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10 - H1 - Desy

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1.5 Analysis motivation and goals 27<br />

variables are estimators of the longitudinal momentum fractions carried by the parton<br />

which enter the hard interaction from the proton side x and from the photon side x γ ,<br />

already introduced in section 1.2. These leading order definitions of the estimators do<br />

not use the energy of the jet. The latter is expected to be reconstructed with relatively<br />

low resolution and thus the leading order estimators yield a higher correlation between<br />

the generated and reconstructed levels. The usage of the variable x LO<br />

γ is recommended<br />

in [49,50] to reduce infrared sensitivity. The variable x LO<br />

p is discussed e.g. in [51]. The<br />

accompanying hadronic jet is required to be within the pseudorapidity range of −1.3 <<br />

η jet < 2.3 and has the transverse energy above 4.5 GeV. The asymmetric energy cut on<br />

the photon and the jet is required to ensure the validity of the NLO calculation [49,52,53]<br />

The prompt photon phase space with additional jet requirement is later on referred to as<br />

exclusive or photon+jet phase space.<br />

Another interesting measurement is the study of the transverse correlations between the<br />

prompt photon and the accompanying jet. For direct events in leading order and at<br />

sufficiently low Q 2 , the measured acoplanarity is directly sensitive to the transverse momentum<br />

k T of the parton entering the hard interaction. The mentioned effect can be<br />

studied using two variables ∆Φ and p ⊥ defined as<br />

p ⊥ ≡ |⃗p γ<br />

T<br />

× ⃗p<br />

jet<br />

T<br />

|<br />

|⃗p jet<br />

T<br />

|<br />

= E γ T<br />

· sin∆Φ. (1.42)<br />

and sketched in the transverse plane 5 in figure 1.22.<br />

p<br />

γ<br />

T<br />

p<br />

∆Φ<br />

Transverse plane<br />

p<br />

jet<br />

T<br />

Figure 1.22: Definition of the variables ∆Φ and p ⊥<br />

between prompt photon and the leading jet.<br />

used to study the correlations<br />

The azimuthal acoplanarity between the photon and the jet ∆Φ and the photon momentum<br />

perpendicular to the jet direction p ⊥ were chosen such as to avoid usage of the jet<br />

energy measurement and thus minimising the potential degradation of the resolution. If<br />

the jet perfectly balances the photon candidate, p ⊥ is equal to zero and ∆Φ is equal to<br />

5 For a definition of the transverse plane the reference system is needed. It is introduced in section 3.2<br />

where transverse plane is also defined.

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