Neutron activation diagnostics at the National Ignition Facility (invited)

被引:80
|
作者
Bleuel, D. L. [1 ]
Yeamans, C. B. [1 ]
Bernstein, L. A. [1 ]
Bionta, R. M. [1 ]
Caggiano, J. A. [1 ]
Casey, D. T. [2 ]
Cooper, G. W. [3 ]
Drury, O. B. [1 ]
Frenje, J. A. [2 ]
Hagmann, C. A. [1 ]
Hatarik, R. [1 ]
Knauer, J. P. [4 ]
Johnson, M. Gatu [2 ]
Knittel, K. M. [1 ]
Leeper, R. J. [5 ]
McNaney, J. M. [1 ]
Moran, M. [1 ]
Ruiz, C. L. [5 ]
Schneider, D. H. G. [1 ]
机构
[1] Lawrence Livermore Natl Lab, Livermore, CA 94550 USA
[2] MIT, Plasma Sci & Fus Ctr, Cambridge, MA 02139 USA
[3] Univ New Mexico, Albuquerque, NM 87131 USA
[4] Univ Rochester, Laser Energet Lab, Rochester, NY 14623 USA
[5] Sandia Natl Labs, Albuquerque, NM 87185 USA
来源
REVIEW OF SCIENTIFIC INSTRUMENTS | 2012年 / 83卷 / 10期
关键词
OMEGA;
D O I
10.1063/1.4733741
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
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 In-115(n,n')(115m) In reaction. Outside the chamber, zirconium and copper are used to measure 14 MeV deuterium-tritium fusion neutrons via Zr-90(n,2n), Cu-63(n,2n), and Cu-65(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. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4733741]
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页数:5
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