deltaT'(T0->PA) = Tpa' - Tt0' -TOFkstop -TOFsec > 0.8 (nsec) ,
after first stage PA/T0 time walk correction on Tpa/Tt0, i.e.Tpa' = Tpa - PAOFFSET(idrun)
andTt0' = Tt0 + T0OFFSET(idrun).
The arm-by-arm behavior of the Kmu2 peak under the event selection above is exhibitted below. Note that PA time walk is not corrected for PA-PB TOF below.
Now, we examine the 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
->delta T' (PA->PB) = Tpb - Tpa'-TOFkmu2
Note that we consciously keep old 1/beta to calculate deltaT (T0->PA).
Now, delta T(PA->PB)/delta T' (PA->PB) center and width are exhibitted and compared.
We activate the PB run-by-run, but arm-by-arm offset obtained here, and calculate the 1/beta by
1/beta (PA->PB) = (Tpb'-Tpa')*c/L_TOF
, where
Tpb' = Tpb - PBOFFSET(idrun).
PBOFFSET(idrun) is defined as the Gaussian center of the distribution of delta T' (PA->PB).
With this 1/beta definition, go back to T0->PA TOF analysis again.