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Report on future detector requirements at ESRF

Report on future detector requirements at ESRF

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Dynamic range:<br />

It is necessary to record the signal both before and after the absorpti<strong>on</strong> edge with a signal to<br />

noise r<strong>at</strong>io better than 10 3 , in order to detect correctly both pre-edge fe<strong>at</strong>ures and EXAFS<br />

oscill<strong>at</strong>i<strong>on</strong>s (with an amplitude down to 1% of the edge). After the edge, where the signal is<br />

the lowest, 10 6 phot<strong>on</strong>s/pixel are necessary to reach the required SNR of 10 3 .<br />

The intensity r<strong>at</strong>io Ibefore edge/Iafter edge can reach 1000 in the most absorbing samples (absorpti<strong>on</strong><br />

edge of 3 in the classical logarithmic represent<strong>at</strong>i<strong>on</strong>). Thus, the required dynamic range does<br />

not exceed 12 bits. Nevertheless, the sensitivity range of the <strong>detector</strong> must extend from<br />

10 6 phot<strong>on</strong>s/pixel (the lowest signals after edge, str<strong>on</strong>g absorpti<strong>on</strong> in sample and in sample<br />

envir<strong>on</strong>ment) up to more than 10 10 phot<strong>on</strong>s/pixel (for I0 measurement in the same acquisiti<strong>on</strong><br />

c<strong>on</strong>diti<strong>on</strong>s than the absorpti<strong>on</strong> spectrum).<br />

Linearity:<br />

For EXAFS, linearity is an important parameter, in particular for dichroism experiments, and<br />

the <strong>detector</strong> should be linear in the whole dynamic range.<br />

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

The flux <strong>on</strong> <strong>detector</strong> is expected to be of the same order of magnitude as it is now <strong>on</strong> ID24 or<br />

<strong>at</strong> maximum multiplied by 3. Th<strong>at</strong> is 10 8 to 10 13 phot<strong>on</strong>s/s <strong>on</strong> the whole <strong>detector</strong>, depending<br />

<strong>on</strong> the sample and sample envir<strong>on</strong>ment absorpti<strong>on</strong>. Due to the energy profile given by the<br />

undul<strong>at</strong>or, the intensity is not distributed uniformly <strong>on</strong> the <strong>detector</strong>: central pixels receive<br />

around 50 times more phot<strong>on</strong>s than border pixels.<br />

It is worth notice th<strong>at</strong> good quality EXAFS spectra can be obtained with 50 integr<strong>at</strong>i<strong>on</strong>s of<br />

100 ps each in the 4-bunch mode and th<strong>at</strong> equivalent d<strong>at</strong>a are expected with integr<strong>at</strong>i<strong>on</strong> times<br />

of few µs in the uniform mode.<br />

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

Direct detecti<strong>on</strong> would improve the overall efficiency of the system. In th<strong>at</strong> case, particular<br />

care should be taken c<strong>on</strong>cerning the radi<strong>at</strong>i<strong>on</strong> damage of the <strong>detector</strong>.<br />

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

The needed <strong>detector</strong> is a 1D device with short integr<strong>at</strong>i<strong>on</strong> time and fast readout. The use of a<br />

1D streak camera is envisaged in order to observe phenomena occurring in the dur<strong>at</strong>i<strong>on</strong> of a<br />

phot<strong>on</strong> bunch in stroboscopic mode.<br />

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

ID24 is currently using a setup composed of a scintill<strong>at</strong>or, a diaphragm and a FReLoN CCD<br />

camera, reading <strong>on</strong>ly 32, 64 or 128 of the 2048 available lines.<br />

Short term possibilities<br />

A collabor<strong>at</strong>i<strong>on</strong> is envisaged with STFC in order to customise and use a fast Ge microstrip<br />

<strong>detector</strong>. In th<strong>at</strong> case, the sp<strong>at</strong>ial resoluti<strong>on</strong> of the <strong>detector</strong> has to be increased for the highest<br />

part of the energy range: charge sharing seems to deterior<strong>at</strong>e the resulting energy resoluti<strong>on</strong> of<br />

the spectra.<br />

Main required improvements<br />

The main expected improvement c<strong>on</strong>cerns the detecti<strong>on</strong> speed (integr<strong>at</strong>i<strong>on</strong> and readout times).<br />

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