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Neutron activation diagnostics at the National Ignition Facility (invited)
Author(s) -
D. L. Bleuel,
C. B. Yeamans,
L. A. Bernstein,
R. M. Bionta,
J. A. Caggiano,
D. T. Casey,
G. W. Cooper,
Owen B. Drury,
J. A. Frenje,
C Hagmann,
R. Hatarik,
J. P. Knauer,
M. Gatu Johnson,
K. Knittel,
R. J. Leeper,
J. M. McNaney,
Matthew Moran,
C. L. Ruiz,
Dieter Schneider
Publication year - 2012
Publication title -
review of scientific instruments
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.605
H-Index - 165
eISSN - 1089-7623
pISSN - 0034-6748
DOI - 10.1063/1.4733741
Subject(s) - neutron , national ignition facility , nuclear physics , neutron activation , materials science , neutron temperature , deuterium , area density , neutron emission , neutron source , oak ridge national laboratory , physics , inertial confinement fusion , optics , plasma
Neutron yields are measured at the National Ignition Facility (NIF) by an extensive suite of neutron activation diagnostics. Neutrons interact with materials whose reaction cross sections threshold just below the fusion neutron production energy, providing an accurate measure of primary unscattered neutrons without contribution from lower-energy scattered neutrons. Indium samples are mounted on diagnostic instrument manipulators in the NIF target chamber, 25-50 cm from the source, to measure 2.45 MeV deuterium-deuterium fusion neutrons through the (115)In(n,n')(115 m) In reaction. Outside the chamber, zirconium and copper are used to measure 14 MeV deuterium-tritium fusion neutrons via (90)Zr(n,2n), (63)Cu(n,2n), and (65)Cu(n,2n) reactions. An array of 16 zirconium samples are located on port covers around the chamber to measure relative yield anisotropies, providing a global map of fuel areal density variation. Neutron yields are routinely measured with activation to an accuracy of 7% and are in excellent agreement both with each other and with neutron time-of-flight and magnetic recoil spectrometer measurements. Relative areal density anisotropies can be measured to a precision of less than 3%. These measurements reveal apparent bulk fuel velocities as high as 200 km/s in addition to large areal density variations between the pole and equator of the compressed fuel.

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