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The photopeak gamma-ray efficiency depends acutely on the geometry employed.
TIARA is designed to be able to use the most close-packed of all the Exogam
geometries, called the ``gamma-cube''. The photopeak efficiencies for several
different geometries are included in Table 1. The
different shield configurations depend on whether the side shields on the
detectors are used, or not.
The maximum
value (at 662 keV) is 28% absolute photopeak efficiency.
Table 1:
Properties of the EXOGAM gamma-ray array in selected geometries using
just the 90 degree detectors (adapted from the project definition document).
The efficiency and resolution are quoted for 662 keV and the resolution is for
a source velocity of 0.075c. The quoted efficiency is for the true absolute
photopeak detection efficiency. Cube-A numbers (%,keV) are scaled from Cube-B results.
| |
Suppression |
Target |
Photopeak |
Energy |
| Geometry |
shield |
distance |
efficiency |
resolution |
| |
configuration |
(mm) |
(%) |
(keV) |
| |
|
|
|
|
| Gamma-Cube |
A |
50.3 |
28 |
15.5 |
| Cube |
B |
68.3 |
15 |
11.4 |
| 8 detectors |
A |
114.1 |
14 |
7.6 |
| |
|
|
|
|
Next: Doppler correction
Up: Gamma-ray detection
Previous: The Exogam Array
Wilton Catford
2000-11-03