4.5 Article Proceedings Paper

A neutron spectrometer for precise measurements of DT neutrons from 10 to 18 MeV at OMEGA and the National Ignition Facility

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REVIEW OF SCIENTIFIC INSTRUMENTS
卷 72, 期 1, 页码 854-858

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AMER INST PHYSICS
DOI: 10.1063/1.1323243

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A model independent method to determine fuel [rhoR] is to measure the energy spectrum and yield of elastically scattered primary neutrons in deuterium-tritium (DT) plasmas. As is the case for complementary methods to measure fuel [rhoR] (in particular from knock-on deuterons and tritons [S. Skupsky and S. Kacenjar, J. Appl. Phys. 52, 2608 (1981); C. K. Li (unpublished)]), minimizing the background is critical for successful implementation. To achieve this objective, a novel spectrometer for measurements of neutrons in the energy range 10-18 MeV is proposed. From scattered neutrons (10-13 MeV), the DT fuel [rhoR] will be measured; from primary neutrons (similar to 14 MeV), the ion temperature and neutron yield will be determined; and from secondary neutrons, in the energy range 12-18 MeV, the fuel [rhoR] in deuterium plasmas will be inferred at the National Ignition Facility. The instrument is based on a magnetic spectrometer with a neutron-to-deuteron (nd) conversion foil for production of deuteron recoils at nearly forward scattered angles. In its initial phase of implementation, CR-39 track detectors will be used in the focal plane to detect the recoil deuterons with extremely high spatial resolution. Besides simplicity, CR-39 track detectors will facilitate a highly accurate energy calibration. However, in a later implementation of the spectrometer design, the recoils will also be detected by an array of fast scintillation counters functioning in current mode. In either detection scheme, the detection efficiency is about 10(-9) for measuring 14 MeV neutrons with an energy resolution of about 3%. Due to its large dynamic range, its relatively high efficiency, and a compliant design that allows for significant background rejection, this spectrometer can be effectively used, with very high resolution, at both OMEGA and the National Ignition Facility. (C) 2001 American Institute of Physics.

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