In the TaLL experiment, 68% of all the gamma-gamma events on tape were due
to 511 keV coincidences in the single pair of opposite detectors at
90
. This rate corresponds to an equivalent cross section of around
200 mbarns, which greatly exceeds the amount of beam stopped in the target
or scattered at 90
, and must be due to positrons from beam stopped
elsewhere in the chamber but annihilating in view of this pair of detectors.
It is useful to consider how this problem is changed when using a bigger
array such as Exogam, which has many more opposite pairs of detectors.
If A is the rate of annihilation in view of each pair of opposite detectors, and
there are
such pairs, then the rate of back-to-back coincidences is
, where
is the total absolute efficiency and
is the
intrinsic efficiency, equal to
divided by the geometrical factor
. Similarly, if R is the rate of reactions in the target,
with average multiplicity
, then with
detectors the
coincidence rate is
. The actual rate of reaction coincidences relative to
annihilation coincidences, R/A, is then modified in the data by an enhancement
factor given by