The information below covers D0 muon ID. A FINAL PAPER was published in 2013 in NIM covering the effort from 1998-2013.
This we page gives an overview of Run II muon identification, including a brief description of the detector,coverage, trigger, and expected resolutions. Also, some comparisonsto the Run I muon ID will be included, as will some discussionsof backgrounds. Preliminary descriptions of offlinealgorithms and analysis tools are also given along with a pointer to software documentation.
Muon reconstruction utilizes the inner tracking, thecalorimeter, and the muon detector elements themselvesto identify muons and determine their energy.
The following figures show the central and forward muon detector eta and phi coverage .Detector coverage will be almost complete for high pt muons,with more than 75% hitting at least 2 layers and more than 90%hitting at least 1 layer (at |eta|<2). For A-layer muons, thereis no coverage for phi from 225 to 315 degrees for |eta|<1giving a geometric acceptance of about 85%.
The detector thickness is in the range 5-9 interaction lengthsin the calorimeter, and 7-9 in the iron. The thickness is shown in:Thickness versus Theta .The plot indicates the thin spots at the CC-EC and CF-EF gaps. Itdoes not show the thin spot at phi=110 degrees in the central (dueto the main ring pipe) or the small loss of material on the bottomfor cables. Energy loss follows thickness, with 1 interaction lengthin the calorimeter or iron equivalent to 0.25 or 0.23 GeV/c energy lossrespectively. This gives a minimum energy of about 1.6 GeV for a muon to exitthe calorimeter, and about 3.3 GeV to exit the iron.
The main weapons in reducing the L1 trigger rate come from matchingmuon detector hits to L1CFT tracks, imposing a timing window ( of about15-20 ns) to define scintillator hits, and forming centroids from wire detector hits in different planes.
There are two types of triggers formed for each octant that wecall MTC05 and MTC10 for historical reasons. MTC05 triggers match tracksfrom the L1CFT to corresponding scintillator hits in muon detector. The L1CFT tracks include PT and sign information. The scintillator hits aredefined by having their times satisfying a modest time window (sigma = 20ns)about the expected time for a prompt muon from collisions. Scintillatorhits can come from one layer or as correlations of hits between layers.MTC10 triggers match centroids (stubs) formed from hits in the muon wire detectors with hits in the scintillator counters. Centroids can come from a single layer or as correlations of centroids between layers. MTC05triggers are primarily triggers in phi and MTC10 triggers are primarilytriggers in eta. Both can be used to define a good octant trigger.
L1MU triggers can be user-defined using PT (four thresholds), region (|eta| < 1.0, 1.5, or 2.0), wire and scintillator quality (none, loose,or tight), and (for dimuons) sign (same, opposite, or either). Loosetriggers presently use a logical or of layers. Tight triggers presentlyuse a logical or of correlations between pairs of layers.