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231225s2018 xx |||||o 00| ||eng c |
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|a 10.1107/S1600577517015442
|2 doi
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|a pubmed24n0931.xml
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|a (NLM)29271749
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|a DE-627
|b ger
|c DE-627
|e rakwb
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|a eng
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|a Zapolnova, Ekaterina
|e verfasserin
|4 aut
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|a THz pulse doubler at FLASH
|b double pulses for pump-probe experiments at X-ray FELs
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|c 2018
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|a Text
|b txt
|2 rdacontent
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|a ƒaComputermedien
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|2 rdamedia
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|a ƒa Online-Ressource
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|2 rdacarrier
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|a Date Revised 12.11.2023
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|a published: Print-Electronic
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|a Citation Status PubMed-not-MEDLINE
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|a FLASH, the X-ray free-electron laser in Hamburg, Germany, employs a narrowband high-field accelerator THz source for unique THz pump X-ray probe experiments. However, the large difference in optical paths of the THz and X-ray beamlines prevents utilization of the machine's full potential (e.g. extreme pulse energies in the soft X-ray range). To solve this issue, lasing of double electron bunches, separated by 28 periods of the driving radiofrequency (at 1.3 GHz), timed for the temporal overlap of THz and X-ray pulses at the experimental station has been employed. In order to optimize conditions for a typical THz pump X-ray probe experiment, X-ray lasing of the first bunch to one-sixth of that of the second has been suppressed. Finally, synchronization of THz radiation pulses was measured to be ∼20 fs (r.m.s.), and a solution for monitoring the arrival time for achieving higher temporal resolution is presented
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|a Journal Article
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|a FLASH
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|a THz beamline
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|a X-rays
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|a double electron bunches
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|a free-electron laser
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|a pump–probe experiments
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|a Golz, Torsten
|e verfasserin
|4 aut
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|a Pan, Rui
|e verfasserin
|4 aut
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|a Klose, Karsten
|e verfasserin
|4 aut
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|a Schreiber, Siegfried
|e verfasserin
|4 aut
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|a Stojanovic, Nikola
|e verfasserin
|4 aut
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|i Enthalten in
|t Journal of synchrotron radiation
|d 1994
|g 25(2018), Pt 1 vom: 01. Jan., Seite 39-43
|w (DE-627)NLM09824129X
|x 1600-5775
|7 nnns
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|g volume:25
|g year:2018
|g number:Pt 1
|g day:01
|g month:01
|g pages:39-43
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|u http://dx.doi.org/10.1107/S1600577517015442
|3 Volltext
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|d 25
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|e Pt 1
|b 01
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|h 39-43
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