XANES, EXAFS, myXANES, myEXAFS
The KMC-2 XANES is a dedicated endstation to investigate the short-range environment around selected atomic species in condensed matter by X-ray Absorption Spectroscopy. This end-station provides possibility for EXAFS, XANES and X-ray fluorescence measurements at-air. The detector system consists of three ionization chambers, Si-PIN photodiode, energy-dispersive detector (Bruker X-Flash 6|60) and scintillation counter. The experimental setup allows for a parallel monitoring of the transmitted through the sample X-ray beam intensity as well as for fluorescence yield measurements. This end-station is permanently attached to the KMC-2 beamline providing medium photon flux between 4000 eV and 15000 eV and linear photon polarization, necessary to exploit the potential of X-ray absorption spectroscopy.
Assigned to beamline(s)
|KMC-2||4 - 15 keV|
|Temperature range||293 K|
|Pressure Range||For details contact the station manager.|
|Detector||Bruker X-Flash 6|60, 3 ionization chambers, Si-PIN photodiodes|
|Sample holder compatibility||For details contact the station manager.|
|Beam intensity stabilization||MOSTAB electronics (accuracy 0.3%)|
|Microfocusing||> 5 μm|
|Micro-EXAFS, micro-fluorescen||limited / no mapping|
|Maximum sample size||unlimited|
|Control system||PC-based BESSY monochromator control system EMP/2|
|Data-acquisition computer||Personal computer, measurement bus-extension, OS/2-operating system|
|Data-acquisition software||Windows-NT, RADICON RDPW software|
X-ray Absorption Spectroscopy (XAS) is a powerful structural technique to investigate the short-range environment around selected atomic species in condensed matter. While scanning the x-ray energy impinging onto the sample, a core level photoelectron is generated. This is scattered by the surroundings matter producing interference effects visible in the absorption cross-section and usually referred to as x-ray absorption fine structure (XAFS). The process itself is general and therefore fundamental to study structural properties in materials like:
• liquids, molecular solutions, liquid crystals;
• single- and poly-crystalline materials;
• amorphous and highly disordered solids;
• molecules and macromolecules containing metallic atoms or partially substituted with heavy atoms.
The energy range 4.0 keV < E < 15 keV is sufficient for K-edge studies of elements in the range 21 < Z < 36 and L-edge studies of elements in the range 49 < Z < 83. The sample thicknesses for experiments are in the µm range for transmission experiments. However, thin film and/or dilute systems studies are still possible in fluorescence mode.