Measurements of K-edge and L-edge extended x-ray absorption fine structure at the national ignition facility (invited).


Journal

The Review of scientific instruments
ISSN: 1089-7623
Titre abrégé: Rev Sci Instrum
Pays: United States
ID NLM: 0405571

Informations de publication

Date de publication:
01 Oct 2024
Historique:
received: 17 05 2024
accepted: 26 09 2024
medline: 22 10 2024
pubmed: 22 10 2024
entrez: 22 10 2024
Statut: ppublish

Résumé

High-energy-density laser facilities and advances in dynamic compression techniques have expanded access to material states in the Terapascal regime relevant to inertial confinement fusion, planetary science, and geophysics. However, experimentally determining the material temperature in these extreme conditions has remained a difficult challenge. Extended X-ray Absorption Fine Structure (EXAFS), referring to the modulations in x-ray absorption above an absorption edge from photoelectrons' interactions with neighboring atoms, has proven to be a versatile and robust technique for probing material temperature and density for mid-to-high Z elements under dynamic compression. The current platform at the National Ignition Facility has developed six configurations for EXAFS measurements between 7 and 18 keV for different absorption edges (Fe K, Co K, Cu K, Ta L3, Pb L3, and Zr K) using a curved-crystal spectrometer and a bright, continuum foil x-ray source. In this work, we describe the platform geometry, x-ray source performance, spectrometer resolution and throughput, design considerations, and data in ambient and dynamic-compression conditions.

Identifiants

pubmed: 39436161
pii: 3317652
doi: 10.1063/5.0219575
pii:
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Informations de copyright

© 2024 Author(s). Published under an exclusive license by AIP Publishing.

Auteurs

H Sio (H)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

A Krygier (A)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

S Stoupin (S)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

R E Rudd (RE)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

S A Bonev (SA)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

D G Braun (DG)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

F Coppari (F)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

A L Coleman (AL)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

N Bhandarkar (N)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

M Bitter (M)

Princeton Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08543, USA.

D K Bradley (DK)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

J Buscho (J)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

J Corbin (J)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

M Dozieres (M)

General Atomics, San Diego, California 92121, USA.

P C Efthimion (PC)

Princeton Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08543, USA.

J H Eggert (JH)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

L Gao (L)

Princeton Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08543, USA.

K W Hill (KW)

Princeton Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08543, USA.

S Hamel (S)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

W Hsing (W)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

B Kozioziemski (B)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

B F Kraus (BF)

Princeton Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08543, USA.

O L Landen (OL)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

K Le Galloudec (K)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

T E Lockard (TE)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

A Mackinnon (A)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

M May (M)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

J M McNaney (JM)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

N Ose (N)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

N Pablant (N)

Princeton Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08543, USA.

H-S Park (HS)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

J Riddles (J)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

M Sharma (M)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

M B Schneider (MB)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

C Stan (C)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

N Thompson (N)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

D B Thorn (DB)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

S Vonhof (S)

General Atomics, San Diego, California 92121, USA.

Y Ping (Y)

Lawrence Livermore National Laboratory, Livermore, California 94550, USA.

Classifications MeSH