Diamond Detectors for Ionizing Radiation - HEPHY
Diamond Detectors for Ionizing Radiation - HEPHY
Diamond Detectors for Ionizing Radiation - HEPHY
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Chapter 9<br />
Summary<br />
The possible application of radiation detectors based on CVD diamond has been demonstrated.<br />
Similar to semiconductor detectors such as silicon, the Bethe-Bloch and Landau<br />
theories are ecient tools to describe the behavior of diamond detectors.<br />
The polycrystalline structure of CVD diamond implies its inhomogeneity. A linear<br />
model over the detector thickness describes the relationship between local and average<br />
collection distances. This model satises experimental data. High quality CVD diamond<br />
is obtained by removing material with poor charge collection properties from the substrate<br />
side. The growth process has been successfully applied to grow large area detectors.<br />
Excellent progress has been achieved over the past years by the RD42 collaboration.<br />
The charge collection distance of diamond has been increased, now reaching 230 m (corresponding<br />
to 8300 e) with a sample 432 m thick and slightly more with thicker samples.<br />
A compact characterization station was built in Vienna, which has been successfully used<br />
<strong>for</strong> pulse height measurements. Due to my contribution and optimization, it has a very<br />
low noise gure (ENC = 270 e).<br />
Moreover, I was involved in the pion irradiation of CVD diamond samples, which was<br />
carried out by the <strong>HEPHY</strong> in the autumns of 1995, 1996 and 1997. I made essential<br />
contributions in preparation, realization and data analysis including further studies such<br />
as the calculation of electric eld distributions in diamond samples. In agreement with the<br />
linear model we could show that diamond samples with higher initial collection distance<br />
are more aected by irradiation than those with lower d c . Similar, we have demonstrated<br />
that the upper (Landau) tail of the signal distribution suers more from radiation than<br />
the low signal region, which remains almost unaected. This implies that the eciency<br />
of applications with a moderate threshold (a few thousand electrons) will be less aected<br />
by radiation than the mean value of the distribution.<br />
Furthermore, the radiation hardness of diamond has been demonstrated <strong>for</strong> all major<br />
particles. Simplifying the results of the irradiation experiments, diamond is expected to<br />
survive a hadronic uence of at least 10 15 particles cm ,2 , corresponding to the projected<br />
charged hadron uence at a radius of 7cm from the vertex in the LHC accelerator at<br />
CERN over 10 years. This is ten times more than present silicon detectors allow.<br />
<strong>Diamond</strong> micro-strip detectors were successfully tested with both slow (VA2) and<br />
fast (SCT128AHC) electronics. With the best diamond sample available, most probable<br />
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