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Deutsche Tagung f ¨ur Forschung mit ... - SNI-Portal

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Methoden und Instrumentierung Vortrag: Do., 11:30–11:50 D-V43<br />

Wavefront Studies at the Free-Electron Laser FLASH<br />

Elke Plönjes 1 , Marion Kuhlmann 1 , Sven Toleikis 1 , Philippe Zeitoun 2 ,<br />

Julien Gautier 2 , Thierry Lefrou 2 , Denis Douillet 2 , Pascal Mercere 3 , Guillaume<br />

Dovillaire 4 , Marta Fajardo 5<br />

1 HASYLAB at DESY, Notkestr. 85, D-22603 Hamburg, Germany – 2 Laboratoire<br />

d’Optique Appliquee, ENSTA, Chemin de la Huniere, F-91761 Palaiseau cedex, France<br />

– 3 Synchrotron SOLEIL, L’Orme des Merisiers - Saint-Aunin - BP 48, 91192 Gif-sur-<br />

Yvette Cedex, France – 4 Imagine Optic, 18 rue Charles de Gaulle, Orsay France 91400,<br />

France – 5 Centro de Fisica dos Plasmas, Institutio Superior Tecnico, Av. Rovisco Pais,<br />

1049-001 Lisboa, Portugal<br />

The Free-Electron Laser in Hamburg (FLASH) is operated in the “self-amplified spontaneous<br />

emission” (SASE) mode and delivers sub-picosecond radiation pulses, with<br />

gigawatt peak powers. At present, lasing has been observed down to about 13 nm<br />

in the fundamental, the shortest wavelength ever achieved with a free electron laser.<br />

User experiments started in August 2005 and were carried out between 45 nm and 13<br />

nm. For these wavelengths, FEL pulse intensities from typical 5 µJ up to more than<br />

50 µJ have been obtained with pulse lengths between 20 and 50 fs. FEL wavefronts<br />

observations have been recorded using a Hartmann sensor (by Imagine Optic). The<br />

Hartmann principle is based on a pinhole array, which divides the incoming beam into<br />

a large number of sub-rays monitored in intensity and position of individual spots.<br />

The identification of the local slope of the incident wavefront makes the aberrations<br />

from a perfect spherical wavefront visible. Ray tracing backwards accesses the beam<br />

focal point in size and position. The intense and coherent vacuum-ultraviolet FEL<br />

beam of various repetition rates leads to unique requirements for the wavefront sensor<br />

setup. The wavefront studies were carried out in the context of commissioning of<br />

the experimental stations. A further goal is to provide an online diagnostic tool for<br />

experiments which need to determine beam parameters which can vary with the shot<br />

to shot characteristic of the FEL, e.g. the focal spot size. We report measurements of<br />

the metrology of flat and curved mirrors at FLASH beamlines. The effects of solid and<br />

gaseous filters are selectively described in the wavelength regime of 10 nm to 32 nm.<br />

The use of wavefront measurements to provide reliable machine parameter is discussed.<br />

The wavefront sensor proved to be a valuable tool to determine the FEL beam quality<br />

and the performance of optical elements, filters and diagnostic tools.

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