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Report on future detector requirements at ESRF

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Flux <strong>on</strong> <strong>detector</strong>:<br />

The flux <strong>on</strong> the <strong>detector</strong> is expected to be between 10 8 and 10 10 phot<strong>on</strong>s/s/mm 2 , depending<br />

<strong>on</strong> the energy. These values are smaller than the flux for other imaging beamlines because of<br />

two reas<strong>on</strong>s: ID17 uses <strong>on</strong>ly <strong>on</strong>e wiggler and the phot<strong>on</strong>s are spread over a larger beam.<br />

Particular oper<strong>at</strong>ing c<strong>on</strong>diti<strong>on</strong>s:<br />

Due to the use of high energy phot<strong>on</strong>s, radi<strong>at</strong>i<strong>on</strong> damage gener<strong>at</strong>es a very rapid blackening of<br />

the taper. Better radi<strong>at</strong>i<strong>on</strong> hardness would be appreci<strong>at</strong>ed.<br />

Required <strong>detector</strong><br />

Required <strong>detector</strong> is a large 2D rectangular <strong>detector</strong>, th<strong>at</strong> can be efficiently used <strong>at</strong> high<br />

energy.<br />

Existing <strong>detector</strong>s<br />

ID17 is currently using a FReLoN 2kx2k, with fibre optic taper and scintill<strong>at</strong>or.<br />

For the applic<strong>at</strong>i<strong>on</strong>s requiring less sp<strong>at</strong>ial resoluti<strong>on</strong> but more efficiency and speed, a Ge<br />

2-strip <strong>detector</strong>, with 350 µm pitch and 10 mm width, is used.<br />

Short term possibilities<br />

Structured CsI scintill<strong>at</strong>ors will be tested. The use of a FReLoN 4M instead of current<br />

FReLoN 2k will improve both dynamic range (by a factor 1.5) and quantum efficiency (65%<br />

efficiency <strong>at</strong> the Gadox emissi<strong>on</strong> wavelengths instead of 35%). Nevertheless, this will not<br />

directly permit to reduce the dose <strong>on</strong> the sample because in the case of taper coupling, where<br />

the light collecti<strong>on</strong> yield is high, the signal to noise r<strong>at</strong>io depends much more <strong>on</strong> the<br />

absorpti<strong>on</strong> coefficient of the scintill<strong>at</strong>or than <strong>on</strong> the quantum efficiency (see DQE formula in<br />

[Koch et al., 1998]). This means th<strong>at</strong> even if the total yield of the <strong>detector</strong> is increased, the<br />

SNR will not be proporti<strong>on</strong>ally improved.<br />

Main required improvements<br />

The main expected improvements c<strong>on</strong>cern the efficiency and the field of view <strong>at</strong> c<strong>on</strong>stant or<br />

better sp<strong>at</strong>ial resoluti<strong>on</strong>. Radi<strong>at</strong>i<strong>on</strong> hardness of optical couplings has to be improved.<br />

Other types of <strong>detector</strong>s<br />

MIA requires other 2D <strong>detector</strong>s (see pages 30, 32 and 39).<br />

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