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Neutron time-of-flight ion temperature diagnostic for inertial-confinement-fusion experiments
We are constructing a {ital T}{sub {ital i}} diagnostic for low neutron yield (5{times}10{sup 7} to above 10{sup 9}) {ital d}-{ital d} and {ital d}-{ital t} targets in the Nova facility at Livermore. The diagnostic measures the neutron energy spread with 960 scintillator-photomultiplier detectors lo...
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Published in: | Review of scientific instruments 1992-10, Vol.63:10 |
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container_title | Review of scientific instruments |
container_volume | 63:10 |
creator | Chrien, R.E. Simmons, D.F. Holmberg, D.L. |
description | We are constructing a {ital T}{sub {ital i}} diagnostic for low neutron yield (5{times}10{sup 7} to above 10{sup 9}) {ital d}-{ital d} and {ital d}-{ital t} targets in the Nova facility at Livermore. The diagnostic measures the neutron energy spread with 960 scintillator-photomultiplier detectors located 28 m from the target and operates in the single-hit mode. Each detector can measure a single neutron arrival with time resolution of 1 ns or better. The arrival time distribution is constructed from the results of typically 200--500 detector measurements. The ion temperature is determined from the spread in neutron energy {Delta}{ital E}{sub {ital n}}{proportional to}{ital T}{sub {ital i}}{sup 1/2}, which is related to the arrival time spread by {Delta}{ital t}/{ital t}{congruent}{minus}(1/2){Delta}{ital E}{sub {ital n}}/{ital E}{sub {ital n}}. Each neutron arrival is detected by using a photomultiplier tube to observe the recoil proton from elastic scattering in a fast plastic scintillator. The timing electronics for each channel consist of a novel constant fraction-like discriminator and a multiple hit time-to-digital converter. The overall system design, together with single-channel performance data, is presented. |
doi_str_mv | 10.1063/1.1143540 |
format | article |
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The diagnostic measures the neutron energy spread with 960 scintillator-photomultiplier detectors located 28 m from the target and operates in the single-hit mode. Each detector can measure a single neutron arrival with time resolution of 1 ns or better. The arrival time distribution is constructed from the results of typically 200--500 detector measurements. The ion temperature is determined from the spread in neutron energy {Delta}{ital E}{sub {ital n}}{proportional to}{ital T}{sub {ital i}}{sup 1/2}, which is related to the arrival time spread by {Delta}{ital t}/{ital t}{congruent}{minus}(1/2){Delta}{ital E}{sub {ital n}}/{ital E}{sub {ital n}}. Each neutron arrival is detected by using a photomultiplier tube to observe the recoil proton from elastic scattering in a fast plastic scintillator. The timing electronics for each channel consist of a novel constant fraction-like discriminator and a multiple hit time-to-digital converter. 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The diagnostic measures the neutron energy spread with 960 scintillator-photomultiplier detectors located 28 m from the target and operates in the single-hit mode. Each detector can measure a single neutron arrival with time resolution of 1 ns or better. The arrival time distribution is constructed from the results of typically 200--500 detector measurements. The ion temperature is determined from the spread in neutron energy {Delta}{ital E}{sub {ital n}}{proportional to}{ital T}{sub {ital i}}{sup 1/2}, which is related to the arrival time spread by {Delta}{ital t}/{ital t}{congruent}{minus}(1/2){Delta}{ital E}{sub {ital n}}/{ital E}{sub {ital n}}. Each neutron arrival is detected by using a photomultiplier tube to observe the recoil proton from elastic scattering in a fast plastic scintillator. The timing electronics for each channel consist of a novel constant fraction-like discriminator and a multiple hit time-to-digital converter. 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The diagnostic measures the neutron energy spread with 960 scintillator-photomultiplier detectors located 28 m from the target and operates in the single-hit mode. Each detector can measure a single neutron arrival with time resolution of 1 ns or better. The arrival time distribution is constructed from the results of typically 200--500 detector measurements. The ion temperature is determined from the spread in neutron energy {Delta}{ital E}{sub {ital n}}{proportional to}{ital T}{sub {ital i}}{sup 1/2}, which is related to the arrival time spread by {Delta}{ital t}/{ital t}{congruent}{minus}(1/2){Delta}{ital E}{sub {ital n}}/{ital E}{sub {ital n}}. Each neutron arrival is detected by using a photomultiplier tube to observe the recoil proton from elastic scattering in a fast plastic scintillator. The timing electronics for each channel consist of a novel constant fraction-like discriminator and a multiple hit time-to-digital converter. The overall system design, together with single-channel performance data, is presented.</abstract><cop>United States</cop><doi>10.1063/1.1143540</doi></addata></record> |
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identifier | ISSN: 0034-6748 |
ispartof | Review of scientific instruments, 1992-10, Vol.63:10 |
issn | 0034-6748 1089-7623 |
language | eng |
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source | AIP Digital Archive; AIP Journals (American Institute of Physics) |
subjects | 70 PLASMA PHYSICS AND FUSION TECHNOLOGY 700320 - Plasma Diagnostic Techniques & Instrumentation- (1992-) DESIGN LASL MEASURING INSTRUMENTS NATIONAL ORGANIZATIONS NEUTRON DETECTORS NOVA FACILITY PHOTOMULTIPLIERS PHOTOTUBES PLASMA DIAGNOSTICS RADIATION DETECTORS RESOLUTION SCINTILLATION COUNTERS SCINTILLATOR-PHOTODIODE DETECTORS TIME-OF-FLIGHT METHOD US AEC US DOE US ERDA US ORGANIZATIONS |
title | Neutron time-of-flight ion temperature diagnostic for inertial-confinement-fusion experiments |
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