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The provisional design for the barrel around the target is shown in
figs. 1 and 2. As shown in fig. 2,
it envisages an octagonal box of silicon strip detectors with a length
of 142 mm and with the width of each detector being 36mm. Each detector will
have four resistive strips of width 9mm and length 140mm. The strips, which will run
axially, will automatically
offer measurement and pixellation of the azimuthal angle in 32 bins
of approximately 11 degrees. The measurement of the position along the strip for scattered
particles will be achieved by resistive division and should have a precision of
better than 0.4 mm. This will give the scattering angle to better
than one degree (limited by a 1 mm beam spot; better beam tracking would improve
this by a factor of between 2 and 4). Resistive strip detectors of this general
design have been used successfully by members of the TIARA team for over 8 years.
Edge-connector technology which exists already
will be able to deal with the extraction of the
signals from both ends of the detectors via one end of their mounting board.
One side of the barrel has been sacrificed
from the angular coverage in the present design. This is
because it is necessary to be able to insert and change targets during the
experiment. In view of the tight space constraints, a relatively simple
plunger mechanism for target changing has been chosen. A more sophisticated
remote controlled arrangement could be considered in the future, and may allow
the eventual completion of the barrel, but in the first stage this is not
included. This partly explains the specific choice of an octagonal geometry for
the barrel. It represents a balance between lost solid angle and the complexity of
building the barrel from many separate detectors and getting their signals out. The
other important reason for the octagonal choice is that it provides a good match between
the geometries of the charged particle detectors and the gamma-ray detectors.
Figure 2:
Strip detectors for TIARA: (a) the rectangular detectors each have 4
resistive strips and are single-sided, (b) they are arranged
with their long sides
touching to form an octagonal box, (c) the annular detectors are double-sided
6-inch wafers with annular strips at 1 mm pitch on one side and radial segments
on the other side
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Next: Annular detectors
Up: Silicon charged-particle detectors for
Previous: Elastically scattered radioactive beam
Wilton Catford
2000-11-03