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root/cvsroot/UserCode/Vuko/Notes/ElectronID/IsoTrack.tex
Revision: 1.1
Committed: Thu Jun 19 15:23:08 2008 UTC (16 years, 10 months ago) by beaucero
Content type: application/x-tex
Branch: MAIN
CVS Tags: HEAD
Log Message:
First Version

File Contents

# User Rev Content
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18     \section{Triggering on Single Charged Particle}
19    
20     For the purpose of Hcal calibration, a dedicated trigger path has been
21     designed in order to record a high rate of single charge particle
22     (mainly pions). Using these data, Hcal will be able to obtained an
23     intercalibration of the cells as well as an energy scale. The momentum
24     of such particle will be equalized using appropriate weight to the sum
25     of the energy deposited in Ecal and Hcal. It is clear that such events
26     can also be used in order to have a clean sample of charged pions. The
27     study of the energy deposition respectively in Ecal and Hcal can then
28     be compared to the simulation in order to tune it.
29    
30    
31     \subsection{Specificity of the Trigger}
32     In order to perform a sensible calibration, Hcal detector needs a
33     important amount of events. Single charge particle will be mainly
34     produced within multijet production and such production is highly
35     prescale at the trigger level.
36    
37     The trigger path has been modified in order to keep the bandwidth low:
38     even if the rate of such events is high, the information kept is
39     minimal. These kind of triggers are named AlCaRaw as their purpose is
40     the calibration of the detector. The selection of the event is strong
41     and the content of it is simply the minimal need request by Hcal
42     calibration.
43    
44     \subsection{Selection of the Events}
45     The High Level Trigger path is seeded using an OR of L1 single jets
46     and L1 single tau jet. The corresponding level 1 rate for a
47     instantaneous luminosity of $2\times 10^{30}$ or $2\times 10^{31}$ is
48     of the order of 4.5 kHz.
49    
50     The selection is based on a L1TauJet object with a matching within a
51     cone of 0.5 to a pixel track with a $p_T > 20$GeV. In a cone of 0.5
52     around this object also no pixel track with $p_T > 2$GeV should be
53     found.
54    
55     Once such candidate is found, the FED collections to be written out is
56     reduced. Only tracker FEDs around the nominal tracks are recorded as
57     well as for the Ecal while most of the FEDs of Hcal are written. This
58     gives the possibility to access to all timing information needed to
59     perform Hcal calibration.
60    
61     The total rate of such events is expected to be around 20Hz which
62     should give a bandwidth occupation of around 2MB/s.
63    
64     Such events require tracker measurement, so they will cover at maximum
65     the calibration up to $|\eta| \leq 2.4$.