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Results from the two analyses show general agreement. Larger
systematic errors are expected for aerogel radiators due to the lower
number of photons detected per event and the relatively large
background. The differences in the ratio of observed to predicted
photon yields which exist between the analyses, are used to assign a
systematic uncertainty. The systematic errors are determined in terms
of their effect on the mean ratio of observed to predicted photon
yields and are ascribed as follows :
- Photon counting - There are clearly substantial correlations
between the two analyses, hence the full
size of the differences is taken as the error on the mean ratio.
These vary from run to run, but on average are 4% for the gas data
and 10% for the aerogel data.
- Pedestal cut - A contribution
of 5% is added to cover the uncertainty in the effect of the
pedestal cut. This error is conservatively assigned to all samples,
although in principle it is less for the gas rings, where the fraction
of hit pixels with two or more photoelectrons is significant.
- Refractive indices - There is an uncertainty in the prediction
due to imprecise knowledge of the refractive indices. It is important
to note that variations in the number of produced photons with changes
in refractive index, are anticorrelated with the change in geometric
acceptance. Therefore the resulting error is relatively small.
Changes of
10% in (n - 1) are considered for all samples, and
the effect of alternative parameterisations of the chromatic
dependence are studied. All variations are found to lie within
2.5% of the number of observed photons.
- Acceptance and optical properties - Additional errors come
from knowledge of the absolute geometric acceptance and from the
modelling of the transmissions, reflectivity, aerogel clarity and
photocathode quantum efficiency. These are estimated to result in a
7% uncertainty.
The total systematic error from the sum of all sources is 13% for
the aerogel and 10% for the gas radiators.
Next: Discussion and detector response
Up: Estimates of the photon
Previous: Results from photon yield
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