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Last modified: 2010-02-11

Beamlines at MAX IV

Workshop: February 22-23, 2010, Scandic Star, Lund, Sweden



Program
      Program Soft X-ray session
      Program Hard X-ray session
      Program Life Science session
Travel information
Map

Proposed beamlines for MAX IV
   Hard X-ray Beamlines
      New Proposals
      Reference group
   Soft X-ray Beamlines
      Reference group
   IR, UV and VUV Beamlines
   Ultrafast hard X-ray Beamline
Instructions for the Beamline Proposals
The MAX IV project

Registration (is closed)
 

New Proposals


Last modified: 2010-02-08

Microfocus X-ray Spectroscopy Beamline

The beamline is intended for high-resolution microfocus spectroscopy on samples in the energy range 3.5 - 25 keV. The beamline will facilitate resonant inelastic scattering (RIXS), non-resonant inelastic X-ray scattering (NIXS), resonant Raman spectroscopy (RRS), X-Ray Raman scattering (XRS), X-ray emission spectroscopy (XES), and high-resolution XANES/high-energy-resolution fluorescence-detected absorption (HERFD) spectroscopy.

Photon energy range
3.5-25 keV

Source
In-vacuum undulator

Monochromator
Heat-load monochromator with interchangeable Si (111) and Si (311) crystals, retractable high-resolution four-bounce post-monochromator with several sets of crystals

Energy resolution
ΔE/E ~ 10-4 (Si 111), ~ 10-5 (Si 311), ~ 10-6 (high-resolution monochromator)

Spot size
~150 x 300 µm2 (v x h)
Microfocus ~1x1 µm2 using KB mirrors

Polarization
Linear (circular with phase retarders)

Equipment
X-ray fluorescence spectrometer with five analyzer-crystals, rotatable to facilitate measurements at various momentum-transfer. Conventional and high-sensitivity fluorescence detectors. Sample chamber for in-situ measurements. Cryostat for measurements down to ~10 K.

Contact person
Sergei Butorin, Physics and Astronomy, Uppsala University



Last modified: 2010-02-15

X-ray Photon Correlation Spectroscopy


X-ray Photon Correlation Spectroscopy (XPCS) beamline at the 3GeV ring at MAX IV will be world leading thanks to outstanding specifications of the synchrotron source concerning emittance and brilliance. The low emittance results in an increase in the beam coherence with at least one order in magnitude. This leads to a significant improvement of the contrast in the experiment enabling studies of weakly scattering processes and systems, complex geometries and sample environments and smaller beam/sample sizes.

In XPCS the partial coherence of the X-ray beam is utilised to study dynamics in time domain by following the intensity fluctuation of the scattered light. The intensity-intensity autocorrelation function calculated from the scattering is directly related to the intermediate scattering function S(Q,t) reflecting the dynamics in the material. XPCS provides information on mesoscopic dynamics (~10-3 – 1 Å-1) over large time scales (10-8-103 s), a region not accessible by any other technique. Examples of research areas that can be addressed are: systems with a heterogeneous microstructure and/or dynamics, polymers, non-Newtonian fluids, colloids, liquid crystals, capillary waves polymer surfaces and of thin polymer films, protein and bio-membrane dynamics, charge density waves, and dynamic critical phenomena. Thus the user community is expected to include researchers from physics, chemistry, biotechnology, and biology.

A co-location of XPCS beamline with a coherent imaging/diffraction station could be of high interest forming a critical mass for exploitation of coherent X-ray scattering techniques at MAX IV.

Guiding beamline specifications:

Photon energy
5-12 keV

Source
undulator (possibly long in-vacuum)

Spot size
10-20 µm

Optics
Coherence preserving


Contact persons
Aleksandar Matic, Chalmers University of Technology
Yngve Cerenius, MAX-lab