Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime

The average temporal (longitudinal) and spatial (transverse) coherence of free-electron-laser pulses in the extreme ultraviolet at FLASH is measured by interfering two time-delayed partial beams directly on a CCD camera. Wavelengths between λ=32  nm and λ=8  nm are examined. A decrease of the cohere...

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Main Authors: S. Roling, B. Siemer, M. Wöstmann, H. Zacharias, R. Mitzner, A. Singer, K. Tiedtke, I. A. Vartanyants
Format: Article
Language:English
Published: American Physical Society 2011-08-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.14.080701
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spelling doaj-fec58e76662547739e9b4389922873d02020-11-25T00:49:46ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022011-08-0114808070110.1103/PhysRevSTAB.14.080701Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regimeS. RolingB. SiemerM. WöstmannH. ZachariasR. MitznerA. SingerK. TiedtkeI. A. VartanyantsThe average temporal (longitudinal) and spatial (transverse) coherence of free-electron-laser pulses in the extreme ultraviolet at FLASH is measured by interfering two time-delayed partial beams directly on a CCD camera. Wavelengths between λ=32  nm and λ=8  nm are examined. A decrease of the coherence time for the fundamental wavelengths from τ_{c}=(6±0.5)  fs at 32 nm to τ_{c}=(2.9±0.5)  fs at 8 nm is measured. At λ=8  nm the fundamental wavelength and the third harmonic of 24 nm are compared to each other. For 8 nm radiation as third harmonic of 24 nm a coherence time of τ_{c}=(2.5±0.5)  fs is observed. The spatial coherence of 24 and 8 nm fundamental pulses are found to be very similar. The visibility decreases to 50% of the maximum visibility at about 3.2 mm overlap of the partial beams, which corresponds to 42% of the beam diameter at a distance of 90 m from the exit of the undulator. These results are analyzed in terms of the Gaussian Schell model resulting in six contributing modes to the total radiation. In addition, the correlation of the visibility between the fundamental radiation at 24 nm and its third harmonic at λ=8  nm is investigated for identical shots.http://doi.org/10.1103/PhysRevSTAB.14.080701
collection DOAJ
language English
format Article
sources DOAJ
author S. Roling
B. Siemer
M. Wöstmann
H. Zacharias
R. Mitzner
A. Singer
K. Tiedtke
I. A. Vartanyants
spellingShingle S. Roling
B. Siemer
M. Wöstmann
H. Zacharias
R. Mitzner
A. Singer
K. Tiedtke
I. A. Vartanyants
Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime
Physical Review Special Topics. Accelerators and Beams
author_facet S. Roling
B. Siemer
M. Wöstmann
H. Zacharias
R. Mitzner
A. Singer
K. Tiedtke
I. A. Vartanyants
author_sort S. Roling
title Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime
title_short Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime
title_full Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime
title_fullStr Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime
title_full_unstemmed Temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime
title_sort temporal and spatial coherence properties of free-electron-laser pulses in the extreme ultraviolet regime
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2011-08-01
description The average temporal (longitudinal) and spatial (transverse) coherence of free-electron-laser pulses in the extreme ultraviolet at FLASH is measured by interfering two time-delayed partial beams directly on a CCD camera. Wavelengths between λ=32  nm and λ=8  nm are examined. A decrease of the coherence time for the fundamental wavelengths from τ_{c}=(6±0.5)  fs at 32 nm to τ_{c}=(2.9±0.5)  fs at 8 nm is measured. At λ=8  nm the fundamental wavelength and the third harmonic of 24 nm are compared to each other. For 8 nm radiation as third harmonic of 24 nm a coherence time of τ_{c}=(2.5±0.5)  fs is observed. The spatial coherence of 24 and 8 nm fundamental pulses are found to be very similar. The visibility decreases to 50% of the maximum visibility at about 3.2 mm overlap of the partial beams, which corresponds to 42% of the beam diameter at a distance of 90 m from the exit of the undulator. These results are analyzed in terms of the Gaussian Schell model resulting in six contributing modes to the total radiation. In addition, the correlation of the visibility between the fundamental radiation at 24 nm and its third harmonic at λ=8  nm is investigated for identical shots.
url http://doi.org/10.1103/PhysRevSTAB.14.080701
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