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DRAFT<br />

material is post processed, i.e. lapped down from 1 mm EG thick wafers by removing several<br />

hundreds of micrometers from the bad substrate side. These much more homogeneous<br />

DG-PC-CVDD films with a charge collection efficiency ≈ 65 % are available between 300 µm and<br />

600 µm thickness. In the next 2-3 years, (10 x 10) mm 2 SC-CVDD samples have been announced<br />

for sale. Intense R&D is going on to achieve areas as large as 2 inch wafers. All those prices<br />

mentioned above are forced at the time being by decisions which do not correspond to real production<br />

costs. It has been demonstrated that PC-CVD-DD operating with low-noise<br />

low-impedance broadband amplifiers are able to measure linearly heavy ion rates in a broad range<br />

from 1 Hz up to > 500 MHz by single particle readout of one detector channel. This value has been<br />

obtained with a detector of large capacitance of 8 pF and a scaler which limited the measurement<br />

due to its 500 MHz bandwidth. The s-p rate capability is higher for reduced strip capacitance and<br />

GHz electronics signal processing [21]. If two-dimensional position resolution on thin detectors is<br />

needed, crossed strips can be applied on opposite sides of the diamond substrate. Note, that although<br />

this type of detector is of high interest for different experimental groups and the expectations<br />

for a successful realization are good, no such a detector has been developed up to now at GSI.<br />

Thus, joined R&D e.g. with the Atomic Physics and R³B collaborations is foreseen. Figure 2.4.81<br />

shows the microscopic image of a pixel structure, which has been processed by sputtering a 1000 Å<br />

Si3N4 layer on a metallized surface. PC-CVDD micro-strip and micro-pixel detectors have been<br />

developed (Figure 2.4.82) and excessively tested by the RD42 Collaboration at CERN [22] (GSI is<br />

a member), striving for MIP tracking at high luminosity colliders.<br />

Figure 2.4.81: Pixel readout by Si3N4 - isolated micro tracks. Microscopic image of a pixel structure on a 1.3<br />

µm thick diamond membrane. The small pixels are (110 x 290) µm 2 and the large ones (400 x 400) µm 2 . The<br />

width of the tracks is 15 µm and their pitch is 30 µm.<br />

For fast micro-electrode readout providing a large dynamic range as needed for HI measurements<br />

no suitable ASIC exists yet. For CBM at FAIR solutions to readout the diamond start detector,<br />

which will be a (20 x 20) mm 2 micro-strip detector of a pitch of 50 µm at a strip width of 25 µm, are<br />

currently developed. The electronics would fit also for beam monitoring and tracking at <strong>Super</strong>-FRS.<br />

84

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