Data Processing Group activities: status and plans. F. Prino, C. Zampolli

Size: px
Start display at page:

Download "Data Processing Group activities: status and plans. F. Prino, C. Zampolli"

Transcription

1 Data Processing Group activities: status and plans F. Prino, C. Zampolli DPG Plenary Meeting, February 21 st 2017

2 Outline DPG organization DPG material New twiki pages with documentation on data sample reconstruction, analysis tools Data Processing: status and plans Good run lists Reconstruction of p-pb data and guidelines for the analysis Monte Carlo productions: status and plans Summary of QM campaign Productions anchored to the p-pb sample(s) QA tools and Analysis Objects and Tools Towards 2017 data taking Alignment and Calibration plans for 2017 New HLT cluster finder Conclusions 02/02/17 F. Prino, C. Zampolli 2

3 detectors detectors DPG Coordination DPG Coordination Chiara Zampolli Francesco Prino PROC Processing Roberto Preghenella Catalin-Lucian Ristea (*) Chiara Zampolli detectors The DPG in alphabetical order: QAT QA and Tools Marie Germain, E. Botta Jacek Otwinowski (*) PWGs AOT Analysis Objects and Tools Catalin-Lucian Ristea (*), David Dobrigkeit Chinellato, Andrea Dainese & Andrea Rossi (*) Recently joined DPG coordination, welcome! PWGs 02/02/17 F. Prino, C. Zampolli 3

4 New twiki page for the Run-2 data samples with completed data processing, summarizing: Main characteristics Reconstruction passes Links to the RCT, QA, run lists MC productions DPG Twiki: news eriodssummary 02/02/17 F. Prino, C. Zampolli 4

5 DPG Twiki: news Twiki page with guidelines for the analysis of Run-2 data samples How to merge together different LHC15o reconstruction passes (with w/o pidfix, cookdedx) NEW: how to merge the three reconstructions of the p-pb sample (CENT_wSDD, CENT_woSDD, FAST) 02/02/17 F. Prino, C. Zampolli 5

6 DPG Twiki: news New twiki page on pileup in Run-2 samples summarising: basic information about same-bunch and out-of-bunch pileup impact on the data analysis tools to remove/cleanup the samples (at the event and track selection level) 02/02/17 F. Prino, C. Zampolli 6

7 Data reconstruction campaign in PbPb, 5 TeV (LHC15o) 2015 pp, 5 TeV (LHC15n) 2016 pp, 13 TeV (LHC16k, l) 2016 ppb, 5 TeV (LHC16q) 2016 ppb, 8 TeV (LHC16r) 2016 Pbp, 8 TeV (LHC16s) 2016 ppb, 5 TeV (LHC16t) From: 02/02/17 F. Prino, C. Zampolli 7

8 Fast cluster in p-pb data sets The 2016 p-pb data collected with the FAST cluster active Difference between MB-FAST and MB- CENT is SDD (slowest detector in Alice) When SDD is BUSY the event is collected without SDD MB-FAST contains all MB triggers both with and without SDD MB-CENT are the events with SDD (subsample of FAST) About 50% of the events are without SDD for LHC16q and LHC16t For LHC16r and LHC16s the FAST cluster was activated only in few runs Three reconstructions preformed: pass1_cent_wsdd: all events in the CENT cluster, i.e. with SDD in the readout, reconstructed including SDD in the tracking pass1_cent_wosdd: all events in the CENT cluster, i.e. with SDD in the readout, reconstructed excluding SDD from the tracking pass1_fast: all events that are only in the in the FAST cluster (and not in the CENT), i.e. without SDD in the readout 02/02/17 F. Prino, C. Zampolli 8

9 Fast cluster in p-pb data sets Tracking and PID performance with and without SDD (details in backup slides): Events without SDD cannot be used in analyses which use ITS PID Special attention to events without SDD needed in analyses using ITS standalone tracks Slightly (5%) lower values of TPC-ITS track matching efficiency for events without SDD Same resolution on the track impact parameter in the transverse plane (DCAxy) Less uniform azimuthal angle distribution of tracks matched to ITS for events without SDD Worse resolution on the lambda and K0s invariant mass peaks for events without SDD Suggestions on how to use the three samples in the analysis: Analyses that do not need the full statistics should use CENT_wSDD (better performance) Analyses that need to use the full statistics: CENT_wSDD and CENT_woSDD are two reconstructions of the same events, should not be summed together To have a sample with best possible tracking performance: use CENT_wSDD and FAST NOTE: cross check for systematics related to mixing events with and without SDD. To have a sample with homogeneous usage of SDD: use CENT_woSDD and FAST NOTE: not necessarily this minimizes the systematics 02/02/17 F. Prino, C. Zampolli 9

10 QA and Run Lists Lists of good runs in AliDPG twiki based on QA output: five lists created requiring: QA good for detector + full acceptance (i.e. RCT flag 1) Tracklets: (ITS + V0 + ZDC) Central Barrel tracking (ITS+V0+TPC + ZDC) Central Barrel Tracking hadron PID: (ITS+V0+TPC +TOF+T0+ ZDC) Central Barrel Tracking electron PID: (ITS+V0+TPC +TOF+TRD ZDC) Central Barrel Tracking calo: (ITS+V0+TPC +EMC+ ZDC) Available lists of good runs: Recent news: Additional list provided for the Central barrel tracking case Including runs for which the TPC is good but with incomplete acceptance (RCT flags 1 19) Run lists created for the 4 p-pb samples: LHC16q, LHC15r, LHC16s and LHC16t New version (v2) with 2 additional good runs for LHC16k 02/02/17 F. Prino, C. Zampolli 10

11 LHC16k, LHC16l Statistics LHC16k (pp 13 TeV) IR ~120 khz (but a few runs lower) Phys Sel Eff in [85%, 98%] LHC16l (pp 13 TeV) IR ~120 khz (but a few runs lower) Phys Sel Eff in [90%, 97%] N.B.: 2 runs still in QA 02/02/17 F. Prino, C. Zampolli 11

12 ppb and Pbp samples: statistics LHC16q (ppb 5 TeV) IR ~30 khz (but 3 first khz) Phys Sel Eff ~98.5% LHC16r (ppb 8 TeV) IR varying in [100, 400] khz (but a few khz) Phys Sel Eff in [85%, 98%] depending on IR LHC16s (Pb p8 TeV) IR varying in [150, 250] khz (but a few khz) Phys Sel Eff in [82%, 98%] depending on IR LHC16t (ppb 5 TeV) IR ~30 khz Phys Sel Eff ~98.7% 02/02/17 F. Prino, C. Zampolli 12

13 Next data reconstruction plan Next data processing: Recover backlog in reconstruction of pp data samples of 2015 and 2016 Features of different periods collected in: xlsx?dl=0 Prioritization of the different pp periods based on the feedback of the PWGs and discussion in the PB Current tentative plan: Start with LHC16f (B=0.2 T) Then the other 2016 pp periods Move to 2015 giving higher priority to LHC15l (closer to 5 TeV, DCal energy calibration available) Current status: Final validation of AliDPG package which will be used instead of macros + scripts from alien 02/02/17 F. Prino, C. Zampolli 13

14 Next data processing Estimated CPU times to reconstruct the 2015 and 2016 pp data samples For each period: 4 days for QA and manual calibration after cpass1 4 days for QA after ppass 2015 CPass0+CPass1 (10K CPUs, d) Total PPass (10K CPUs, d) LHC15g LHC15h LHC15i LHC15j LHC15k LHC15l TOTAL CPass0+CPass1 (10K CPUs, d) Total PPass (10K CPUs, d) LHC16d LHC16e LHC16f LHC16g LHC16h LHC16i LHC16j LHC16m LHC16o LHC16p TOTAL /02/17 F. Prino, C. Zampolli 14

15 Next data processing Tentative plan Current estimate for completion of all periods is August 2017 Not yet considered the overlap with the processing of the new 2017 data 02/02/17 F. Prino, C. Zampolli 15

16 Monte Carlo campaign for QM All done but 1 production, postponed (AMPT for PWG-CF, code was not ready) 02/02/17 F. Prino, C. Zampolli 16

17 Next Monte Carlo productions General purpose p-pb simulations started Two cycles with two different event generators (EPOS-LHC, DPMJET) Three productions per cycle, matching the 3 data reconstructions (CENT_wSDD, CENT_woSDD, FAST) Productions anchored to 5 TeV data samples (16q) are presently in 10% QA 02/02/17 F. Prino, C. Zampolli 17

18 QA tools GOAL: develop common set of tools for online and offline QA and for software release validation Meetings: Wednesday afternoon at 2.30 pm Big progresses in the last months Details in the next talks by Jacek and Markus 02/02/17 F. Prino, C. Zampolli 18

19 AOT: Analysis Objects and Tools AOT-Event: event characterization and selection Event properties: event plane, centrality (talk by Alberica later this morning) Event selection: plans Revise the event selection for Pb-Pb and pp tuned for QM Room to improve? Special selections for high-multiplicity pp? Pileup removal/mitigation (in common with AOT-track selection) Study event selection for the p-pb samples Add them to OADB/AliEventCuts AOT-Tracks: track properties and selection Main activities: QA/documentation of track reconstruction performance Track selection for Run2 data sets Book-keeping, clean-up, maintenance of track filter bits in AODs Details later this morning in the talk by Andrea Rossi 02/02/17 F. Prino, C. Zampolli 19

20 Towards 2017 data taking: calibration needs TPC calibration For every field polarity we need low and high intensity runs before going to standard CPass Each run with at least 2 M tracks (~30 mins for pp) Detector alignment Main goal: try to remove the bias seen in the impact parameter Statistics: cosmics can be used, but also beam data are needed Central Barrel: With full ITS, TPC, TRD and TOF in the readout» Cosmics: ~50M of back-to-back triggers (C0OB3) for B+,B- and B0 each (the trigger rate w/o ITS in the trigger ~90Hz -> 1 week of 100% eff per polarity)» pp data: ~10M pp triggers at IR<20kHz for B+ and B- each. B0 is preferable but not obligatory. MUON: Cosmics with MTR trigger The alignment procedure takes ~1 month for data filtering and analysis The data collected until the new alignment is available will need a new ppass 02/02/17 F. Prino, C. Zampolli 20

21 Towards 2017 data taking: improved HLT Cluster Finder Improvements in the TPC cluster finding and data compression in the HLT for the 2017 data taking New cluster finder implemented in software FPGA implementation ongoing Tested on 2015 low-intensity data New features Improved rejection of noise clusters heavily seen in 2016, maintaining the current physics performance Performance could indeed slightly improve, because noise clusters could disturb tracking Improved compression algorithm using track model compression, data format improvement, arithmetic encoding Ongoing Additional benefits: Split cluster flag available, to be used for improved de/dx calculation HLT tracks can be used as seeds for offline, reducing memory footprint and computing time 02/02/17 F. Prino, C. Zampolli 21

22 Towards 2017 data taking: improved HLT Cluster Finder Noise cluster rejection 35% reduction in number of clusters compared to old HLT Cluster Finder Overall data size reduced by 20-25% Performance No significant difference in Nclusters/track; c 2 ; de/dx resolution and PID separation Slight improvement in TPC-ITS matching at sector edge, might be able to improve further 02/02/17 F. Prino, C. Zampolli 22

23 Summary New tools provided to the analyzers to understand and deal with the data New Twiki s summarizing the features of the reconstructed periods New Twiki on pileup under construction Guidelines for pa reconstructions included in the Twiki on data samples Data reconstruction will focus on old data samples till 2017 data taking starts QA activities will be very high need responsive and well-organized QA experts Monte Carlo is now focusing on remaining requests from last year and ppb simualtions QA tools and AOT activities cover several topics Manpower always welcome! Preparation of 2017 data taking ongoing New HLT cluster finder validation planned in detail Calibration & Alignment data Quark Matter is not the end 02/02/17 F. Prino, C. Zampolli 23

24 BACKUP 02/02/17 F. Prino, C. Zampolli 24

25 Problems spotted during data reconstruction The pidfix issue Bug in the PID hypothesis used during the last tracking step (TPCrefit) Usage of old (old gas) Bethe-Bloch parameterization + 5s cut on the TPC de/dx Effect: momentum bias and reduced matching efficiency for low-p T protons (<0.4 GeV/c) Due to wrong E-loss correction for protons tracked with wrong mass hypothesis Fixed code+ocdb used for: last group of Pb-Pb runs (LHC15o pass1_pidfix); lowir PbPb (LHC15o pass3_lowir_pidfix), pp 5 TeV (LHC15n, pass3), LHC16l and LHC16k pass1 The cookdedx issue Bug in the PID hypothesis used during the first tracking step (TPCin) The de/dx values were not passed to AliTPCseed::CookdEdx and the pion mass hypothesis was used in the first prolongation of tracks from TPC to ITS Effect: reduced matching efficiency for low-p T protons (<0.8 GeV/c) and kaons (<0.4 GeV/c) The final kinematics was instead OK because the "correct" mass was used in the refit step Fixed code used for: lowir PbPb (LHC15o pass4_lowir_pidfix_cookdedx), pp 5 TeV (LHC15n, pass3), LHC16l and LHC16k pass1 In PbPb 2015 data: Runs without ZDC (no_zdc) or miscalibrated ZDC (fix_zdc) QA for these runs done manually after updates in the physics selection code. They appear separately in the good runs lists. 02/02/17 F. Prino, C. Zampolli 25

26 DPG Material: TWiki /02/17 F. Prino, C. Zampolli 26

27 DPG Material: TWiki /02/17 F. Prino, C. Zampolli 27

28 DPG Material: TWiki /02/17 F. Prino, C. Zampolli 28

29 DPG Material: TWiki o_ pdf Any feedback on the pages is more than welcome! Please, refer to these pages, JIRA, reports for any question, and also, of course, to the experts 02/02/17 F. Prino, C. Zampolli 29

30 Packages AliDPG repository: MC part of AliDPG is stable, fully integrated in central production workflow and currently used for all the productions for QM Data processing macros and scripts added recently, currently under test Note: macros and scripts used so far in data processing are taken from alien directories QA and AOD train macros 02/02/17 F. Prino, C. Zampolli 30

31 AliDPG: Monte Carlo 02/02/17 F. Prino, C. Zampolli 31

32 AliDPG: Data processing Recently added to the package, currently under test Same macros and scripts for pp and Pb-Pb data processing 02/02/17 F. Prino, C. Zampolli 32

33 QA tools Current status Different solutions for DQM, HLT and offline QA Offline QA carried out by detector experts, each using different tools Software release validation Performance benchmarks on data and MC simulations Validation (not automatic) with reference data and MC GOAL: develop common set of tools for online and offline QA, to be used both by non experts, and by experts Easy comparison data vs MC Now in exploratory phase; 3 lines of developments currently ongoing: ROOT tree based DB (TPC QA generalization) recently complemented with Jupyter notebook (visualization) Elasticsearch (nosql database) + Kibana/Kibi (visualisation) Overwatch (EMCAL QA generalization, python+root based) with ZODB (database) + JSROOT (visualization) Extensive report in the ALICE Offline Week on November 2 ( 02/02/17 F. Prino, C. Zampolli 33

34 AOT: track characterization Book-keeping of track filter bit definition per AOD set (ongoing) TWiki already existing (maintained as service task in the past) Task developed to monitor the AOD tracks per filter bit Different option under evaluation for storing and retrieving the information about how the AOD set was created Revision, clean-up, maintenance of AOD filter bits (to be started) Need input from PWG and BTG More organized way to implement new filter bits Better testing, validation, propagation of information Track selection for Run2 data sets (started) Test and validate new cuts to remove bad tracks due to TPC SP distortions QA/documentation of track reconstruction performance (ongoing) Tasks developed for ESD and AOD tracks, will be added to central QA Systematic uncertainty on track reconstruction efficiency Track impact parameter resolution and bias Common interface for ESD and AOD track selection 02/02/17 F. Prino, C. Zampolli 34

35 TPC-ITS matching efficiency A. Barbano, C. Terrevoli TPC-ITS matching efficiency systematics Systematic uncertainty on tracking efficiency estimated from the difference in TPC-ITS matching efficiency between data and MC Affected also by different amount of secondaries in data and MC Procedure (similar to the one used in the 5 TeV spectra and RAA analyses, Extract from MC the fractions and the matching efficiencies of primary and secondary particles Extract the fractions of primary and secondary particles in data via template fits to impact parameter distributions Re-weight the MC efficiencies with the fractions of primary and secondary particles from data 02/02/17 F. Prino, C. Zampolli Data MC primaries MC secondaries MC out of the box MC reweighted p T (GeV/c) 35

36 Impact parameter resolution A. Festanti Same impact parameter resolution in highir and lowir runs Slightly worse resolution in data than MC Slightly larger data-mc discrepancy w.r.t /02/17 F. Prino, C. Zampolli 36

37 Impact parameter bias A. Festanti Impact parameter distribution not centered at 0 Larger displacement w.r.t data Data-MC discrepancy up to μm for the mean 02/02/17 F. Prino, C. Zampolli 37

38 Impact parameter bias: checks A. Festanti LHC15o lowir TPC+ITS tracks LHC15o lowir ITSsa tracks LHC15f TPC+ITS tracks 02/02/17 F. Prino, C. Zampolli Bias present in different eta/phi regions Bias present (although slightly smaller) also for ITS standalone tracks Bias present (although reduced) when excluding tracks crossing ITS modules not realigned in 2015 Smaller bias in LHC15f Detector alignment changed? Difference between pp and Pb-Pb? Check LHC15n PWGs should evaluate the effect of this bias in their analyses 38

39 PID issues during the tracking pidfix: Problem with dedx parameterization used to assign the PID in the tracking + number of sigma used to cut on the signal pion mass hypothesis used for higher mass particles effects are relevant for protons with pt<0.4 GeV/c, kaons with pt<0.3 GeV/c and nuclei Affected datasets: 2/3 HI LHC15o ( pass1 ), LHC15n, pass2 LI LHC15o See Talk at the Physics Forum on 5.10 cookdedx: Missing identification during the TPCin early step of the reconstruction (due to missing TPC clusters) pion mass hypothesis always used it affect kaons with pt<0.4 GeV/c and protons with pt<0.8 GeV/c Affected datasets: HI LHC15o ( pass1, and pass1_pidfix ), LHC15n, pass3 LI LHC15o 02/02/17 F. Prino, C. Zampolli 39

40 Matching rate cookdedx: data vs MC R. Shahoyan Data MC 02/02/17 F. Prino, C. Zampolli 40

41 Matching rate cookdedx: data vs MC R. Shahoyan Data MC Compatible behaviour in data and MC Absolute difference in match eff between data and MC comes from the pile-up in LHC16l and higher secondaries contamination in data More studies started using the low IR sample from LHC15o (reconstructed both with and without the fix, with corresponding MC) 02/02/17 F. Prino, C. Zampolli 41

42 Large extrapolation error at low p T R. Shahoyan Symptom: small ITS-TPC matching efficiency at low pt , pass2_lowir , pass3_lowir_pidfix p T p T Difference: in pass3 fluctuations are accounted by extra errors added to clusters and additional covariance matrix accounting for errors correlation At low p T the inconsistency in correlated error matrix building wrt original formula leads to too large extrapolated error of the track and its rejection by a fiducial cut in ITS 02/02/17 F. Prino, C. Zampolli 42

43 Large extrapolation error at low p T R. Shahoyan Symptom: small ITS-TPC matching efficiency at low pt 0.8 Match eff vs phi , pass2_lowir , pass3_lowir_pidfix 0.55 p T p T , pass2_lowir , pass3_lowir_pidfix Difference: in pass3 fluctuations are accounted by extra errors added to clusters and additional covariance matrix accounting for errors correlation Effect is particularly bad in run due to strongly overestimated distortions fluctuations error 02/02/17 F. Prino, C. Zampolli 43

44 Large extrapolation error at low p T R. Shahoyan Symptom: small ITS-TPC matching efficiency at low pt , pass2_lowir , pass3_lowir_pidfix Reason of inconsistency: the method used Kalman fit matrix instead of LLS matrix used in derivation: their difference is too large at low low p T Fixed in aliroot since last week Since many samples have been reconstructed with this feature, important to verify data vs MC comparison Effect becomes significant at top IR (~7.5 khz) around distortion hot spots, where the distortion fluctuation error becomes very large (up to 1 cm) 02/02/17 F. Prino, C. Zampolli 44

45 R. Shahoyan Large extrapolation error at low p T : data vs MC Few percent difference data vs MC as known from secondaries The assigned TPC track errors are well reproduced in the MC, hence the effect of the Invariant cut on matching rate is also reproduced. 02/02/17 F. Prino, C. Zampolli 45

46 Large extrapolation error at low p T : impact on data LHC15n (pp, 5 TeV): no bad run found LHC15o: one bad run found: (low IR, 12K kint7 triggers) In total we have 4.7M kint7 in the low IR sample Other (~25) runs with drop by 5-6% in match eff at low p T on the C- side, not marked as bad since this is reproduced in MC (see before) LHC16l: 8 bad runs found: , , , , , (SSD C-side off, 3.2M total events, ~1.7M kint7), , (2 SSD DDLs not readout, 2.8M total events, 477K kint7)» In total we have: 323M total events, 54M kint7 LHC16k: no bad run found 02/02/17 F. Prino, C. Zampolli 46

47 LHC15o, PbPb, 5 TeV Statistics of golden runs (CentralBarrel) Full ITS, TPC, V0, ZDC pass N. Run (tot) N. Ev (tot) (M) N. Ev with TPC (tot) (M) Golden runs (corresponding total without selection - figures in parenthesis) N. kint7 (tot) (M) Anchored Gen Purp MC pass2_lowir 12 (12) 9 (9) 8 (8) 5 (5) LHC16h8(a, b) pass3_lowir_pi dfix pass4_lowir_pi dfix_cookdedx 11 (12) 9 (9) 8 (8) 5 (5) LHC16g1(a, b, c) 11 (12) 9 (9) 8 (8) 5 (5) LHC16j7(a, b) pass1 78 (108) 299 (406) 111 (154) 71 (100) LHC16g1(a, b, c) pass1_pidfix 6 (42) 15 (140) 6 (55) 5 (44) LHC16g1(a, b, c) Golden runs, no ZDC (corresponding total without selection - figures in parenthesis) lowir (all passes) 1 (1) 0.1 (0.1) 0.1 (0.1) 0.1 (0.1) LHC16g1(a, b, c), LHC16j7(a,b) pass1 4 (8) 17 (27) 6 (9) 4 (7) LHC16g1(a, b, c) pass1_pidfix 1 (1) 0.2 (0.2) 0.2 (0.2) 0.2 (0.2) LHC16g1(a, b, c) Golden runs, fix ZDC (corresponding total without selection - figures in parenthesis) pass1 3 (9) 13 (34) 6 (14) 5 (12) LHC16g1(a, b, c) 02/02/17 F. Prino, C. Zampolli 47

48 LHC15o, PbPb, 5 TeV Statistics of runs w/o full TPC acceptance (CentralBarrel) pass N. Run (tot) N. Ev (tot) (M) N. Ev with TPC (tot) (M) N. kint7 (tot) (M) Not full TPC acceptance (corresponding total without selection - figures in parenthesis) Anchored Gen Purp MC pass1 6 (108) 14 (406) 6 (154) 5 (100) LHC16g1(a, b, c) pass1_pidfix 33 (42) 120 (140) 46 (55) 38 (44) LHC16g1(a, b, c) Not Full TPC acceptance, no ZDC (corresponding total without selection - figures in parenthesis) Not Full TPC acceptance, fix ZDC (corresponding total without selection - figures in parenthesis) pass1 6 (9) 21 (34) 8 (14) 6 (12) LHC16g1(a, b, c) N.B.: 1. The runs with Not Full TPC Acceptance are excluded by definition in the Golden runs lists 2. The Golden run lists are defined asking for full ITS, V0, ZDC, TPC 3. Only runs with full ITS, TPC, TRD in data taking are considered (in tot numbers) 02/02/17 F. Prino, C. Zampolli 48

49 Statistics of golden runs (CentralBarrel) pass N. Run (tot) N. Ev (tot) (M) N. Ev with TPC (tot) (M) Golden runs (total in parenthesis) N. kint7 (tot) (M) Anchored Gen Purp MC pass2 27 (27) 187 (187) 138 (138) 13 (13) n/a LHC15n, pp, 5 TeV 02/02/17 F. Prino, C. Zampolli 49

50 Match eff vs phi Match eff vs pt Reco with vs without SDD (CENT events) Ad hoc reco done, output at /alice/cern.ch/user/p/pwg_pp/lhc16q/ /pass1 ITS refit ITS refit + SPD any Eta > 0 (A side) Black vs blue: ~5% difference Black vs blue: ~2% difference withsdd w/osdd Strong dependence on ITS status Black vs blue: ~2% difference Black vs blue: ~0% difference 17/11/16 F. Prino, C. Zampolli 50

51 Match eff vs phi Match eff vs pt Reco with vs without SDD (CENT events) Ad hoc reco done, output at /alice/cern.ch/user/p/pwg_pp/lhc16q/ /pass1 ITS refit ITS refit + SPD any Eta < 0 (C side) Black vs blue: ~5% difference Black vs blue: ~2% difference withsdd w/osdd Strong dependence on ITS status Black vs blue: ~2% difference Black vs blue: ~0% difference 17/11/16 51

52 Reco with vs without SDD (CENT events) Ad hoc reco done, output at /alice/cern.ch/user/p/pwg_pp/lhc16q/ /pass1 Eta > 0 (A side) Eta < 0 (C side) ITS refit, no TOF bc ITS refit, TOF bc SPD any, no TOF bc 17/11/16 52 SPD any, TOF bc

53 Without SDD With SDD Reco with vs without SDD (CENT events) Ad hoc reco done, output at /alice/cern.ch/user/p/pwg_pp/lhc16q/ /pass1 Λ, all pt antiλ, all pt No selection on the position of the Λ decay vertex Mean = Sigma = 1.38 Mean = Sigma = 1.37 Mean = Sigma = 1.57 Mean = Sigma = /11/16 53

54 Reco with vs without SDD (CENT events) Ad hoc reco done, output at /alice/cern.ch/user/p/pwg_pp/lhc16q/ /pass1 Λ, all pt - With SDD - Intervals of radius of Λ decay vertex Sigma = 1.38 Sigma = 1.37 Sigma = 1.32 Sigma = /11/16 54

55 Reco with vs without SDD (CENT events) Ad hoc reco done, output at /alice/cern.ch/user/p/pwg_pp/lhc16q/ /pass1 Λ, all pt - Without SDD - Intervals of radius of Λ decay vertex Sigma = 1.43 Sigma = 1.51 Sigma = 1.69 Sigma = /11/16 55

56 Reco with vs without SDD (CENT events) Ad hoc reco done, output at /alice/cern.ch/user/p/pwg_pp/lhc16q/ /pass1 Eta > 0 (A side) Eta < 0 (C side) 3pi/4 < phi < 5pi/4 with SDD without SDD 56

57 Physics Selection in LHC16k Efficiency Interaction Rate 02/02/17 F. Prino, C. Zampolli 57

58 Physics Selection in LHC16r Efficiency Interaction Rate 02/02/17 F. Prino, C. Zampolli 58

59 Physics Selection in LHC16q Efficiency Interaction Rate 02/02/17 F. Prino, C. Zampolli 59

Stefania Beolè (Università di Torino e INFN) for the ALICE Collaboration. TIPP Chicago, June 9-14

Stefania Beolè (Università di Torino e INFN) for the ALICE Collaboration. TIPP Chicago, June 9-14 ALICE SDD ITS performance with pp and Pb-Pb beams Stefania Beolè (Università di Torino e INFN) for the ALICE Collaboration - Chicago, June 9-14 Inner Tracking System (I) Six layers of silicon detectors

More information

ALICE tracking system

ALICE tracking system ALICE tracking system Marian Ivanov, GSI Darmstadt, on behalf of the ALICE Collaboration Third International Workshop for Future Challenges in Tracking and Trigger Concepts 1 Outlook Detector description

More information

PoS(High-pT physics09)036

PoS(High-pT physics09)036 Triggering on Jets and D 0 in HLT at ALICE 1 University of Bergen Allegaten 55, 5007 Bergen, Norway E-mail: st05886@alf.uib.no The High Level Trigger (HLT) of the ALICE experiment is designed to perform

More information

arxiv: v1 [physics.ins-det] 18 Jan 2011

arxiv: v1 [physics.ins-det] 18 Jan 2011 arxiv:111.3491v1 [physics.ins-det] 18 Jan 11 Alice Alignment, Tracking and Physics Performance Results University of Padova and INFN E-mail: rossia@pd.infn.it for the ALICE Collaboration The ALICE detector

More information

Charged Particle Reconstruction in HIC Detectors

Charged Particle Reconstruction in HIC Detectors Charged Particle Reconstruction in HIC Detectors Ralf-Arno Tripolt, Qiyan Li [http://de.wikipedia.org/wiki/marienburg_(mosel)] H-QM Lecture Week on Introduction to Heavy Ion Physics Kloster Marienburg/Mosel,

More information

Status of PID. PID in in Release Muon Identification Influence of of G4-Bug on on PID. BABAR Collaboration Meeting, Oct 1st 2005

Status of PID. PID in in Release Muon Identification Influence of of G4-Bug on on PID. BABAR Collaboration Meeting, Oct 1st 2005 Status of PID PID in in Release 18 18 Run Run 3,, Run Run 5 Muon Identification Influence of of G4-Bug on on PID The PID-Group: David Aston (*), Bipul Bhuyan (*), Thorsten Brandt, Kevin Flood, Jonathan

More information

Analysis of Σ 0 baryon, or other particles, or detector outputs from the grid data at ALICE

Analysis of Σ 0 baryon, or other particles, or detector outputs from the grid data at ALICE Analysis of Σ 0 baryon, or other particles, or detector outputs from the grid data at ALICE Introduction Analysis Chain Current status of Σ 0 analysis Examples of root files from the data and MC Discussion

More information

Tracking POG Update. Tracking POG Meeting March 17, 2009

Tracking POG Update. Tracking POG Meeting March 17, 2009 Tracking POG Update Tracking POG Meeting March 17, 2009 Outline Recent accomplishments in Tracking POG - Reconstruction improvements for collisions - Analysis of CRAFT Data Upcoming Tasks Announcements

More information

8.882 LHC Physics. Track Reconstruction and Fitting. [Lecture 8, March 2, 2009] Experimental Methods and Measurements

8.882 LHC Physics. Track Reconstruction and Fitting. [Lecture 8, March 2, 2009] Experimental Methods and Measurements 8.882 LHC Physics Experimental Methods and Measurements Track Reconstruction and Fitting [Lecture 8, March 2, 2009] Organizational Issues Due days for the documented analyses project 1 is due March 12

More information

Tracking and compression techniques

Tracking and compression techniques Tracking and compression techniques for ALICE HLT Anders Strand Vestbø The ALICE experiment at LHC The ALICE High Level Trigger (HLT) Estimated data rate (Central Pb-Pb, TPC only) 200 Hz * 75 MB = ~15

More information

Track reconstruction with the CMS tracking detector

Track reconstruction with the CMS tracking detector Track reconstruction with the CMS tracking detector B. Mangano (University of California, San Diego) & O.Gutsche (Fermi National Accelerator Laboratory) Overview The challenges The detector Track reconstruction

More information

Event reconstruction in STAR

Event reconstruction in STAR Chapter 4 Event reconstruction in STAR 4.1 Data aquisition and trigger The STAR data aquisition system (DAQ) [54] receives the input from multiple detectors at different readout rates. The typical recorded

More information

Performance of the ATLAS Inner Detector at the LHC

Performance of the ATLAS Inner Detector at the LHC Performance of the ALAS Inner Detector at the LHC hijs Cornelissen for the ALAS Collaboration Bergische Universität Wuppertal, Gaußstraße 2, 4297 Wuppertal, Germany E-mail: thijs.cornelissen@cern.ch Abstract.

More information

Direct photon measurements in ALICE. Alexis Mas for the ALICE collaboration

Direct photon measurements in ALICE. Alexis Mas for the ALICE collaboration Direct photon measurements in ALICE Alexis Mas for the ALICE collaboration 1 Outline I - Physics motivations for direct photon measurements II Direct photon measurements in ALICE i - Conversion method

More information

Real-time Analysis with the ALICE High Level Trigger.

Real-time Analysis with the ALICE High Level Trigger. Real-time Analysis with the ALICE High Level Trigger C. Loizides 1,3, V.Lindenstruth 2, D.Röhrich 3, B.Skaali 4, T.Steinbeck 2, R. Stock 1, H. TilsnerK.Ullaland 3, A.Vestbø 3 and T.Vik 4 for the ALICE

More information

ALICE ANALYSIS PRESERVATION. Mihaela Gheata DASPOS/DPHEP7 workshop

ALICE ANALYSIS PRESERVATION. Mihaela Gheata DASPOS/DPHEP7 workshop 1 ALICE ANALYSIS PRESERVATION Mihaela Gheata DASPOS/DPHEP7 workshop 2 Outline ALICE data flow ALICE analysis Data & software preservation Open access and sharing analysis tools Conclusions 3 ALICE data

More information

b-jet identification at High Level Trigger in CMS

b-jet identification at High Level Trigger in CMS Journal of Physics: Conference Series PAPER OPEN ACCESS b-jet identification at High Level Trigger in CMS To cite this article: Eric Chabert 2015 J. Phys.: Conf. Ser. 608 012041 View the article online

More information

CMS Conference Report

CMS Conference Report Available on CMS information server CMS CR 2005/021 CMS Conference Report 29 Septemebr 2005 Track and Vertex Reconstruction with the CMS Detector at LHC S. Cucciarelli CERN, Geneva, Switzerland Abstract

More information

ALICE is one of the four large-scale experiments at the

ALICE is one of the four large-scale experiments at the Online Calibration of the TPC Drift Time in the ALICE High Level Trigger David Rohr, Mikolaj Krzewicki, Chiara Zampolli, Jens Wiechula, Sergey Gorbunov, Alex Chauvin, Ivan Vorobyev, Steffen Weber, Kai

More information

The ALICE High Level Trigger

The ALICE High Level Trigger The ALICE High Level Trigger Richter Department of Physics and Technology, of Bergen, Norway for the ALICE HLT group and the ALICE Collaboration Meeting for CERN related Research in Norway Bergen, November

More information

The ALICE electromagnetic calorimeter high level triggers

The ALICE electromagnetic calorimeter high level triggers Journal of Physics: Conference Series The ALICE electromagnetic calorimeter high level triggers To cite this article: F Ronchetti et al 22 J. Phys.: Conf. Ser. 96 245 View the article online for updates

More information

Primary Vertex Reconstruction at LHCb

Primary Vertex Reconstruction at LHCb LHCb-PUB-214-44 October 21, 214 Primary Vertex Reconstruction at LHCb M. Kucharczyk 1,2, P. Morawski 3, M. Witek 1. 1 Henryk Niewodniczanski Institute of Nuclear Physics PAN, Krakow, Poland 2 Sezione INFN

More information

ATLAS ITk Layout Design and Optimisation

ATLAS ITk Layout Design and Optimisation ATLAS ITk Layout Design and Optimisation Noemi Calace noemi.calace@cern.ch On behalf of the ATLAS Collaboration 3rd ECFA High Luminosity LHC Experiments Workshop 3-6 October 2016 Aix-Les-Bains Overview

More information

First LHCb measurement with data from the LHC Run 2

First LHCb measurement with data from the LHC Run 2 IL NUOVO CIMENTO 40 C (2017) 35 DOI 10.1393/ncc/i2017-17035-4 Colloquia: IFAE 2016 First LHCb measurement with data from the LHC Run 2 L. Anderlini( 1 )ands. Amerio( 2 ) ( 1 ) INFN, Sezione di Firenze

More information

Software and computing evolution: the HL-LHC challenge. Simone Campana, CERN

Software and computing evolution: the HL-LHC challenge. Simone Campana, CERN Software and computing evolution: the HL-LHC challenge Simone Campana, CERN Higgs discovery in Run-1 The Large Hadron Collider at CERN We are here: Run-2 (Fernando s talk) High Luminosity: the HL-LHC challenge

More information

Tracking and Vertex reconstruction at LHCb for Run II

Tracking and Vertex reconstruction at LHCb for Run II Tracking and Vertex reconstruction at LHCb for Run II Hang Yin Central China Normal University On behalf of LHCb Collaboration The fifth Annual Conference on Large Hadron Collider Physics, Shanghai, China

More information

ATLAS NOTE. December 4, ATLAS offline reconstruction timing improvements for run-2. The ATLAS Collaboration. Abstract

ATLAS NOTE. December 4, ATLAS offline reconstruction timing improvements for run-2. The ATLAS Collaboration. Abstract ATLAS NOTE December 4, 2014 ATLAS offline reconstruction timing improvements for run-2 The ATLAS Collaboration Abstract ATL-SOFT-PUB-2014-004 04/12/2014 From 2013 to 2014 the LHC underwent an upgrade to

More information

Performance of the MRPC based Time Of Flight detector of ALICE at LHC

Performance of the MRPC based Time Of Flight detector of ALICE at LHC Performance of the MRPC based Time Of Flight detector of ALICE at LHC (for the ALICE Collaboration) Museo Storico della Fisica e Centro Studi e Ricerche "Enrico Fermi", Rome, Italy Dipartimento di Fisica

More information

Online Reconstruction and Calibration with Feedback Loop in the ALICE High Level Trigger

Online Reconstruction and Calibration with Feedback Loop in the ALICE High Level Trigger Online Reconstruction and Calibration with Feedback Loop in the ALICE High Level Trigger David Rohr 1,a, Ruben Shahoyan 2, Chiara Zampolli 2,3, Mikolaj Krzewicki 1,4, Jens Wiechula 4, Sergey Gorbunov 1,4,

More information

Tracking and Vertexing performance in CMS

Tracking and Vertexing performance in CMS Vertex 2012, 16-21 September, Jeju, Korea Tracking and Vertexing performance in CMS Antonio Tropiano (Università and INFN, Firenze) on behalf of the CMS collaboration Outline Tracker description Track

More information

Prompt data reconstruction at the ATLAS experiment

Prompt data reconstruction at the ATLAS experiment Prompt data reconstruction at the ATLAS experiment Graeme Andrew Stewart 1, Jamie Boyd 1, João Firmino da Costa 2, Joseph Tuggle 3 and Guillaume Unal 1, on behalf of the ATLAS Collaboration 1 European

More information

A New Segment Building Algorithm for the Cathode Strip Chambers in the CMS Experiment

A New Segment Building Algorithm for the Cathode Strip Chambers in the CMS Experiment EPJ Web of Conferences 108, 02023 (2016) DOI: 10.1051/ epjconf/ 201610802023 C Owned by the authors, published by EDP Sciences, 2016 A New Segment Building Algorithm for the Cathode Strip Chambers in the

More information

PoS(TIPP2014)204. Tracking at High Level Trigger in CMS. Mia TOSI Universitá degli Studi di Padova e INFN (IT)

PoS(TIPP2014)204. Tracking at High Level Trigger in CMS. Mia TOSI Universitá degli Studi di Padova e INFN (IT) Universitá degli Studi di Padova e INFN (IT) E-mail: mia.tosi@gmail.com The trigger systems of the LHC detectors play a crucial role in determining the physics capabilities of the experiments. A reduction

More information

Disentangling P ANDA s time-based data stream

Disentangling P ANDA s time-based data stream Disentangling P ANDA s time-based data stream M. Tiemens on behalf of the PANDA Collaboration KVI - Center For Advanced Radiation Technology, University of Groningen, Zernikelaan 25, 9747 AA Groningen,

More information

Time of CDF (II)

Time of CDF (II) TOF detector lecture, 19. august 4 1 Time of Flight @ CDF (II) reconstruction/simulation group J. Beringer, A. Deisher, Ch. Doerr, M. Jones, E. Lipeles,, M. Shapiro, R. Snider, D. Usynin calibration group

More information

First results from the LHCb Vertex Locator

First results from the LHCb Vertex Locator First results from the LHCb Vertex Locator Act 1: LHCb Intro. Act 2: Velo Design Dec. 2009 Act 3: Initial Performance Chris Parkes for LHCb VELO group Vienna Conference 2010 2 Introducing LHCb LHCb is

More information

PoS(EPS-HEP2017)523. The CMS trigger in Run 2. Mia Tosi CERN

PoS(EPS-HEP2017)523. The CMS trigger in Run 2. Mia Tosi CERN CERN E-mail: mia.tosi@cern.ch During its second period of operation (Run 2) which started in 2015, the LHC will reach a peak instantaneous luminosity of approximately 2 10 34 cm 2 s 1 with an average pile-up

More information

The performance of the ATLAS Inner Detector Trigger Algorithms in pp collisions at the LHC

The performance of the ATLAS Inner Detector Trigger Algorithms in pp collisions at the LHC X11 opical Seminar IPRD, Siena - 7- th June 20 he performance of the ALAS Inner Detector rigger Algorithms in pp collisions at the LHC Mark Sutton University of Sheffield on behalf of the ALAS Collaboration

More information

Calorimeter Object Status. A&S week, Feb M. Chefdeville, LAPP, Annecy

Calorimeter Object Status. A&S week, Feb M. Chefdeville, LAPP, Annecy Calorimeter Object Status St A&S week, Feb. 1 2017 M. Chefdeville, LAPP, Annecy Outline Status of Pi0 calibration Calibration survey with electrons (E/p) Calorimeter performance with single photons from

More information

Performance of the GlueX Detector Systems

Performance of the GlueX Detector Systems Performance of the GlueX Detector Systems GlueX-doc-2775 Gluex Collaboration August 215 Abstract This document summarizes the status of calibration and performance of the GlueX detector as of summer 215.

More information

The CMS Computing Model

The CMS Computing Model The CMS Computing Model Dorian Kcira California Institute of Technology SuperComputing 2009 November 14-20 2009, Portland, OR CERN s Large Hadron Collider 5000+ Physicists/Engineers 300+ Institutes 70+

More information

HLT Hadronic L0 Confirmation Matching VeLo tracks to L0 HCAL objects

HLT Hadronic L0 Confirmation Matching VeLo tracks to L0 HCAL objects LHCb Note 26-4, TRIG LPHE Note 26-14 July 5, 26 HLT Hadronic L Confirmation Matching VeLo tracks to L HCAL objects N. Zwahlen 1 LPHE, EPFL Abstract This note describes the HltHadAlleyMatchCalo tool that

More information

ATLAS PILE-UP AND OVERLAY SIMULATION

ATLAS PILE-UP AND OVERLAY SIMULATION ATLAS PILE-UP AND OVERLAY SIMULATION LPCC Detector Simulation Workshop, June 26-27, 2017 ATL-SOFT-SLIDE-2017-375 22/06/2017 Tadej Novak on behalf of the ATLAS Collaboration INTRODUCTION In addition to

More information

PoS(EPS-HEP2017)492. Performance and recent developments of the real-time track reconstruction and alignment of the LHCb detector.

PoS(EPS-HEP2017)492. Performance and recent developments of the real-time track reconstruction and alignment of the LHCb detector. Performance and recent developments of the real-time track reconstruction and alignment of the LHCb detector. CERN E-mail: agnieszka.dziurda@cern.ch he LHCb detector is a single-arm forward spectrometer

More information

Track reconstruction of real cosmic muon events with CMS tracker detector

Track reconstruction of real cosmic muon events with CMS tracker detector Track reconstruction of real cosmic muon events with CMS tracker detector Piergiulio Lenzi a, Chiara Genta a, Boris Mangano b a Università degli Studi di Firenze and Istituto Nazionale di Fisica Nucleare

More information

Performance of Tracking, b-tagging and Jet/MET reconstruction at the CMS High Level Trigger

Performance of Tracking, b-tagging and Jet/MET reconstruction at the CMS High Level Trigger Journal of Physics: Conference Series PAPER OPEN ACCESS Performance of Tracking, b-tagging and Jet/MET reconstruction at the CMS High Level Trigger To cite this article: Mia Tosi 205 J. Phys.: Conf. Ser.

More information

CMS Alignement and Calibration workflows: lesson learned and future plans

CMS Alignement and Calibration workflows: lesson learned and future plans Available online at www.sciencedirect.com Nuclear and Particle Physics Proceedings 273 275 (2016) 923 928 www.elsevier.com/locate/nppp CMS Alignement and Calibration workflows: lesson learned and future

More information

OPERA: A First ντ Appearance Candidate

OPERA: A First ντ Appearance Candidate OPERA: A First ντ Appearance Candidate Björn Wonsak On behalf of the OPERA collaboration. 1 Overview The OPERA Experiment. ντ Candidate Background & Sensitivity Outlook & Conclusions 2/42 Overview The

More information

Tracking and flavour tagging selection in the ATLAS High Level Trigger

Tracking and flavour tagging selection in the ATLAS High Level Trigger Tracking and flavour tagging selection in the ATLAS High Level Trigger University of Pisa and INFN E-mail: milene.calvetti@cern.ch In high-energy physics experiments, track based selection in the online

More information

arxiv: v1 [physics.ins-det] 26 Dec 2017

arxiv: v1 [physics.ins-det] 26 Dec 2017 EPJ Web of Conferences will be set by the publisher DOI: will be set by the publisher c Owned by the authors, published by EDP Sciences, 2017 arxiv:1712.09434v1 [physics.ins-det] 26 Dec 2017 Online Reconstruction

More information

arxiv:hep-ph/ v1 11 Mar 2002

arxiv:hep-ph/ v1 11 Mar 2002 High Level Tracker Triggers for CMS Danek Kotliński a Andrey Starodumov b,1 a Paul Scherrer Institut, CH-5232 Villigen, Switzerland arxiv:hep-ph/0203101v1 11 Mar 2002 b INFN Sezione di Pisa, Via Livornese

More information

Muon Reconstruction and Identification in CMS

Muon Reconstruction and Identification in CMS Muon Reconstruction and Identification in CMS Marcin Konecki Institute of Experimental Physics, University of Warsaw, Poland E-mail: marcin.konecki@gmail.com An event reconstruction at LHC is a challenging

More information

b-jet slice performances at L2/EF

b-jet slice performances at L2/EF 20 March 2007 Outline b-jet slice status b-tagging performance Status/Outlook b-jet slice The b-tagging selection is an element of flexibility in the ATLAS HLT framework: it might help to increase acceptance

More information

PoS(IHEP-LHC-2011)002

PoS(IHEP-LHC-2011)002 and b-tagging performance in ATLAS Università degli Studi di Milano and INFN Milano E-mail: andrea.favareto@mi.infn.it The ATLAS Inner Detector is designed to provide precision tracking information at

More information

ALICE Run3/Run4 Computing Model simulation software

ALICE Run3/Run4 Computing Model simulation software ALICE Run3/Run4 Computing Model simulation software Armenuhi.Abramyan, Narine.Manukyan Alikhanyan National Science Laboratory (Yerevan Physics Institute) @cern.ch Outline O2 Computing System upgrade program

More information

Automated reconstruction of LAr events at Warwick. J.J. Back, G.J. Barker, S.B. Boyd, A.J. Bennieston, B. Morgan, YR

Automated reconstruction of LAr events at Warwick. J.J. Back, G.J. Barker, S.B. Boyd, A.J. Bennieston, B. Morgan, YR Automated reconstruction of LAr events at Warwick J.J. Back, G.J. Barker, S.B. Boyd, A.J. Bennieston, B. Morgan, YR Challenges Single electron, 2 GeV in LAr: Easy 'by-eye' in isolation Challenging for

More information

LAr Event Reconstruction with the PANDORA Software Development Kit

LAr Event Reconstruction with the PANDORA Software Development Kit LAr Event Reconstruction with the PANDORA Software Development Kit Andy Blake, John Marshall, Mark Thomson (Cambridge University) UK Liquid Argon Meeting, Manchester, November 28 th 2012. From ILC/CLIC

More information

Electron and Photon Reconstruction and Identification with the ATLAS Detector

Electron and Photon Reconstruction and Identification with the ATLAS Detector Electron and Photon Reconstruction and Identification with the ATLAS Detector IPRD10 S12 Calorimetry 7th-10th June 2010 Siena, Italy Marine Kuna (CPPM/IN2P3 Univ. de la Méditerranée) on behalf of the ATLAS

More information

8.882 LHC Physics. Analysis Tips. [Lecture 9, March 4, 2009] Experimental Methods and Measurements

8.882 LHC Physics. Analysis Tips. [Lecture 9, March 4, 2009] Experimental Methods and Measurements 8.882 LHC Physics Experimental Methods and Measurements Analysis Tips [Lecture 9, March 4, 2009] Physics Colloquium Series 09 The Physics Colloquium Series Thursday, March 5 at 4:15 pm in room 10-250 Spring

More information

ATLAS NOTE ATLAS-CONF July 20, Commissioning of the ATLAS high-performance b-tagging algorithms in the 7 TeV collision data

ATLAS NOTE ATLAS-CONF July 20, Commissioning of the ATLAS high-performance b-tagging algorithms in the 7 TeV collision data ALAS NOE ALAS-CONF-2-2 July 2, 2 Commissioning of the ALAS high-performance b-tagging algorithms in the ev collision data he ALAS collaboration ALAS-CONF-2-2 2 July 2 Abstract he ability to identify jets

More information

05/09/07 CHEP2007 Stefano Spataro. Simulation and Event Reconstruction inside the PandaRoot Framework. Stefano Spataro. for the collaboration

05/09/07 CHEP2007 Stefano Spataro. Simulation and Event Reconstruction inside the PandaRoot Framework. Stefano Spataro. for the collaboration for the collaboration Overview Introduction on Panda Structure of the framework Event generation Detector implementation Reconstruction The Panda experiment AntiProton Annihilations at Darmstadt Multi

More information

Status Report of PRS/m

Status Report of PRS/m Status Report of PRS/m D.Acosta University of Florida Current U.S. activities PRS/m Activities New PRS organization 1 EMU Software Workshop Workshop held at UCDavis in late February helped focus EMU software

More information

Performance of FPCCD vertex detector. T. Nagamine Tohoku University Feb 6, 2007 ACFA 9, IHEP,Beijin

Performance of FPCCD vertex detector. T. Nagamine Tohoku University Feb 6, 2007 ACFA 9, IHEP,Beijin Performance of FPCCD vertex detector T. Nagamine Tohoku University Feb 6, 27 ACFA 9, IHEP,Beijin Outline FPCCD and Vertex Detector Structure Impact Parameter Resolution Pair Background in Vertex Detector

More information

Physics CMS Muon High Level Trigger: Level 3 reconstruction algorithm development and optimization

Physics CMS Muon High Level Trigger: Level 3 reconstruction algorithm development and optimization Scientifica Acta 2, No. 2, 74 79 (28) Physics CMS Muon High Level Trigger: Level 3 reconstruction algorithm development and optimization Alessandro Grelli Dipartimento di Fisica Nucleare e Teorica, Università

More information

Time and position resolution of high granularity, high counting rate MRPC for the inner zone of the CBM-TOF wall

Time and position resolution of high granularity, high counting rate MRPC for the inner zone of the CBM-TOF wall Time and position resolution of high granularity, high counting rate MRPC for the inner zone of the CBM-TOF wall M. Petris, D. Bartos, G. Caragheorgheopol, M. Petrovici, L. Radulescu, V. Simion IFIN-HH

More information

Event Displays and LArg

Event Displays and LArg Event Displays and LArg Columbia U. / Nevis Labs Slide 1 Introduction Displays are needed in various ways at different stages of the experiment: Software development: understanding offline & trigger algorithms

More information

CMS FPGA Based Tracklet Approach for L1 Track Finding

CMS FPGA Based Tracklet Approach for L1 Track Finding CMS FPGA Based Tracklet Approach for L1 Track Finding Anders Ryd (Cornell University) On behalf of the CMS Tracklet Group Presented at AWLC June 29, 2017 Anders Ryd Cornell University FPGA Based L1 Tracking

More information

Beam test measurements of the Belle II vertex detector modules

Beam test measurements of the Belle II vertex detector modules Beam test measurements of the Belle II vertex detector modules Tadeas Bilka Charles University, Prague on behalf of the Belle II Collaboration IPRD 2016, 3 6 October 2016, Siena, Italy Outline Belle II

More information

CMS High Level Trigger Timing Measurements

CMS High Level Trigger Timing Measurements Journal of Physics: Conference Series PAPER OPEN ACCESS High Level Trigger Timing Measurements To cite this article: Clint Richardson 2015 J. Phys.: Conf. Ser. 664 082045 Related content - Recent Standard

More information

Studies of the KS and KL lifetimes and

Studies of the KS and KL lifetimes and Studies of the KS and KL lifetimes and BR(K ) with KLOE ± ± + Simona S. Bocchetta* on behalf of the KLOE Collaboration KAON09 Tsukuba June 9th 2009 * INFN and University of Roma Tre Outline DA NE and KLOE

More information

π ± Charge Exchange Cross Section on Liquid Argon

π ± Charge Exchange Cross Section on Liquid Argon π ± Charge Exchange Cross Section on Liquid Argon Kevin Nelson REU Program, College of William and Mary Mike Kordosky College of William and Mary, Physics Dept. August 5, 2016 Abstract The observation

More information

PoS(Baldin ISHEPP XXII)134

PoS(Baldin ISHEPP XXII)134 Implementation of the cellular automaton method for track reconstruction in the inner tracking system of MPD at NICA, G.A. Ososkov and A.I. Zinchenko Joint Institute of Nuclear Research, 141980 Dubna,

More information

Monte Carlo programs

Monte Carlo programs Monte Carlo programs Alexander Khanov PHYS6260: Experimental Methods is HEP Oklahoma State University November 15, 2017 Simulation steps: event generator Input = data cards (program options) this is the

More information

Update on Energy Resolution of

Update on Energy Resolution of Update on Energy Resolution of the EMC Using µµγ Sample David Hopkins Royal Holloway, University of London EMC Reconstruction Workshop, December 5 th, 2004 Outline Study of photon energy resolution Compare

More information

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS CR -2008/100 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 02 December 2008 (v2, 03 December 2008)

More information

EicRoot software framework

EicRoot software framework EicRoot software framework Alexander Kiselev EIC Software Meeting Jefferson Lab September,24 2015 Contents of the talk FairRoot software project EicRoot framework structure Typical EicRoot applications

More information

THE ATLAS INNER DETECTOR OPERATION, DATA QUALITY AND TRACKING PERFORMANCE.

THE ATLAS INNER DETECTOR OPERATION, DATA QUALITY AND TRACKING PERFORMANCE. Proceedings of the PIC 2012, Štrbské Pleso, Slovakia THE ATLAS INNER DETECTOR OPERATION, DATA QUALITY AND TRACKING PERFORMANCE. E.STANECKA, ON BEHALF OF THE ATLAS COLLABORATION Institute of Nuclear Physics

More information

Measurement of fragmentation cross-section of 400 MeV/u 12 C beam on thin targets

Measurement of fragmentation cross-section of 400 MeV/u 12 C beam on thin targets Measurement of fragmentation cross-section of 400 MeV/u 12 C beam on thin targets Candidate: Abdul Haneefa Kummali Supervisor : Dr. Vincenzo Monaco PhD School - Department of Physics XXVII cycle 14-February-2014

More information

Alignment of the CMS Silicon Tracker

Alignment of the CMS Silicon Tracker Alignment of the CMS Silicon Tracker Tapio Lampén 1 on behalf of the CMS collaboration 1 Helsinki Institute of Physics, Helsinki, Finland Tapio.Lampen @ cern.ch 16.5.2013 ACAT2013 Beijing, China page 1

More information

3D-Triplet Tracking for LHC and Future High Rate Experiments

3D-Triplet Tracking for LHC and Future High Rate Experiments 3D-Triplet Tracking for LHC and Future High Rate Experiments André Schöning Physikalisches Institut, Universität Heidelberg Workshop on Intelligent Trackers WIT 2014 University of Pennsylvania May 14-16,

More information

1. Introduction. Outline

1. Introduction. Outline Outline 1. Introduction ALICE computing in Run-1 and Run-2 2. ALICE computing in Run-3 and Run-4 (2021-) 3. Current ALICE O 2 project status 4. T2 site(s) in Japan and network 5. Summary 2 Quark- Gluon

More information

Full Silicon Tracking Studies for CEPC

Full Silicon Tracking Studies for CEPC Full Silicon Tracking Studies for CEPC Weiming Yao (IHEP/LBNL) for Silicon Tracking Study Group CEPC-SppC Study Group Meeting, September 2-26, Beihang University http://cepc.ihep.ac.cn/ cepc/cepc twiki/index.php/pure

More information

The creation of a Tier-1 Data Center for the ALICE experiment in the UNAM. Lukas Nellen ICN-UNAM

The creation of a Tier-1 Data Center for the ALICE experiment in the UNAM. Lukas Nellen ICN-UNAM The creation of a Tier-1 Data Center for the ALICE experiment in the UNAM Lukas Nellen ICN-UNAM lukas@nucleares.unam.mx 3rd BigData BigNetworks Conference Puerto Vallarta April 23, 2015 Who Am I? ALICE

More information

Track reconstruction for the Mu3e experiment based on a novel Multiple Scattering fit Alexandr Kozlinskiy (Mainz, KPH) for the Mu3e collaboration

Track reconstruction for the Mu3e experiment based on a novel Multiple Scattering fit Alexandr Kozlinskiy (Mainz, KPH) for the Mu3e collaboration Track reconstruction for the Mu3e experiment based on a novel Multiple Scattering fit Alexandr Kozlinskiy (Mainz, KPH) for the Mu3e collaboration CTD/WIT 2017 @ LAL-Orsay Mu3e Experiment Mu3e Experiment:

More information

Data Quality Monitoring at CMS with Machine Learning

Data Quality Monitoring at CMS with Machine Learning Data Quality Monitoring at CMS with Machine Learning July-August 2016 Author: Aytaj Aghabayli Supervisors: Jean-Roch Vlimant Maurizio Pierini CERN openlab Summer Student Report 2016 Abstract The Data Quality

More information

Data handling and processing at the LHC experiments

Data handling and processing at the LHC experiments 1 Data handling and processing at the LHC experiments Astronomy and Bio-informatic Farida Fassi CC-IN2P3/CNRS EPAM 2011, Taza, Morocco 2 The presentation will be LHC centric, which is very relevant for

More information

Study of the Higgs boson coupling to the top quark and of the b jet identification with the ATLAS experiment at the Large Hadron Collider.

Study of the Higgs boson coupling to the top quark and of the b jet identification with the ATLAS experiment at the Large Hadron Collider. Study of the Higgs boson coupling to the top quark and of the b jet identification with the ATLAS experiment at the Large Hadron Collider. Calvet Thomas CPPM, ATLAS group PhD day 25 novembre 2015 2 The

More information

Alignment of the ATLAS Inner Detector

Alignment of the ATLAS Inner Detector Alignment of the ATLAS Inner Detector Heather M. Gray [1,2] on behalf of the ATLAS ID Alignment Group [1] California Institute of Technology [2] Columbia University The ATLAS Experiment tile calorimeter

More information

SoLID GEM Detectors in US

SoLID GEM Detectors in US SoLID GEM Detectors in US Kondo Gnanvo University of Virginia SoLID Collaboration Meeting @ JLab, 08/26/2016 Outline Design Optimization U-V strips readout design Large GEMs for PRad in Hall B Requirements

More information

Dijet A LL Dijet cross section 2006 Dijet A LL Preparation for Tai Sakuma MIT

Dijet A LL Dijet cross section 2006 Dijet A LL Preparation for Tai Sakuma MIT Dijet A LL 2005 Dijet cross section 2006 Dijet A LL Preparation for 2008 Tai Sakuma MIT Motivation for dijet A LL is to constrain ΔG G with initial event kinematics The initial state variables can be written

More information

LArTPC Reconstruction Challenges

LArTPC Reconstruction Challenges LArTPC Reconstruction Challenges LArTPC = Liquid Argon Time Projection Chamber Sowjanya Gollapinni (UTK) NuEclipse Workshop August 20 22, 2017 University of Tennessee, Knoxville LArTPC program the big

More information

TPC digitization and track reconstruction: efficiency dependence on noise

TPC digitization and track reconstruction: efficiency dependence on noise TPC digitization and track reconstruction: efficiency dependence on noise Daniel Peterson, Cornell University, DESY, May-2007 A study of track reconstruction efficiency in a TPC using simulation of the

More information

arxiv: v1 [physics.ins-det] 26 Dec 2017

arxiv: v1 [physics.ins-det] 26 Dec 2017 arxiv:1712.09407v1 [physics.ins-det] 26 Dec 2017 ALICE HLT TPC Tracking of Pb-Pb Events on GPUs David Rohr 1, Sergey Gorbunov 1, Artur Szostak 2, Matthias Kretz 1, Thorsten Kollegger 1, Timo Breitner 1,

More information

PoS(ACAT08)101. An Overview of the b-tagging Algorithms in the CMS Offline Software. Christophe Saout

PoS(ACAT08)101. An Overview of the b-tagging Algorithms in the CMS Offline Software. Christophe Saout An Overview of the b-tagging Algorithms in the CMS Offline Software Christophe Saout CERN, Geneva, Switzerland E-mail: christophe.saout@cern.ch The CMS Offline software contains a widespread set of algorithms

More information

TPC Detector Response Simulation and Track Reconstruction

TPC Detector Response Simulation and Track Reconstruction TPC Detector Response Simulation and Track Reconstruction Physics goals at the Linear Collider drive the detector performance goals: charged particle track reconstruction resolution: δ(1/p)= ~ 4 x 10-5

More information

Robustness Studies of the CMS Tracker for the LHC Upgrade Phase I

Robustness Studies of the CMS Tracker for the LHC Upgrade Phase I Robustness Studies of the CMS Tracker for the LHC Upgrade Phase I Juan Carlos Cuevas Advisor: Héctor Méndez, Ph.D University of Puerto Rico Mayagϋez May 2, 2013 1 OUTLINE Objectives Motivation CMS pixel

More information

Track pattern-recognition on GPGPUs in the LHCb experiment

Track pattern-recognition on GPGPUs in the LHCb experiment Track pattern-recognition on GPGPUs in the LHCb experiment Stefano Gallorini 1,2 1 University and INFN Padova, Via Marzolo 8, 35131, Padova, Italy 2 CERN, 1211 Geneve 23, Switzerland DOI: http://dx.doi.org/10.3204/desy-proc-2014-05/7

More information

Study of t Resolution Function

Study of t Resolution Function Belle-note 383 Study of t Resolution Function Takeo Higuchi and Hiroyasu Tajima Department of Physics, University of Tokyo (January 6, 200) Abstract t resolution function is studied in detail. It is used

More information

Recent developments in tracking and

Recent developments in tracking and Recent developments in tracking and impact on B-tagging Boris Mangano for Tracking POG group page 1 Outline B-tagging Enemies Recent developments in iterative tracking and impact on V0 reconstruction efficiency.

More information

Performance studies of the Roman Pot timing detectors in the forward region of the IP5 at LHC

Performance studies of the Roman Pot timing detectors in the forward region of the IP5 at LHC TOTEM NOTE 2014 001 August 1, 2014 Performance studies of the Roman Pot timing detectors in the forward region of the IP5 at LHC M. Berretti (CERN) Abstract CERN-TOTEM-NOTE-2014-001 01/08/2014 The detection

More information