24.08.2013 Views

Report on future detector requirements at ESRF

Report on future detector requirements at ESRF

Report on future detector requirements at ESRF

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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

Point <strong>detector</strong>s will c<strong>on</strong>tinue to be used but 2D <strong>detector</strong>s can be useful for small angle<br />

sc<strong>at</strong>tering and for the study of dynamic structures (q dependence of the diffracti<strong>on</strong> p<strong>at</strong>tern). In<br />

most cases, a sp<strong>at</strong>ial resoluti<strong>on</strong> of 100 µm would be c<strong>on</strong>venient.<br />

Efficiency:<br />

To reach the desired time resoluti<strong>on</strong>, APDs are used. In order to improve the detecti<strong>on</strong><br />

efficiency <strong>at</strong> high energies, the APD can be chosen thicker and/or tilted to increase the<br />

effective thickness seen by the phot<strong>on</strong>s. Nevertheless, this has two drawbacks. First, if the<br />

<strong>detector</strong> chip collects more phot<strong>on</strong>s, it can s<strong>at</strong>ur<strong>at</strong>e the electr<strong>on</strong>ics. Sec<strong>on</strong>d, in thick diodes,<br />

the time of propag<strong>at</strong>i<strong>on</strong> of the electr<strong>on</strong>s is not negligible compared to the studied time<br />

structures. Thus, <strong>on</strong>e loses time resoluti<strong>on</strong>, which is even worse <strong>at</strong> high energies than <strong>at</strong> lower<br />

<strong>on</strong>es because the lifetime is shorter.<br />

In order to avoid those drawbacks, the efficiency is increased by stacking several diodes <strong>on</strong>e<br />

behind the other and by synchr<strong>on</strong>izing the corresp<strong>on</strong>ding electr<strong>on</strong>ics.<br />

Dynamic range and linearity:<br />

The <strong>detector</strong> must be able to count single phot<strong>on</strong>s as well as support the high intensity of the<br />

prompt pulse (10 10 to 10 11 phot<strong>on</strong>s/s). It can be noticed th<strong>at</strong> measuring the intensity of the<br />

prompt pulse is not needed and th<strong>at</strong> the signal can be g<strong>at</strong>ed so th<strong>at</strong> it does not reach the<br />

counter.<br />

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

The expected flux <strong>on</strong> the <strong>detector</strong> can reach 10 11 phot<strong>on</strong>s/s in the prompt pulse (th<strong>at</strong> is<br />

70 000 phot<strong>on</strong>s in the pulse) and ranges from 0.01 phot<strong>on</strong>/s to 10 5 phot<strong>on</strong>s/s in the delayed<br />

signal.<br />

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

The <strong>detector</strong> is oper<strong>at</strong>ing near magnetic fields. Intents have been made to put it inside the<br />

cryost<strong>at</strong> in order to increase the detecti<strong>on</strong> solid angle. Even if up to now the low temper<strong>at</strong>ures<br />

have disturbed the avalanche process in the diodes, the eventuality can be kept in mind.<br />

The <strong>detector</strong> is mounted <strong>on</strong> a diffractometre arm.<br />

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

The required <strong>detector</strong> must be fast, with high count r<strong>at</strong>e, good time resoluti<strong>on</strong> and be capable<br />

of making a very fast recovery after high flux exposure.<br />

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

The current <strong>detector</strong>s are APDs c<strong>on</strong>nected to fast electr<strong>on</strong>ics: (amplifier, c<strong>on</strong>stant fracti<strong>on</strong><br />

discrimin<strong>at</strong>or, time to amplitude c<strong>on</strong>vertor and then ADC and MCA to record the signal).<br />

For the highest energies, up to 24 APDs are staked in order to improve the efficiency.<br />

Short term possibilities<br />

The chosen technology is likely to remain APD, with improved electr<strong>on</strong>ics. Projects for<br />

developing 1D and 2D APD arrays are starting (XNAP project).<br />

Main required improvements<br />

The main expected improvement c<strong>on</strong>cerns first the ability of the electr<strong>on</strong>ics to resolve high<br />

count r<strong>at</strong>es very rapidly. Then, the aim is to have 2D <strong>detector</strong>s using the same technology.<br />

18

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!