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Report on future detector requirements at ESRF

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Standard diffracti<strong>on</strong> and 2D/3D diffracti<strong>on</strong> - mapping<br />

Project (Former BL) Applic<strong>at</strong>i<strong>on</strong><br />

UPBL0: NINA (ID22) Diffracti<strong>on</strong> and diffracti<strong>on</strong> mapping (2D/3D)<br />

UPBL11: TEXAS/EXAFS (BM29) Diffracti<strong>on</strong><br />

Aim of the detecti<strong>on</strong> system<br />

The aim of the detecti<strong>on</strong> system is to record 2D or 3D diffracti<strong>on</strong> maps in order to rec<strong>on</strong>struct<br />

images of polycrystalline samples and to measure diffracti<strong>on</strong> p<strong>at</strong>terns as complementary<br />

inform<strong>at</strong>i<strong>on</strong> to the main technique of the beamline (absorpti<strong>on</strong> spectroscopy, imaging) <strong>on</strong><br />

powders or single crystals.<br />

M<strong>on</strong>ochrom<strong>at</strong>ic<br />

beam<br />

Sample<br />

Detector<br />

Oper<strong>at</strong>ing c<strong>on</strong>diti<strong>on</strong>s and specific<strong>at</strong>i<strong>on</strong>s<br />

Energy range:<br />

The energy ranges from 15 to 60 keV. It is a m<strong>on</strong>ochrom<strong>at</strong>ic beam <strong>on</strong> both TEXAS\EXAFS<br />

and NINA, which will carry out diffracti<strong>on</strong> <strong>on</strong>ly <strong>on</strong> the “NA” branch (Nano-Analysis) of the<br />

beamline.<br />

Integr<strong>at</strong>i<strong>on</strong> time:<br />

Integr<strong>at</strong>i<strong>on</strong> times will range between tens of millisec<strong>on</strong>ds and few sec<strong>on</strong>ds. One goal is to<br />

follow chemical reacti<strong>on</strong>s or pressure evoluti<strong>on</strong> <strong>at</strong> the same time by diffracti<strong>on</strong> and<br />

spectroscopy, measuring <strong>on</strong>e diffracti<strong>on</strong> p<strong>at</strong>tern <strong>at</strong> the end of each absorpti<strong>on</strong> spectrum. This<br />

requires integr<strong>at</strong>i<strong>on</strong> and readout times comp<strong>at</strong>ible with the kinetics of the reacti<strong>on</strong>. Moreover,<br />

in order to perform 2D and 3D mapping efficiently, the readout time must be smaller or <strong>at</strong><br />

least not l<strong>on</strong>ger than the integr<strong>at</strong>i<strong>on</strong> time.<br />

Energy resoluti<strong>on</strong>:<br />

Energy resoluti<strong>on</strong> is not needed for this applic<strong>at</strong>i<strong>on</strong>.<br />

Sp<strong>at</strong>ial resoluti<strong>on</strong>:<br />

The sample-to-<strong>detector</strong> distance can be adapted to obtain the desired angular resoluti<strong>on</strong>. Pixel<br />

size between 50 and 150 µm and 2kx2k pixels would be c<strong>on</strong>venient. A an example, a 2D<br />

<strong>detector</strong> with 2kx2k pixels of 100 µm placed <strong>at</strong> 20 cm from the sample would let record<br />

reflecti<strong>on</strong>s up to θ=25 degrees with a resoluti<strong>on</strong> of about 1 mrad, which is similar to wh<strong>at</strong> is<br />

currently obtained.<br />

48

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