Diamond Detectors for Ionizing Radiation - HEPHY
Diamond Detectors for Ionizing Radiation - HEPHY
Diamond Detectors for Ionizing Radiation - HEPHY
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CHAPTER 8. DETECTOR GEOMETRIES 50<br />
300 V<br />
641 µm<br />
(a)<br />
0V<br />
1.0 1.5 1.75 2.0 r [mm]<br />
300 V<br />
0V<br />
641 µm<br />
(b)<br />
0V<br />
Figure 8.2: Cross-section of a diamond sample, showing potentials and the electric eld without<br />
(a) and with (b) a grounded guard ring.<br />
the digital (or, binary) resolution RMS of<br />
RMS dr =<br />
p p<br />
12<br />
: (8.1)<br />
When the strip pitch is small enough, charge sharing between two or more electrodes<br />
occurs, and together with proper analysis tools, the particle track can be reconstructed<br />
with much higher resolution than digital, depending primarily on the SNR. Using a silicon<br />
detector (300 m thick) with a strip pitch ofp=50m and a high-quality amplier (e.g.,<br />
the VA2), it is easy to obtain a spatial resolution of a few micrometers.<br />
8.2.2 Measurements<br />
When a diamond strip detector is measured in a test beam, the particle track is monitored<br />
with a number of high-resolution silicon strip reference detectors. Half of the reference<br />
detectors are rotated by 90 in order to obtain x and y position in<strong>for</strong>mation. A system of<br />
such detectors, shown in g. 8.3, is called \beam telescope". The RD42 telescope utilizes<br />
8 planes of silicon strip detectors with a pitch of50m, which are read out by VA2 chips.<br />
The intrinsic resolution of this telescope is approximately 1:5 m.