S117 meeting, 25.7.95
ZDO
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If one plots the neighbour detector of an detector with unidentified line,
coincidences to the ULI look like punchtrough particles: a certain amount of
energy is missing. The particle penetrates the DE detector and is scattered in
the neighbour detector (ULI line: no DE).
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Wolgang suggests a check: detector without neigbours shouldn't show any ULI's.
Punchthroughs
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A new chi2 (robust) methode was applied to the search of the punchthrough
branch: no success.
- Uli wants to have a 2-dim fit: the angles of p and alpha-punchtroughs are
given by the energy loss in the silicon.
- Michael shows that the E projections give only little information about the
punchthrough-location.
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Burkhard shows offsets of the hodoscopes: he compares the offsets determined with
alpha-peak and pulser slope (~25#,large spread) and the offsets determined with
alpha-peak and proton-PT (~40#, small spread). Since the calibration is
meanwhile on the 20 keV level, one should take into account quenching effects of
the silicons. Low voltage silicons show larger quenching effects.
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Burkhard shows also a E-E plot for alphas from neighbouring detectors showing a
line at E1=E2 (Be8--> a+a (0MeV). Carsten produced a preliminary a-a correlation
showing this feature as a peak at the right relative momentum (20 MeV/c). The
correlation is still to low and has to be corrected for different possible
error sources.
Italians
Givanni and 2 collaborators will help this week Burkhard with the energy
calibration.
July 25th, 1995 Carsten Schwarz,