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10 - H1 - Desy

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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.

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