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Report on future detector requirements at ESRF

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of projecti<strong>on</strong>s. A dynamic range larger than 13 bits is needed for 2k pixels and it grows as √N<br />

as the number of pixels increases.<br />

The scintill<strong>at</strong>or resp<strong>on</strong>se should not degrade the required dynamic range (afterglow effects,<br />

emissi<strong>on</strong> from substr<strong>at</strong>e).<br />

Linearity:<br />

The devi<strong>at</strong>i<strong>on</strong> from linearity should be less than 0.5% <strong>on</strong> the whole dynamic range (current<br />

value is better than 2% with the FReLoN camera).<br />

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

The flux for imaging is typically 10 10 to 10 13 phot<strong>on</strong>s/s/mm 2 . The absolute maximum <strong>on</strong><br />

<strong>detector</strong> is estim<strong>at</strong>ed to 10 15 phot<strong>on</strong>s/s/mm 2 (flux obtained <strong>on</strong> ID22 with present<br />

c<strong>on</strong>figur<strong>at</strong>i<strong>on</strong> in pink beam – should be less <strong>on</strong> NINA, which will be l<strong>on</strong>ger).<br />

Other comments:<br />

D<strong>at</strong>a acquisiti<strong>on</strong> and storage: D<strong>at</strong>a correcti<strong>on</strong> and compressi<strong>on</strong> techniques built in the<br />

<strong>detector</strong> may be useful. D<strong>at</strong>a compressi<strong>on</strong> may even present losses provided th<strong>at</strong> they are well<br />

defined and adapted to quantit<strong>at</strong>ive volume imaging.<br />

Radi<strong>at</strong>i<strong>on</strong> hardness and stability: In certain cases, the <strong>detector</strong>s will need to oper<strong>at</strong>e under<br />

heavy irradi<strong>at</strong>i<strong>on</strong> and he<strong>at</strong> load c<strong>on</strong>diti<strong>on</strong>s. Both scintill<strong>at</strong>ors and optics may need to be stable<br />

and radi<strong>at</strong>i<strong>on</strong> tolerant, even compromising performance in some cases.<br />

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

ID19, ID22 and ID22NI are currently using FReLoN cameras with scintill<strong>at</strong>ors and several<br />

optical couplings giving pixel sizes from 0.2 µm to 30 µm.<br />

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

Required <strong>detector</strong> is a 2D sensor coupled via optical set-up to scintill<strong>at</strong>or. The c<strong>on</strong>cept of<br />

FReLoN camera as general-purpose camera is extremely c<strong>on</strong>venient: same imaging sensor for<br />

all optical c<strong>on</strong>figur<strong>at</strong>i<strong>on</strong>s.<br />

Main required improvements<br />

The main expected improvements are efficiency, both in detecti<strong>on</strong> and time (read out as well<br />

as fast shuttering scheme to shorten the smallest possible exposure time). Then, the number of<br />

pixels, i.e. the field of view for a given sp<strong>at</strong>ial resoluti<strong>on</strong>, should be increased, preserving<br />

other specific<strong>at</strong>i<strong>on</strong>s. Expected improvements are summarised below:<br />

Short<br />

term<br />

Medium term L<strong>on</strong>g term<br />

Parameter Efficiency<br />

Efficiency<br />

+ Field of View<br />

Efficiency + Field of View<br />

+ Speed<br />

DQE 50% <strong>at</strong> 20 keV with 1µm resoluti<strong>on</strong><br />

Number of pixels 4kx4k 8kx8k<br />

Dynamic range > 13 bits (imposed by tomography needs)<br />

> 95% @ 100ms exposure<br />

Duty cycle<br />

mechanical shutter<br />

impossible<br />

Maximum frame<br />

> 1000 fps for 1kx1k pixels<br />

r<strong>at</strong>e<br />

> 100 fps for 8kx8k pixels<br />

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