10 - H1 - Desy
10 - H1 - Desy
10 - H1 - Desy
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Chapter 7<br />
Calibration and tuning<br />
In this analysis MC is used to correct the detector level measurement to hadron level cross<br />
sections. For the correction being valid, MC events need to resemble data to high precision<br />
level and to ensure it, additional checks and calibrations explained in this chapter were<br />
performed. All the selection described in chapters 4 and 5, together with multivariate<br />
analysis introduced in chapter 6 were repeated with the corrected properties.<br />
The most influential tuning, being the check of the cluster shape description in MC is<br />
discussed in section 7.1. Sections 7.2 and 7.3 describe electromagnetic and hadronic<br />
energy calibrations. The method of direct and resolved relative scale tuning is explained<br />
in section 7.4.<br />
7.1 Cluster shapes tuning<br />
The multivariable analysis introduced in chapter 6 heavily relies on the proper description<br />
of the cluster shape variables in MC. A special effort was taken to tune the MC cluster<br />
shape simulation and to correctly evaluate systematic uncertainty associated with its<br />
description.<br />
Three data samples were used for the study of the cluster shape description:<br />
• BH electrons.<br />
The first sample is a selection of Bethe-Heitler (BH) electons produced in a process<br />
visualised with the diagrams presented in figure 7.1a and 7.1b. Events are selected<br />
with a scattered electron in the LAr calorimeter, identified as an electromagnetic<br />
cluster with a track pointing to it, a photon in the SPACAL and nothing else in the<br />
detector.<br />
• DVCS photons.<br />
The complementary sample to BH electrons is the selection of deeply virtual Compton<br />
scattering (DVCS) events with electron reconstructed in the SPACAL and a<br />
photon in LAr. The Feyman diagram of the DVCS event is pictured in figure 7.1c.