The energy scales of the two silicon detectors were calibrated with 241Am sources, which were attached to the diffuser and hence could be removed during the muon beam measurements.
Figure 8.1 illustrates the calibration spectra for one of
the silicon detector (Si2) taken with the source. Measurement with no
target present in the system is shown in Fig. 8.1(a) which
had a full width half maximum resolution of about 40 keV. This is partly due
to the resolution of the source itself, and the detector resolution may be
better. The spectrum in Fig. 8.1(b), on the other hand, was
taken with 2 T,
or about 6.8 Ci of tritium
present (Target II-14 in Table 4.4 in
page
). The effect of tritium caused the peak width to
be about 65 keV, due to the
decay background.
Since energy spectroscopy is not the purpose of our experiments, the absolute energy scale was not very crucial. However, as we found in the thickness measurements in Section 3.3, the change in the detector temperature could cause significant variation in the energy gain, hence frequent calibration was performed to ensure the relative stability of the energy scale. In addition, the fusion signal itself, whose energy is well known, could provide the calibration information.
Figure 8.2 shows the position of the centroid of the peak
corresponding to 241Am for different calibration runs. The centroid
value was determined by Eq. 3.1 (page )
in a similar manner to the thickness measurements described in
Section 3.3 with the lower and upper cut off values 5300 ch
and 5600 ch, respectively. The error bars in the figure indicate
statistical uncertainties in the centroid. Changing the lower cut off value
to 5200 ch caused less than 3 ch change in the centroid, indicating the
systematic uncertainty in the calibration. The average of the measured
centroid values is 5486.9 ch (4.7 ch) for Si1 and 5473.5 ch (3.4 ch) for
Si2, respectively with the values in parentheses being the standard
deviation of 14 measurements. These should be compared to the weighted
average of 3 alpha lines of 241Am, 5491 keV (note that the peak energy
for the strongest line is 5486 keV). Assuming there is no
significant offset, which was confirmed by a test using a pulse generator,
the calibration is very close to 1 ch = 1 keV for both detectors.