First we looked how efficient the generated single muons are reconstructed by
the RPC and DTBX trigger systems with respect to their kinematical variables
,
and
. In fig. 2 we plot the ratio of
reconstructed to generated tracks as a function these variables.

Obviously in the regions of
and
both RPC and DTBX show inefficiencies. Geometrically this corresponds to
crack positions, where two wheels carrying RPC and DTBX chambers are
fitted together. For
> 0.8 a rather different behaviour for DTBX
and RPC is observable. In this regime obviously the overlap region to
the forward muon system starts to be important especially for the DTBX system,
since no CSC information was included in this study.
Similarly we find inefficiencies in
, which appear every 30 degrees
reflecting the setup of the detector planes.
On the other hand we do not observe a strong
dependence of the trigger
efficiency. DTBX has a slightly higher trigger efficiency compared to
RPC, but has clearly losses in the low-
region < 10 GeV/c.
Therefore in fig. 3 the
dependence of the efficiency is
separately plotted for our small sample of low
muons.
To put our analysis of both trigger systems on a comparable footing we restrict
our analysis to the region of
< 0.8.
In table 3 we calculated the overall capability of
the two trigger systems to reconstruct muons in this restricted
regime.
RPC will find in 95.5% and DTBX in 93.2% of the cases one muon from one
generated, but for 4.5% and 3.6% of the tracks the reconstruction fails.
More than one muon (e.g. ghost tracks) are found by RPC in 0.02% of the generated single muon events, but by DTBX with a much higher percentage of 3.3%, which is a reflection of the left/right ambiguity of the DTBX system and needs careful investigation to avoid problems at higher muon multiplicities.
The charge of the generated muons is incorrectly reconstructed in about 4% of
the cases for both RPC and DTBX. The probability for such misassignments
increases with higher
and can be attributed to
reconstruction
problems. This occurs in the critical (i.e. less efficient)
regions (1.,
0.75, 0.2), where the input
spectra get distorted during reconstruction.
Either the reconstructed transverse momenta for muons with a wrong charge
assigned are very low ( < 30 GeV/c) for DTBX or very (100 GeV/c) for the
RPC.