Phased plan for the implementation of the time-resolving magnetic recoil spectrometer on the National Ignition Facility (NIF)

Author:

Kunimune J. H.1ORCID,Gatu Johnson M.1ORCID,Moore A. S.2ORCID,Trosseille C. A.2ORCID,Johnson T. M.1ORCID,Berg G. P. A.3ORCID,Mackinnon A. J.2ORCID,Kilkenny J. D.2,Frenje J. A.1ORCID

Affiliation:

1. MIT PSFC, Cambridge, Massachusetts 02139, USA

2. LLNL, Livermore, California 94550, USA

3. Department of Physics and Astronomy, Notre Dame, Indiana 46556, USA

Abstract

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 × 1017. The PDDT will be used for optimal efficiency and resolution in phase 3.

Funder

Lawrence Livermore National Laboratory

Center of Excellence

Publisher

AIP Publishing

Subject

Instrumentation

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