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4.3 Triggering 57<br />

energetic tracks in the tracker. Subtriggers s82 and s83 were used. The exact definition<br />

for the s82 subtrigger has been changed in the year 2006 from demanding at least 3 tracks<br />

with p T > 400 MeV to at least one track with p T > 900 MeV. The change has been<br />

in charge from run 488289 on. The subtrigger s83 has been additionally verified by L2<br />

topological finder in order to detect D ∗ or di-jet events and was available until run 487915.<br />

Since the statistics of the alternative monitor sample is insufficient for a reliable determination<br />

of the trigger efficiency, the subtrigger s61, based on both SPACAL energy deposition<br />

(including the inner part of the calorimeter) and the tracker, has been included.<br />

Table 4.2 summarises the subtriggers used to determine the efficiency of s67. The overlap<br />

between two samples amounts to 50% of the main monitor sample.<br />

Subtrigger L1 Condition L2/L3 Condition<br />

Monitor<br />

Sample<br />

s0 E IET (outer) > 6 GeV R Spacal > 20 cm<br />

s3 E IET (outer) > 9 GeV R Spacal > 30 cm<br />

s9 E IET (outer) > 2 GeV R Spacal > 30(40) cm<br />

E ET6 > 3 GeV<br />

s82<br />

NTrack 400MeV > 2<br />

−<br />

Alternative<br />

Monitor<br />

Sample<br />

s83<br />

(NTrack 900MeV > 0)<br />

E ET6 > 3 GeV<br />

NTrack 400MeV > 2<br />

D ∗ or di-jet<br />

s61<br />

E IET (all) > 6 GeV<br />

NTrack 900MeV > 0<br />

−<br />

Table 4.2: Subtriggers definitions used for monitoring s67 trigger efficiency.<br />

The trigger efficiency has been evaluated for clusters passing the same cluster selection<br />

as used later in the main selection with the sole exception of the isolation criteria, which<br />

has been skipped altogether. A consistent usage of only highly isolated clusters decreases<br />

the statistics of monitor sample overall by 70% and particularly in forward direction by<br />

85% introducing a high error on fitted trigger efficiency. The possible bias due to missing<br />

isolation criteria has been studied and the results are compatible within statistical errors.<br />

The LAr trigger suffered during the HERA II running period from various localised hardware<br />

problems. In order to restrict the measurement to the well triggered events the<br />

trigger efficiency has been studied as a function of the variable zr defined as<br />

zr =<br />

{<br />

z<br />

r + 300 cm<br />

for CB1, CB2, CB3, FB1, FB2 LAr wheels<br />

for IE1 LAr wheel.<br />

(4.3)

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