dc.contributor.author | Kunimune, JH | |
dc.contributor.author | Gatu Johnson, M | |
dc.contributor.author | Moore, AS | |
dc.contributor.author | Trosseille, CA | |
dc.contributor.author | Johnson, TM | |
dc.contributor.author | Berg, GPA | |
dc.contributor.author | Mackinnon, AJ | |
dc.contributor.author | Kilkenny, JD | |
dc.contributor.author | Frenje, JA | |
dc.date.accessioned | 2022-09-19T18:15:28Z | |
dc.date.available | 2022-09-19T18:15:28Z | |
dc.date.issued | 2022-08-01 | |
dc.identifier.uri | https://hdl.handle.net/1721.1/145504 | |
dc.description.abstract | <jats:p> The time-resolving magnetic recoil spectrometer (MRSt) is a transformative diagnostic that will be used to measure the time-resolved neutron spectrum from an inertial confinement fusion implosion at the National Ignition Facility (NIF). It uses a CD foil on the outside of the hohlraum to convert fusion neutrons to recoil deuterons. An ion-optical system positioned outside the NIF target chamber energy-disperses and focuses forward-scattered deuterons. A pulse-dilation drift tube (PDDT) subsequently dilates, un-skews, and detects the signal. While the foil and ion-optical system have been designed, the PDDT requires more development before it can be implemented. Therefore, a phased plan is presented that first uses the foil and ion-optical systems with detectors that can be implemented immediately—namely CR-39 and hDISC streak cameras. These detectors will allow the MRSt to be commissioned in an intermediate stage and begin collecting data on a reduced timescale, while the PDDT is developed in parallel. A CR-39 detector will be used in phase 1 for the measurement of the time-integrated neutron spectra with excellent energy-resolution, necessary for the energy calibration of the system. Streak cameras will be used in phase 2 for measurement of the time-resolved spectrum with limited spectral coverage, which is sufficient to diagnose the time-resolved ion temperature. Simulations are presented that predict the performance of the streak camera detector, indicating that it will achieve excellent burn history measurements at current yields, and good time-resolved ion-temperature measurements at yields above 3 × 10<jats:sup>17</jats:sup>. The PDDT will be used for optimal efficiency and resolution in phase 3. </jats:p> | en_US |
dc.language.iso | en | |
dc.publisher | AIP Publishing | en_US |
dc.relation.isversionof | 10.1063/5.0100996 | en_US |
dc.rights | Creative Commons Attribution 4.0 International license | en_US |
dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | en_US |
dc.source | American Institute of Physics (AIP) | en_US |
dc.title | Phased plan for the implementation of the time-resolving magnetic recoil spectrometer on the National Ignition Facility (NIF) | en_US |
dc.type | Article | en_US |
dc.identifier.citation | Kunimune, JH, Gatu Johnson, M, Moore, AS, Trosseille, CA, Johnson, TM et al. 2022. "Phased plan for the implementation of the time-resolving magnetic recoil spectrometer on the National Ignition Facility (NIF)." Review of Scientific Instruments, 93 (8). | |
dc.contributor.department | Massachusetts Institute of Technology. Plasma Science and Fusion Center | en_US |
dc.relation.journal | Review of Scientific Instruments | en_US |
dc.eprint.version | Final published version | en_US |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
dc.date.updated | 2022-09-19T17:59:18Z | |
dspace.orderedauthors | Kunimune, JH; Gatu Johnson, M; Moore, AS; Trosseille, CA; Johnson, TM; Berg, GPA; Mackinnon, AJ; Kilkenny, JD; Frenje, JA | en_US |
dspace.date.submission | 2022-09-19T17:59:22Z | |
mit.journal.volume | 93 | en_US |
mit.journal.issue | 8 | en_US |
mit.license | PUBLISHER_CC | |
mit.metadata.status | Authority Work and Publication Information Needed | en_US |