Time-resolved RIXS experiment with pulse-by-pulse parallel readout data collection using X-ray free electron laser.


Journal

Scientific reports
ISSN: 2045-2322
Titre abrégé: Sci Rep
Pays: England
ID NLM: 101563288

Informations de publication

Date de publication:
17 Dec 2020
Historique:
received: 18 08 2020
accepted: 30 11 2020
entrez: 18 12 2020
pubmed: 19 12 2020
medline: 19 12 2020
Statut: epublish

Résumé

Time-resolved resonant inelastic X-ray scattering (RIXS) is one of the developing techniques enabled by the advent of X-ray free electron laser (FEL). It is important to evaluate how the FEL jitter, which is inherent in the self-amplified spontaneous emission process, influences the RIXS measurement. Here, we use a microchannel plate (MCP) based Timepix soft X-ray detector to conduct a time-resolved RIXS measurement at the Ti L

Identifiants

pubmed: 33335197
doi: 10.1038/s41598-020-79210-4
pii: 10.1038/s41598-020-79210-4
pmc: PMC7746750
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

22226

Subventions

Organisme : U.S. Department of Energy (DOE)
ID : DE-AC02-76SF00515

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Auteurs

H Lu (H)

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road, Menlo Park, CA, 94025, USA.

A Gauthier (A)

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road, Menlo Park, CA, 94025, USA.

M Hepting (M)

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road, Menlo Park, CA, 94025, USA.

A S Tremsin (AS)

Space Sciences Laboratory, University of California at Berkeley, Berkeley, CA, 94720, USA.

A H Reid (AH)

Linac Coherent Light Source (LCLS), SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA.

P S Kirchmann (PS)

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road, Menlo Park, CA, 94025, USA.
Geballe Laboratory for Advanced Materials, Departments of Physics and Applied Physics, Stanford University, Stanford, CA, 94305, USA.

Z X Shen (ZX)

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road, Menlo Park, CA, 94025, USA.
Geballe Laboratory for Advanced Materials, Departments of Physics and Applied Physics, Stanford University, Stanford, CA, 94305, USA.

T P Devereaux (TP)

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road, Menlo Park, CA, 94025, USA.
Geballe Laboratory for Advanced Materials, Departments of Physics and Applied Physics, Stanford University, Stanford, CA, 94305, USA.
Department of Materials Science and Engineering, Stanford University, Stanford, CA, 94305, USA.

Y C Shao (YC)

Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA.

X Feng (X)

Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA.

G Coslovich (G)

Linac Coherent Light Source (LCLS), SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA.

Z Hussain (Z)

Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA.

G L Dakovski (GL)

Linac Coherent Light Source (LCLS), SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA.

Y D Chuang (YD)

Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA.

W S Lee (WS)

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road, Menlo Park, CA, 94025, USA. leews@stanford.edu.

Classifications MeSH