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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.

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