S t a t u s a n d u pd a t e s

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Status and updates Gabriella Cataldi (INFN Lecce) & the group Gabriella Cataldi (INFN Lecce) & the group Moore … in the H8 test-beam … in the HLT(Pesa environment) … work in progress

description

S t a t u s a n d u pd a t e s. Gabriella Cataldi (INFN Lecce) & the group. Moore … in the H8 test-beam … in the HLT(Pesa environment) … work in progress. Moore for H8 test-beam. - PowerPoint PPT Presentation

Transcript of S t a t u s a n d u pd a t e s

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Status and updates

Gabriella Cataldi (INFN Lecce) & the groupGabriella Cataldi (INFN Lecce) & the group

• Moore … in the H8 test-beam• … in the HLT(Pesa environment)• … work in progress

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Moore for H8 test-beamByteStream format implemented in read out classes: easier to move eventually to different formatsMDT and RPC ROD data decoding as in HLT converters -The converters are filling the new muon EDM

Code usable by everyone, upgrades following Athena releasesNtuples for the analysis

Conditions data as calibrations (from Calib) and electronic mappings

Athena services available to all algorithms (MuonTBCalibrationSvc, MuonTBCablingSvc)

Initialized from plan ASCII files (located in the Athena repository)

First tests being performed using the IntervalOfValidity Service (see dedicated talk by Katharina Mair (Calibration and Alignement session on Wednesday afternoon14:00)

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Ntuples are intended as an analysis tool for MDT and RPC, and reconstruction

Example: comparison between MDT track segment extrapolation on RPC planes and RPC hits position (from MOORE reconstruction)

Moore - H8 test-beam (I)

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Moore - H8 test-beam (II) MOORE MDT segments reconstruction (calibrations from Calib)

• For the full 3-dim reconstruction the standard MOORE ntuple can be used

Chambers misalignments180 GeV beam

Barrel sagitta

Angle between segments Angle between segments reconstructed in reconstructed in

BIL and BML stationBIL and BML station

Angle between segments Angle between segments reconstructed in reconstructed in

BIL and BOL stationBIL and BOL station

Angle between segments Angle between segments reconstructed in reconstructed in

BML and BOL stationBML and BOL station

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TrigMoore: Implementation of MOORE/MuID in the framework of High Level Trigger at the Event Filter stage.

Wrapped Strategy- Allows to execute the offline reconstruction chain from the online environment, reconstructing the event by accessing at all the Spectrometer data. The implemented chain is composed by Moore and MuidStandAlone performing an extrapolation of tracks reconstructed by MOORE to the interaction point.

Seeded Strategy – Uses the hypotesys formed at the previous stage in the trigger process, accessing only to subdetectors data that are of interest for the selected trigger regions. (By now only regions selected by the LVL1 trigger have been used).

Moore in HLT- TrigMoore

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Moore in HLT- a contact point between offline and online.

Main ideas

The algorithms operating in the High Level Trigger at the Event Filter stage should not operate only in a general purpose mode (reconstructing the event in full scan) but should be able to operate starting from hypothesys formed in the previous stages of the triggering process.

Avoid the code duplication! Only the seeding has an ``ad hoc’’ implementation for the online environment.

RecMuonRoI

( ±±)RegionSelector Hash offline IDs

DigitsCollection

(RPCs and MDTs)

RPCDigitContainerMDTDigitContainer

TDS(ZEBRA)

MooMakePhiSegmentSeededMooMakeRZSegmentSeeded

PhiSegmentContainerRZSegmentContainer

(TDS)

MooMakeRoadsMooMakeTracksTracks

MooHLTAlgodecision

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TrigMoore timing tests (I) Atlas pcatr machine (2.4GHz) Atlas pcatr machine (2.4GHz) OPT buildOPT build Timing package: TrigTools/TrigTimeTiming package: TrigTools/TrigTime Strategies Seeded/wrappedStrategies Seeded/wrapped Conservative approach (i.e. data access

and data preparation are included)

Timing test performed on 6.0.4 release Timing test performed on 6.0.4 release Timing test performed on 6.0.4 release Timing test performed on 6.0.4 release

DC1 single Muons DC1 single Muons execution timesexecution timesDC1 single Muons DC1 single Muons execution timesexecution times

TailsTailsTailsTails

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TrigMoore timing tests(II)

DC1 single Muons DC1 single Muons execution timesexecution timesDC1 single Muons DC1 single Muons execution timesexecution times

Timing test performed on 6.0.4 release Timing test performed on 6.0.4 release The use (from ATLAS release 6.6) of The use (from ATLAS release 6.6) of Compact Identifiers and the changes Compact Identifiers and the changes introduced in the fitter can influence the introduced in the fitter can influence the timingtiming

Timing test performed on 6.0.4 release Timing test performed on 6.0.4 release The use (from ATLAS release 6.6) of The use (from ATLAS release 6.6) of Compact Identifiers and the changes Compact Identifiers and the changes introduced in the fitter can influence the introduced in the fitter can influence the timingtiming

In the table the average and rms is In the table the average and rms is calculated on the events left after calculated on the events left after rejecting 5% of the events included in the rejecting 5% of the events included in the high execution time tail high execution time tail

Wrapped, Full event Reconstruction

Seeded: Access only the RoI from the LVL1

pT

(GeV/c)<T> (msec)

rms (msec)

<T> (msec)

rms (msec)

8 73 30 68 30

20 59 15 58 21

50 61 19 58 25

100 61 75 64 26

300 75 23 64 32100+X1 763 37 2680 450100+X2 1218 50 5900 1100

Single Muons + Pile upSingle Muons + Pile upSingle Muons + Pile upSingle Muons + Pile up

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TrigMoore timing efficiencyA time efficiency has been defined as the ratio between the number of reconstructed tracks in one second and the total number of reconstructed tracks

A time efficiency has been defined as the ratio between the number of reconstructed tracks in one second and the total number of reconstructed tracks

DC1 single MuonsDC1 single MuonsDC1 single MuonsDC1 single Muons

•Average on events with time<1sec•Mean time almost constant over Pt•Wrapped mode times rather similar

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Wrapped strategy || < 1.05Wrapped strategy || < 1.05

Strategy seeded || < 1.05Strategy seeded || < 1.05Strategy wrapped || < 1.05Strategy wrapped || < 1.05

Efficiency for the reconstruction of single Muons Efficiency for the reconstruction of single Muons sample in sample in wrappedwrapped strategy ( strategy (event scanevent scan). This is ). This is equivalent to the execution of the offline version of the equivalent to the execution of the offline version of the code. The analysis has been restricted to the barrel code. The analysis has been restricted to the barrel region in order to be directly compared with the region in order to be directly compared with the seeded strategy. (LVL1/LVL2 restricted to the barrel)seeded strategy. (LVL1/LVL2 restricted to the barrel)Resolution in Resolution in wrappedwrapped and and seeded seeded strategy.strategy.

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Present and Future work on TrigMoore.

TrigMoore in release 7.0.0 towards 7.1.0 Migration to gcc3.2 accomplished Wrapped strategy (working)

Seeded strategy (MOORE not started-investigating)

When running in the main release more general changes have to be considered (e.g. Compact Identifiers- Id Helpers- changes in the fitter). Those changes effect the MOORE execution time. Timing table has to be evaluated once again and the optimization of the time consuming algorithmic

part has to be accomplished Implementation of the complete Muon slice

Read LVL2 output results

Efficiency curves and trigger rates Calculation of efficiency curves and trigger rates using single muons sample Calculation of efficiency curves and trigger rates using realistic event samples

EventFilter Selection on Physic samples

RPC bytestream converters Full online implementation of TrigMoore- The data access via ByteStream has not been considered

up to now from MOORE. Also in this case we expect a change in the timing performance.

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Moore and the CSCs

Moore can now understand the CSC strips, but we don’t

have data with properly simulated CSCs digits (only specially simulated samples have been used)

The current version of MOORE does not give better results

with the old data since in these data the CSC digits don’t have the charge information

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Conclusions

… for more information: Moore as Event Filter in the ATLAS High Level Trigger ATL-SOFT-2003-008, ATL-DAQ-2003-020

Track reconstruction in the ATLAS Muon Spectrometer with MOORE ATL-SOFT-2003-007