Author/Authors :
Raimondi، نويسنده , , L. and Svetina، نويسنده , , C. and Mahne، نويسنده , , N. and Cocco، نويسنده , , D. and Abrami، نويسنده , , A. and de Marco، نويسنده , , M. and Fava، نويسنده , , C. and Gerusina، نويسنده , , S. and Gobessi، نويسنده , , R. and Capotondi، نويسنده , , F. and Pedersoli، نويسنده , , E. and Kiskinova، نويسنده , , M. and De Ninno، نويسنده , , G. and Zeitoun، نويسنده , , P. and Dovillaire، نويسنده , , G. and Lambert، نويسنده , , G. and Boutu، نويسنده , , W. and Merdji، نويسنده , , H. and Gonzalez، نويسنده , , A.I. and Gauthier، نويسنده , , D. and Zangrando، نويسنده , , M.، نويسنده ,
Abstract :
FERMI@Elettra, the first seeded EUV-SXR free electron laser (FEL) facility located at Elettra Sincrotrone Trieste has been conceived to provide very short (10–100 fs) pulses with ultrahigh peak brightness and wavelengths from 100 nm to 4 nm. A section fully dedicated to the photon transport and analysis diagnostics, named PADReS, has already been installed and commissioned. Three of the beamlines, EIS-TIMEX, DiProI and LDM, installed after the PADReS section, are in advanced commissioning state and will accept the first users in December 2012. These beam lines employ active X-ray optics in order to focus the FEL beam as well as to perform a controlled beam-shaping at focus.
ng from mirror surface metrology characterization, it is difficult to predict the focal spot shape applying only methods based on geometrical optics such as the ray tracing. Within the geometrical optics approach one cannot take into account the diffraction effect from the optics edges, i.e. the aperture diffraction, and the impact of different surface spatial wavelengths to the spot size degradation. Both these effects are strongly dependent on the photon beam energy and mirror incident angles.
loyed a method based on physical optics, which applies the Huygens–Fresnel principle to reflection (on which the WISE code is based). In this work we report the results of the first measurements of the focal spot in the DiProI beamline end-station and compare them to the predictions computed with Shadow code and WISE code, starting from the mirror surface profile characterization.
Keywords :
Wavefront propagation , K–B mirrors , free electron laser , Fresnel diffraction