deltaT'''(T0->PA) = Tpa'' - Tt0'' -TOFkstop -TOFsec' > 0.8 (nsec) ,
after second stage PA/T0 time walk correction on Tpa/Tt0, i.e.Tpa'' = Tpa' - PAOFFSET2(idrun)
andTt0'' = Tt0' + T0OFFSET2(idrun),
to study run-by-run behavior of the Kmu2 peak taking the PA time walk determined by T0-PA TOF analysis into account, namely,
delta T'' (PA->PB) = Tpb' - Tpa' -TOFkmu2 (centered at 0. by definition)
->delta T''' (PA->PB) = Tpb' - Tpa''-TOFkmu2
Note that TOFsec' is calculated with Tpb' and Tpa'.
Run-by-run behavior of delta T''' (PA->PB) center and width are exhibitted below.
We activate the second-stage run-by-run, but arm-by-arm PB offset, PBOFFSET2(idrun), and calculate the 1/beta by
1/beta (PA->PB) = (Tpb''-Tpa'')*c/L_TOF
, whereTpb'' = Tpb' - PBOFFSET2(idrun).
PBOFFSET2(idrun) is defined as the Gaussian center of the distribution of delta T''' (PA->PB).
Here, we go back to delta T(T0->PA) again. Now, Delta T''''(T0->PA) is defined by
deltaT''''(T0->PA) = Tpa'' - Tt0'' -TOFkstop -TOFsec'' ,
where TOFsec'' is now calculated from the 1/beta obtained above. Then, T0-by-T0/PA-by-PA deltaT''''(T0->PA) are as exhibitted below.
Here, we define the updated T0->PA time residual, delta T'''''(T0->PA), by
deltaT'''''(T0->PA) = Tpa''' - Tt0''' -TOFkstop -TOFsec''
, whereTpa''' = Tpa'' - PAOFFSET3(idrun)
andTt0''' = Tt0'' + T0OFFSET3(idrun).
T0->PA TOF resolution defined as the Gaussian sigma value of delta T'''''(T0->PA) distribution has been now converged, and T0/PA time offsets have been completely determined.