10 - H1 - Desy
10 - H1 - Desy
10 - H1 - Desy
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144 Conclusions and outlook<br />
is consistent with the one made in the previous <strong>H1</strong> publication [35]. The improvement can<br />
be associated with the lower NLO corrections in the exclusive case, which may suggest<br />
that the higher order corrections for inclusive prompt photon cross sections may still be<br />
significant.<br />
The cross sections in bins of x LO<br />
γ and x LO<br />
p variables were also measured and found to be<br />
consistent with the predictions within errors.<br />
Correlation between the prompt photon and the hadronic jet were studied in the part<br />
of the phase space with enhanced contribution from direct events (x LO<br />
γ > 0.8) and the<br />
complementary one (x LO<br />
γ < 0.8). In both cases, the predicted rate of events with the<br />
photon not being fully balanced by the leading hadronic jet is below the measured cross<br />
sections. Higher order corrections are expected to introduce additional imbalance, possibly<br />
improving the calculations. The fraction of events in the tails of the studied distributions<br />
may also be increased by introduction of the additional intrinsic 〈k T 〉 of the partons<br />
entering the hard interaction. The comparison of the measured cross sections in the<br />
direct enhanced phase space with the QCD calculations corrected for the 〈k T 〉 effects<br />
leads to the conclusion that though the improvement is clearly visible, the intrinsic 〈k T 〉<br />
can not solely remove the observed discrepancy.<br />
The difference in the azimuthal angle between prompt photon and the accompanying jet<br />
∆Φ in the exclusive phase space with additional requirement x LO<br />
γ < 0.8 shows vulnerability<br />
of the FGH calculation. The back-to-back region, ∆Φ → 180 ◦ , is sensitive to multiple<br />
soft gluon radiation which limits the validity of fixed order calculations. The LZ calculation<br />
includes multiple gluon radiation in the initial state before the hard subprocess and<br />
describes problematic region significantly better.<br />
The prompt photon measurement presented in this thesis may still be improved. Most<br />
significantly, higher statistics of monitor sample which consists of pure photons is needed<br />
to improve the cluster shape description and decrease the leading systematic error. The<br />
limited statistics of deeply virtual Compton scattering events in the kinematic range of<br />
this analysis demands finding more suitable source of the photon monitor sample. The<br />
errors of this measurement are low enough to resolve the deficits in the QCD calculations<br />
applied for the comparison.<br />
The conclusions drawn from this study may become stronger by improving the theoretical<br />
understanding of the prompt photon production. Especially, better understanding of the<br />
hadronisation model would help in decreasing the error of the predictions. The new parton<br />
density functions coming from combined <strong>H1</strong> and ZEUS data will help with calculation of<br />
more precise predictions. The sizeable NLO corrections lead to the conclusion that higher<br />
orders should be investigated in future. The box diagram, significantly contributing to<br />
the prompt photon cross sections, on the level of <strong>10</strong>%, should be taken into account in all<br />
the calculations, as well as contribution from the quark-to-photon fragmentation function.<br />
The latter should also be studied in more details.