10 - H1 - Desy
10 - H1 - Desy
10 - H1 - Desy
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116 Cross section building<br />
8.4.3 Cross sections<br />
The output of the bin averaging procedure explained in section 8.4.1 is the final number<br />
of prompt photons N i measured in bin i. The error treatment associates with it a fully<br />
correlated error a i and a fully uncorrelated error δ i . The single differential cross section<br />
in bin i of variable x and double differential cross section in bin i of variable x and bin j<br />
of variable y is calculated with the formula<br />
( dσ<br />
dx ) i =<br />
( dσ<br />
dxdy ) i,j =<br />
N i<br />
L · w x,i<br />
±<br />
N i,j<br />
L · w x,i · w y,j<br />
±<br />
a i<br />
L · w x,i<br />
(corr.) ±<br />
a i,j<br />
L · w x,i · w y,j<br />
(corr.) ±<br />
δ i<br />
L · w x,i<br />
(uncr.) (8.40)<br />
δ i,j<br />
L · w x,i · w y,j<br />
(uncr.) (8.41)<br />
(8.42)<br />
where L is the integrated luminosity (see section 3.1) of the considered event selection<br />
(340 pb −1 ), and w x,i (w y,j ) is the width of i th (j th ) bin of variable x (y).<br />
The total cross section σ tot is determined for each unfolding by averaging over all the<br />
Signal Bins of ⃗x true within the phase space. Since it is a single number, and the error<br />
division into a correlated and uncorrelated error does not make sense, the total cross<br />
sections are quoted together with statistical error (averaged over the sum of E unf and<br />
E mc and systematic error (averaged over the sum of E i sys ).<br />
8.5 Total cross section consistency check<br />
The unfolding procedure has been repeated ten times, in order to calculate cross sections<br />
binned in different variables. Particularly, one of those unfoldings (A) leads to the inclusive<br />
prompt photon production cross sections, five (B, C, D, E, F) were performed<br />
in the exclusive photon plus jet phase space, two (G, H) in the direct enhanced phase<br />
space and two (I, J) in the resolved enhanced phase space. Different unfoldings in the<br />
same phase space produce the same cross sections projected on a different direction, so<br />
the comparison of the total cross sections can be treated as a consistency check.<br />
Figure 8.9 presents the comparison of the total cross sections in the exclusive phase space<br />
obtained with five different unfoldings. The inner error bars represent the statistical error<br />
while outer error bars statistical and systematic added in quadrature. The shaded area<br />
and horizontal lines indicate error ranges for the most precise and least complex unfolding<br />
B. The consistency of all obtained total cross sections increase the confidence level in the<br />
relatively complex method explained in this chapter.<br />
8.6 Toy Monte Carlo study<br />
The most common way of checking the quality of the unfolding procedure is a toy Monte<br />
Carlo study like the one presented in this section. The whole set of toy MC samples