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Trends in the kinematics for transfer
To study transfer reactions with radioactive beams, it is necessary to
use inverse kinematics. The simplest transfer reactions to attempt in the
first instance are those induced by light particles as mentioned above: for
example, 1H and 2H nuclei. If `heavy ion' targets were used, then
an example would be 13C for neutron transfer.
Considering the hydrogen targets first, there is a general property of the
kinematics depending on whether a `pickup' reaction such as (p,d) or
a `stripping' reaction such as (d,p) is employed. In cases such as (p,d),
the light particle tends to be confined to the forward hemisphere in the
laboratory frame. In contrast, for reactions such as (d,p) the light products
tend to be concentrated in the backward hemisphere. Example calculations
are presented for a selection of (p,d), (d,p) and (d,3He) reactions,
in section 10 of this technical document.
For reactions using the `heavy ion' targets, the target-like reaction products
of interest tend to be emitted near 90 degrees in the laboratory. An
example calculation is given for a reaction on 13C in section
10.
In each case, the precise angular range of interest depends crucially on
the reaction Q-value, so it is not possible to give hard limits for the
angular ranges to be covered for each kind of reaction. Experience has
shown that there is some scope
in an individual experiment to adjust other experimental parameters
in order to work within a specified angular range, but this
is limited. Thus, in some experiments using p and d targets
the annular detectors will cover
sufficient of the
angular range for the transfer experiment, but in others
the Q-value and masses will conspire to spread the reaction products over a
wider range of angles.
For this reason,
the barrel part of the array is important for studying reactions on light
target nuclei, as well as for studying reactions on heavier
targets as already mentioned. In addition, the barrel makes it possible to design
experiments to study several different transfer channels simultaneously,
regardless of their different detailed kinematic focussing properties.
Next: Coulomb excitation near the
Up: Nuclear reaction kinematics
Previous: Energy resolution
Wilton Catford
2000-11-03