / Maslennikov, I / Mason, D / Mason, R J / Masse, L / Massey, W / Masson-Laborde, P-E / Masters, N D / Mathisen, D / Mathison, E / Matone, J / Matthews, M J / Mattoon, C / Mattsson, T R / Matzen, K / Mauche, C W / Mauldin, M / McAbee, T / McBurney, M / Mccarville, T / McCrory, R L / McEvoy, A M / McGuffey, C / Mcinnis, M / McKenty, P / McKinley, M S / McLeod, J B / McPherson, A / Mcquillan, B / Meamber, M / Meaney, K D / Meezan, N B / Meissner, R / Mehlhorn, T A / Mehta, N C / Menapace, J / Merrill, F E / Merritt, B T / Merritt, E C / Meyerhofer, D D / Mezyk, S / Mich, R J / Michel, P A / Milam, D / Miller, C / Miller, D / Miller, D S / Miller, E / Miller, E K / Miller, J / Miller, M / Miller, P E / Miller, T / Miller, W / Miller-Kamm, V / Millot, M / Milovich, J L / Minner, P / Miquel, J-L / Mitchell, S / Molvig, K / Montesanti, R C / Montgomery, D S / Monticelli, M / Montoya, A / Moody, J D / Moore, A S / Moore, E / Moran, M / Moreno, J C 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Physical review letters

2024 Volume 132, Issue 6, Page(s) 65102

Abstract: On December 5, 2022, an indirect drive fusion implosion on the National Ignition Facility (NIF) achieved a target gain G_{target} of 1.5. This is the first laboratory demonstration of exceeding "scientific breakeven" (or G_{target}>1) where 2.05 MJ of ... ...

Abstract	On December 5, 2022, an indirect drive fusion implosion on the National Ignition Facility (NIF) achieved a target gain G_{target} of 1.5. This is the first laboratory demonstration of exceeding "scientific breakeven" (or G_{target}>1) where 2.05 MJ of 351 nm laser light produced 3.1 MJ of total fusion yield, a result which significantly exceeds the Lawson criterion for fusion ignition as reported in a previous NIF implosion [H. Abu-Shawareb et al. (Indirect Drive ICF Collaboration), Phys. Rev. Lett. 129, 075001 (2022)PRLTAO0031-900710.1103/PhysRevLett.129.075001]. This achievement is the culmination of more than five decades of research and gives proof that laboratory fusion, based on fundamental physics principles, is possible. This Letter reports on the target, laser, design, and experimental advancements that led to this result.
Language	English
Publishing date	2024-02-23
Publishing country	United States
Document type	Journal Article
ZDB-ID	208853-8
ISSN	1079-7114 ; 0031-9007
ISSN (online)	1079-7114
ISSN	0031-9007
DOI	10.1103/PhysRevLett.132.065102
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Article ; Online: Lawson Criterion for Ignition Exceeded in an Inertial Fusion Experiment.

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Zaka, F / Ze, F / Zeiger, B / Zika, M / Zimmerman, G B / Zobrist, T / Zuegel, J D / Zylstra, A B

Physical review letters

2021 Volume 129, Issue 7, Page(s) 75001

Abstract: For more than half a century, researchers around the world have been engaged in attempts to achieve fusion ignition as a proof of principle of various fusion concepts. Following the Lawson criterion, an ignited plasma is one where the fusion heating ... ...

Abstract	For more than half a century, researchers around the world have been engaged in attempts to achieve fusion ignition as a proof of principle of various fusion concepts. Following the Lawson criterion, an ignited plasma is one where the fusion heating power is high enough to overcome all the physical processes that cool the fusion plasma, creating a positive thermodynamic feedback loop with rapidly increasing temperature. In inertially confined fusion, ignition is a state where the fusion plasma can begin "burn propagation" into surrounding cold fuel, enabling the possibility of high energy gain. While "scientific breakeven" (i.e., unity target gain) has not yet been achieved (here target gain is 0.72, 1.37 MJ of fusion for 1.92 MJ of laser energy), this Letter reports the first controlled fusion experiment, using laser indirect drive, on the National Ignition Facility to produce capsule gain (here 5.8) and reach ignition by nine different formulations of the Lawson criterion.
Language	English
Publishing date	2021-03-18
Publishing country	United States
Document type	Journal Article
ZDB-ID	208853-8
ISSN	1079-7114 ; 0031-9007
ISSN (online)	1079-7114
ISSN	0031-9007
DOI	10.1103/PhysRevLett.129.075001
Database	MEDical Literature Analysis and Retrieval System OnLINE

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