Current two-dimensional X-ray imaging at the National Ignition Facility (NIF) uses time resolved pinhole cameras with ∼10-25 μm pinholes. This method has limitations in the smallest resolvable features that can be imaged with reasonable photon statistics for inertial confinement fusion (ICF) applications. ICF sources have a broadband self-emission spectrum that causes the pinhole images obtained, through thin foil filters, to contain a similarly broadband spectrum complicating the interpretation of structure in the source. In order to study phenomena on the scale of ∼5 μm, such as dopant mix in the ICF capsule, a narrow energy band, higher spatial resolution microscope system with improved signal/noise has been developed using X-ray optics. Utilizing grazing incidence mirrors in a Kirkpatrick-Baez microscope (KBM) configuration [P. Kirkpatrick and A. V. Baez, J. Opt. Soc. Am. 38, 766–774 (1948)], an X-ray microscope has been designed and fielded on NIF with four imaging channels. The KBM has ∼12 × magnification, <8 μm resolution, and higher throughput in comparison to similar pinhole systems. The first KBM mirrors are coated with a multilayer mirror to allow a “narrow band” energy response at 10.2 keV with ΔE ∼ 3 keV. By adjusting the mirror coating only, the energy response can be matched to the future experimental requirements. Several mirror packs have been commissioned and are interchangeable in the diagnostic snout.
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November 2016
Research Article|
August 10 2016
The National Ignition Facility modular Kirkpatrick-Baez microscope
L. A. Pickworth;
L. A. Pickworth
a)
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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J. Ayers;
J. Ayers
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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P. Bell;
P. Bell
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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N. F. Brejnholt;
N. F. Brejnholt
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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J. G. Buscho;
J. G. Buscho
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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D. Bradley;
D. Bradley
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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T. Decker;
T. Decker
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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S. Hau-Riege;
S. Hau-Riege
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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J. Kilkenny;
J. Kilkenny
2
General Atomics
, San Diego, California 92121, USA
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T. McCarville;
T. McCarville
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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T. Pardini;
T. Pardini
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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J. Vogel;
J. Vogel
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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C. Walton
C. Walton
1
Lawrence Livermore National Laboratory
, Livermore, California 94550, USA
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a)
Author to whom correspondence should be addressed. Electronic mail: pickworth1@llnl.gov
Contributed paper, published as part of the Proceedings of the 21st Topical Conference on High-Temperature Plasma Diagnostics, Madison, Wisconsin, USA, June 2016.
Rev. Sci. Instrum. 87, 11E316 (2016)
Article history
Received:
June 06 2016
Accepted:
July 13 2016
Citation
L. A. Pickworth, J. Ayers, P. Bell, N. F. Brejnholt, J. G. Buscho, D. Bradley, T. Decker, S. Hau-Riege, J. Kilkenny, T. McCarville, T. Pardini, J. Vogel, C. Walton; The National Ignition Facility modular Kirkpatrick-Baez microscope. Rev. Sci. Instrum. 1 November 2016; 87 (11): 11E316. https://doi.org/10.1063/1.4960417
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