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Methoden und Instrumentierung Poster: Mi., 14:00–16:30 M-P87<br />

The Variable Polarization XUV Beamline at PETRA III<br />

Jens Viefhaus 1<br />

1 HASYLAB bei DESY, Notkestr. 85, 22607 Hamburg<br />

The 6 GeV energy of the storage ring PETRA III (DESY, Hamburg) together with<br />

its very low e<strong>mit</strong>tance of 1 nm rad makes it an excellent facility to host a Variable<br />

Polarization XUV Beamline. The high brilliance and flux of the beamline provided<br />

in a broad photon energy range (200 eV to 3000 eV) will open up completely new<br />

scientific opportunities in fields like:<br />

A. Spectromicroscopy<br />

B. High resolution photoelectron spectroscopy<br />

C. Soft X-Ray scattering<br />

D. Magnetic studies E. Gas phase targets<br />

F. Surface Chemistry<br />

Key absorption edges of practically all important elements lie in the range of photon<br />

energies provided by the beamline which creates the possibility to uniquely determine<br />

the element-specific local electronic structure in complex materials by exploiting atomic<br />

resonances.<br />

In the future polarization-dependent studies with soft X-rays will play a key role in<br />

enhancing our knowledge of the structure of matter. The source of the beamline will<br />

be a 5 m APPLE-II-type undulator (65.6 mm period) allowing full polarization control<br />

by the user. The undulator can operate over the whole photon energy range in the<br />

first harmonic thereby simultaneously providing high flux and complete polarization.<br />

Using current technology it is possible to achieve a spectral resolving power of more<br />

than 10000 at 1 keV with an extremely high flux (more than 10 12 photons/sec) focused<br />

on the sample.<br />

Special attention will be paid to provide both small focal spot size as well as high<br />

photon flux required by the different user communities.<br />

Together with the main source parameters a detailed layout of the beamline will be<br />

presented.<br />

User operation of the beamline will start in 2009 right after the startup phase of<br />

PETRA III.

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