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000000376 037__ $$aDESY-2013-00854
000000376 041__ $$aeng
000000376 088__ $$a1466
000000376 245__ $$aOptical-EUV Pump and Probe Experiments With Variable Polarization on the Newly Open LDM Beamline of FERMI@Elettra
000000376 260__ $$c2013
000000376 269__ $$a2013
000000376 502__ $$cBrookhaven National Laboratory
000000376 520__ $$aTwo color experiments are now available to users at the low-density matter beamline (LDM) operating at the Free Electron Laser (FEL) source FERMI@Elettra [1]. The seeded FEL method used at FERMI allows generation of high power, coherent pulses in the femtosecond regime, with a high level of shot-to-shot stability. Variable polarization is also available. LDM is dedicated to atomic, molecular and cluster physics. The LDM endstation,equipped with a velocity map imaging and a time-of-flight detector [2], is an ideal tool to characterize fast multiphoton processes. LDM was open to users in December 2012 and in February 2013 performed its firstpump and probe experiment on photoionization of atomic He and generation of spectral sidebands. The FERMI FEL-1 source, delivered EUV photons with several tens of microjoule per pulse (about 100 fs wide) in atunable wavelength range from 65 to 20 nm, while the 780 nm, optical pulses were from the same Ti:sapphire laser used to form the FEL seed pulse. This paper gives details about the pump and probe experimental setupand shows the straightforward use of the pump and probe data to measure the FEL pulse width.
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000000376 546__ $$aEnglish
000000376 690__ $$aExternal experiment
000000376 693__ $$0EXP:(DE-MLZ)External-20140101$$5EXP:(DE-MLZ)External-20140101$$eMeasurement at external facility$$x0
000000376 693__ $$0EXP:(DE-H253)XFEL-SQS-20150101$$1EXP:(DE-H253)XFEL-20150101$$5EXP:(DE-H253)XFEL-SQS-20150101$$6EXP:(DE-H253)XFEL-SASE3-20150101$$aXFEL$$eSQS: Small Quantum Systems$$fSASE3$$x1
000000376 7001_ $$0P:(DE-HGF)0$$aFinetti R. Borghes, P.$$b0$$eCorresponding author
000000376 7001_ $$0P:(DE-HGF)0$$aCallegari, C.$$b1
000000376 7001_ $$0P:(DE-HGF)0$$aCinquegrana, P.$$b2
000000376 7001_ $$0P:(DE-HGF)0$$aDanailov, M. B.$$b3
000000376 7001_ $$0P:(DE-HGF)0$$aDemidovich, A. A.$$b4
000000376 7001_ $$0P:(DE-HGF)0$$aFava, C.$$b5
000000376 7001_ $$0P:(DE-HGF)0$$aGerusina, S.$$b6
000000376 7001_ $$0P:(DE-HGF)0$$aGrazioli, C.$$b7
000000376 7001_ $$0P:(DE-H253)PIP1019912$$aIvanov, R.$$b8
000000376 7001_ $$0P:(DE-HGF)0$$aKurdi, G.$$b9
000000376 7001_ $$0P:(DE-HGF)0$$aLonza, M.$$b10
000000376 7001_ $$0P:(DE-H253)PIP1019968$$aMahne, N.$$b11
000000376 7001_ $$0P:(DE-HGF)0$$aNikolov, I.$$b12
000000376 7001_ $$0P:(DE-HGF)0$$aPivetta, L.$$b13
000000376 7001_ $$0P:(DE-HGF)0$$aPlekan, O.$$b14
000000376 7001_ $$0P:(DE-HGF)0$$aRaimondi, L.$$b15
000000376 7001_ $$0P:(DE-HGF)0$$aSigalotti, P.$$b16
000000376 7001_ $$0P:(DE-HGF)0$$aSvetina, C.$$b17
000000376 7001_ $$0P:(DE-HGF)0$$aZangrando, D.$$b18
000000376 7001_ $$0P:(DE-H253)PIP1011428$$aZangrando, Marco$$b19
000000376 7001_ $$0P:(DE-HGF)0$$aAvaldi, L.$$b20
000000376 7001_ $$0P:(DE-HGF)0$$aBolognesi, P.$$b21
000000376 7001_ $$0P:(DE-HGF)0$$aCoreno, M.$$b22
000000376 7001_ $$0P:(DE-HGF)0$$aO’Keeffe, P.$$b23
000000376 7001_ $$0P:(DE-HGF)0$$aDiFraia, M.$$b24
000000376 7001_ $$01623$$aIlchen, M.$$b25
000000376 7001_ $$01144$$aMazza, T.$$b26
000000376 7001_ $$01125$$aMeyer, Michael$$b27
000000376 7001_ $$01175$$aRafipoor, A. J.$$b28
000000376 7001_ $$0P:(DE-H253)PIP1008279$$aUeda, Kiyoshi$$b29
000000376 7112_ $$a35th International Free-Electron Laser Conference$$cNew York$$d2013-08-26 - 2013-08-30$$gFEL 2013$$wUSA
000000376 790__ $$aEuXFEL guest
000000376 790__ $$aEuXFEL staff
000000376 8564_ $$uhttp://www.c-ad.bnl.gov/fel2013/
000000376 8564_ $$s56021$$uhttps://xfel.tind.io/record/376/files/DESY-2013-00854.pdf$$yOpenAccess
000000376 8560_ $$fjulika.wagner@desy.de
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000000376 9141_ $$y2013
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000000376 961__ $$ajulika.wagner@desy.de$$c2016-01-06T12:52:11.434784$$i2013-09-26T16:22:36.360542$$x2013-09-26T16:05:02.441737$$z2016-01-06T12:52:11.434784
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