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If the photon is reflected away from the detector, the cat is spared.
It may subsequently interact again at some other location or simply escape from the detector.
In any elastic-scattering interaction, the energy that is not transferred to the recoil nucleus is retained by the scattered neutron which, depending on the dimensions of the detector, may interact again or simply escape from the detector volume.
As shown in Table 1, from the detector perspective, there are three different types of symbols.
This indicates absorption and possibly scattering of light away from the detector.
In this paper, we summarize the system design and present characterization results from the detector modules.
The count from the detector was varied with the neutron incident angle due to the moderator.
Significant error, as large as 47%, was seen with the samples 140 mm from the detector.
Some of the preliminary results from the detector stack will also be highlighted.
The table includes the DOYs, when they occurred, and values of 〈k〉 computed from the detector data.
Also, from the detector perspective it is not possible to resolve the timing between arbitrarily close pulses.
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