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As outlined in section 1,
the spectroscopic study of nuclei via transfer reactions in inverse kinematics
imposes severe constraints on the target thicknesses that can be used. This is
one of the key reasons for developing the TIARA array to take advantage of
gamma-ray detection. The next problem is how to
insert and replace targets when they are surrounded as much as possible by
charged-particle and gamma-ray detectors.
In the initial implementation of TIARA, the target materials are envisaged as
being fairly easy to manipulate, i.e. natural or deuterated polyethylene foils for
transfer, or nickel or lead foils for Coulomb excitation. In the longer term,
the planning should allow for the transfer of targets that have been stored in
vacuum such as 40Ca, which could be employed for studies along the N=Z
line with fusion-evaporation.
When the target thickness is a key parameter, as it is for transfer studies,
then the angle that it is mounted with respect to the beam must also be
important. Also, for Coulomb excitation experiments, the range of scattering
angles of interest will affect the choice of target angle. In some cases a
perpendicular orientation would be best, but in some cases the target could be
aligned for example with the angle at which the coverage of the annular detectors
and the barrel detectors meet.
Finally, it is never possible simply to put the beam down the beamline and do
an experiment. It is always necessary to focus, and often to perform runs with
a range of targets to characterise background reactions. The focussing can be
achieved in this case using a small blank aperture together with PPAC tracking
detectors and the zero degree telescope.
Thus, the TIARA design has been chosen to include a simple and reliable target
changer which operates with a rod. Space limitations mean that only one target
can be mounted at a time, but the target can be withdrawn on the rod into a
vacuum transfer cell, and replaced without breaking the vacuum in the target
chamber. Again for simplicity and reliability, the target enters the detector
barrel through a gap created by omitting one side of the octagonal barrel. This
also provides sufficient room to insert targets mounted on specially designed
tips for the rod, which allow any desired target angle to be employed.
Next: Gamma-ray detection
Up: No Title
Previous: Zero-degree telescope
Wilton Catford
2000-11-03