PANDA Software Trigger Status/Plans PANDA Collaboration Meeting Giessen, Mar. 2015 K. Götzen, D. Kang, R. Kliemt, F. Nerling GSI Darmstadt/HI Mainz.

Slides:



Advertisements
Similar presentations
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Advertisements

High Level Trigger (HLT) for ALICE Bergen Frankfurt Heidelberg Oslo.
H/Abb -> 4b’s process & Multi-Et-Threshold Study for 4jet Trigger Kohei Yorita Young-Kee Kim University of the FTK Meeting on July 13 th, 2006.
PDCMSSW - Luca Perrozzi1 Looking for… Punch throughs… Looking for… Punch throughs…
Sharpening the Physics case for Charm at SuperB D. Asner, G. Batignani, I. Bigi, F. Martinez-Vidal, N. Neri, A. Oyanguren, A. Palano, G. Simi Charm AWG.
Alain Romeyer - January Light higgs decay in SUSY cascade - Status report Introduction Trigger efficiency B tagging Jet calibration Invariant mass.
M.Mevius Open and hidden beauty production in 920 GeV proton –nucleus collisions at HERA-B M.Mevius DESY.
The Silicon Track Trigger (STT) at DØ Beauty 2005 in Assisi, June 2005 Sascha Caron for the DØ collaboration Tag beauty fast …
Aras Papadelis, Lund University 8 th Nordic LHC Physics Workshop Nov , Lund 1 The ATLAS B-trigger - exploring a new strategy for J/  (ee) ●
27 th June 2008Johannes Albrecht, BEACH 2008 Johannes Albrecht Physikalisches Institut Universität Heidelberg on behalf of the LHCb Collaboration The LHCb.
1  trigger optimization in CMS Tracker Giuseppe Bagliesi On behalf of  tracking group Workshop on B/tau Physics at LHC Helsinki, May 30 - June 1, 2002.
Agnes Lundborg Open Seminar 9 th of April 2003 in Uppsala on the SweGrid project PANDA computing “a tiny specification”
Status Analysis pp -> D s D s0 (2317) Overview Reconstruction Some QA plots Figure of merit First approach/strategy.
1 Rutherford Appleton Laboratory The 13th Annual International Conference on Supersymmetry and Unification of the Fundamental Interactions Durham, 2005.
Sep. 29, 2006 Henry Band - U. of Wisconsin 1 Hadronic Charm Decays From B Factories Henry Band University of Wisconsin 11th International Conference on.
Inclusive  Production at Y(1S) Sheldon Stone Jianchun Wang Syracuse University CLEO Meeting 09/13/02.
September 27, 2005FAKT 2005, ViennaSlide 1 B-Tagging and ttH, H → bb Analysis on Fully Simulated Events in the ATLAS Experiment A.H. Wildauer Universität.
Measurement of B + K + νν David Doll Ilya Narsky David Hitlin 1 California Institute of Technology Department of Energy Review July 24, 2007.
DPF Victor Pavlunin on behalf of the CLEO Collaboration DPF-2006 Results from four CLEO Y (5S) analyses:  Exclusive B s and B Reconstruction at.
Daniele Benedetti CMS and University of Perugia Chicago 07/02/2004 High Level Trigger for the ttH channel in fully hadronic decay at LHC with the CMS detector.
James Ritman Univ. Giessen PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter Overview of the PANDA Pbar-A Program The Pbar Facility.
CHARM 2007, Cornell University, Aug. 5-8, 20071Steven Blusk, Syracuse University D Leptonic Decays near Production Threshold Steven Blusk Syracuse University.
Sept 30 th 2004Iacopo Vivarelli – INFN Pisa FTK meeting Z  bb measurement in ATLAS Iacopo Vivarelli, Alberto Annovi Scuola Normale Superiore,University.
Search for B     with SemiExclusive reconstruction C.Cartaro, G. De Nardo, F. Fabozzi, L. Lista Università & INFN - Sezione di Napoli.
1 A Feasibility Study for a Strange Sea Asymmetry Analysis at ATLAS: update II Laura Gilbert and Jeff Tseng 13/12/07.
Tau Jet Identification in Charged Higgs Search Monoranjan Guchait TIFR, Mumbai India-CMS collaboration meeting th March,2009 University of Delhi.
Current Status of Hadron Analysis Introduction Hadron PID by PHENIX-TOF  Current status of charged hadron PID  CGL and track projection point on TOF.
 Candidate events are selected by reconstructing a D, called a tag, in several hadronic modes  Then we reconstruct the semileptonic decay in the system.
H → ZZ →  A promising new channel for high Higgs mass Sara Bolognesi – Torino INFN and University Higgs meeting 23 Sept – CMS Week.
2004 Xmas MeetingSarah Allwood WW Scattering at ATLAS.
Progress on H/Abb -> 4b’s channel for the FTK physics case ~ 4jets Trigger w/ and w/o FTK ~ Kohei Yorita Young-Kee Kim University of the FTK.
L. Bellagamba, Excited fermions and other searches at HERA 1 International Conference on High Energy Physics Amsterdam July 2002 Excited fermions.
HEP 2005 WorkShop, Thessaloniki April, 21 st – 24 th 2005 Efstathios (Stathis) Stefanidis Studies on the High.
ICHEP 2002 First Heavy Flavor Results Using the Silicon Vertex Trigger A. Cerri.
Pavel Krokovny Heidelberg University on behalf of LHCb collaboration Introduction LHCb experiment Physics results  S measurements  prospects Conclusion.
WIN-03, Lake Geneva, WisconsinSanjay K Swain Hadronic rare B decays Hadronic rare B-decays Sanjay K Swain Belle collaboration B - -> D cp K (*)- B - ->
FIMCMS, 26 May, 2008 S. Lehti HIP Charged Higgs Project Preparative Analysis for Background Measurements with Data R.Kinnunen, M. Kortelainen, S. Lehti,
LHCb: Xmas 2010 Tara Shears, On behalf of the LHCb group.
Preliminary results for the BR(K S  M. Martini and S. Miscetti.
CBM Simulation Walter F.J. Müller, GSI CBM Simulation Week, May 10-14, 2004 Tasks and Concepts.
Paul Balm - EPS July 17, 2003 Towards CP violation results from DØ Paul Balm, NIKHEF (for the DØ collaboration) EPS meeting July 2003, Aachen This.
Search for the  + in photoproduction experiments at CLAS APS spring meeting (Dallas) April 22, 2006 Ken Hicks (Ohio University) for the CLAS Collaboration.
Study on search of a SM Higgs (120GeV) produced via VBF and decaying in two hadronic taus V.Cavasinni, F.Sarri, I.Vivarelli.
1 What I did last year Nick Barlow Manchester Christmas meeting January 2005.
By Henry Brown Henry Brown, LHCb, IOP 10/04/13 1.
29/08/2008ALICE Italia Analysis of the D + s  K + K - π + channel in the ALICE experiment Serhiy Senyukov Università & INFN di Torino (4050 m. asl)
Julia Thom, FNALEPS 2003 Aachen Rare Charm and B decays at CDF Julia Thom FNAL EPS 7/18/2003 Tevatron/CDF Experiment Decay Rate Ratios and CP Asymmetries.
LHCbComputing Computing for the LHCb Upgrade. 2 LHCb Upgrade: goal and timescale m LHCb upgrade will be operational after LS2 (~2020) m Increase significantly.
Elliptic flow of D mesons Francesco Prino for the D2H physics analysis group PWG3, April 12 th 2010.
Régis Lefèvre (LPC Clermont-Ferrand - France)ATLAS Physics Workshop - Lund - September 2001 In situ jet energy calibration General considerations The different.
Processing large data sets Brad Abbott. Now J/Psi Starting with root-tuples Add 4-momentum to look for candidates Pick events (raw) -> reconstruct event.
1 The use of control channels in the analysis of the B s  μ + μ - decay Tuesday Meeting, 2 June 2009.
Feb. 3, 2007IFC meeting1 Beam test report Ph. Bruel on behalf of the beam test working group Gamma-ray Large Area Space Telescope.
Aug _5071 Top stop by charm channel analysis using D0 runI data OUTLINE physics process of top to stop Monte Carlo simulation for signal data.
Eduardo RodriguesLHCb Collaboration Week, 26th November Studies of Generator-level Selection Eduardo Rodrigues, CERN I. Proposal II. Procedure III.
Hadron production in C+C at 2 A GeV measured by the HADES spectrometer Nov02 gen3 analysis and results for spline tracks (shown in Dubna) changes - removing.
Status of Analysis Tools in PandaROOT K. Götzen, GSI 1.
Search for Invisible Higgs Decays at the ILC Ayumi Yamamoto, Akimasa Ishikawa, Hitoshi Yamamoto (Tohoku University) Keisuke Fujii (KEK)
Elisa manoni FastSim meeting January 21st, FastSim meeting, FastSim meeting, January 21st, 2010 Had Breco code: status report Elisa Manoni INFN.
Charm Form Factors from from B -Factories A. Oyanguren BaBar Collaboration (IFIC –U. Valencia)
PHENIX J/  Measurements at  s = 200A GeV Wei Xie UC. RiverSide For PHENIX Collaboration.
Status of the measurement of K L lifetime - Data sample (old): ~ 440 pb -1 ( ) - MC sample: ~125 pb -1 ( mk0 stream ) Selection: standard tag (|
PANDA Software Trigger Status/Plans PANDA DAQT-FEE Workshop Apr. 2015, GSI Darmstadt K. Götzen, D. Kang, R. Kliemt, F. Nerling GSI Darmstadt/HI Mainz.
Open and Hidden Beauty Production in 920 GeV p-N interactions Presented by Mauro Villa for the Hera-B collaboration 2002/3 data taking:
INFN - PadovaBeauty Measurements in pp with the Central Detector 1 Beauty Measurements in p-p with the Central Detector F. Antinori, C. Bombonati, A. Dainese,
PANDA Software Trigger K. Götzen Dec Challenge Required reduction factor: ~1/1000 (all triggers in total) A lot of physics channel triggers → even.
SuperB and its computing requirements
Quarkonium production in ALICE
Hadronic recoil analysis:
Problems in π0 Reconstruction
Presentation transcript:

PANDA Software Trigger Status/Plans PANDA Collaboration Meeting Giessen, Mar K. Götzen, D. Kang, R. Kliemt, F. Nerling GSI Darmstadt/HI Mainz

Software Trigger within Trigger System Online Trigger System (FPGA, GPU, CPU) Raw Data Online Reco Event Building Tracking PID Neutral Reco Software Trigger Data Storage Configuration Trigger Tag Mar. 2015K.Goetzen - ST status - CM Giessen2

Strategy for Investigation EvtGen Physics Channel 1 Physics Channel 2... Physics Channel m DPM Background Fast MCFull MC Trigger 1Trigger n Trigger Decision (Logical OR) Event Generation Signal Background Simulation & Reconstruction Event Filtering Combinatorics Mass Window Selection Trigger Specific Selection → Event Tagging Trigger 2... Global Trigger Tag Trigger 3 Mar. 2015K.Goetzen - ST status - CM Giessen3

Extended Trigger Scheme Status report 2014 –n = 10 trigger lines –m = 10 signal event types –4 energies: E cm = 2.4, 3.77, 4.5, 5.5 GeV Extended scheme 2015 –n = 57 trigger lines (added subdecays and new modes) Trigger of 17 different particle/reaction types –m = 791 signal event types (considering different recoils) 10 Recoils: - / γ / π 0 / η / π 0 π 0 / π + π - / K + K - / K 0 K 0 / ηη / π + π - π 0 –7 energies: E cm = 2.4, 3.0, 3.5, 3.8, 4.5, 5.0, 5.5 GeV Mar. 2015K.Goetzen - ST status - CM Giessen4

'Complete' List of Triggers Tr#Res.Channels (BR[%])NCode Σ BR[%] 1ηcηc K + K - π 0 (1.2), K S K ± π ∓ (2.4), γγ, K + K - π + π - π 0 (3.5), K S K ± π + π - π ∓ (1.8)522x8.3 2J/ψe + e - (5.9), μ + μ - (5.9)220x11.9 3χ c0 π + π - K + K - (1.8), K ± π ∓ K S π 0 (0.8)224x2.6 4D0D0 K - π + (3.9), K - π + π 0 (13.9), K - 2π + π - (8.1), K S π + π - π 0 (3.7), K S π + π - (2.0)510x31.6 5D+D+ K - 2π + (9.4), K - 2π + π 0 (6.1), K S 2π + π - (2.1), K S π + π 0 (4.8)412x22.4 6Ds+Ds+ K + K - π ± (5.5), K + K - π ± π 0 (5.6)214x11.1 7D* 0 D 0 π 0 (61.9), D 0 γ (38.1)1011x31.6 8D* + D 0 π + (67.7), D + π 0 (30.7)913x28.7 9Ds*+Ds*+ D s + γ (94.2)215x Λp π - (63.9) Λc+Λc+ p K ∓ π ± (5.0), p K ∓ π ± π 0 (3.4), p K S π 0 (1.2)342x9.6 12Σ+Σ+ p π 0 (51.6) φK + K - (48.9) e + e - XNR; X = none / γ / π 0 360x 15μ + μ - XNR; X = none / γ / π 0 362x 16γ γ XNR; X = none / γ / π 0 364x 17γπ 0 NR1660 All K S mode include BR(K S → π + π - ) Σ=57 Triggers/modes from report Mar. 2015K.Goetzen - ST status - CM Giessen5

Charmonia ReactionTrigger #via decayTaggable η c + X18.3% J/ψ + X211.9% χ c0 (1P) + X32.6% χ c1 (1P) + X2J/ψ γ (34,4%)4.1% χ c2 (1P) + X2J/ψ γ (19,5%)2.3% h c + X1η c γ (54,3%)4.5% η c (2S) + X--0.0% ψ(2S) + X2J/ψ X (59,6%)7.1% ψ(3770) + X4,5D 0 D 0 (52%), D + D - (41%)44,0% X(3823) + X2χ c1 γ (?)< 4.1% X(3872) + X2J/ψ π + π - (>2,6%), D 0 D 0 π 0 (>32%)> 17.4% Z c + (3900) + X2,4,5,7,8J/ψ π + (?), (DD*)+ (?)< 11.9% Z c 0 (3900) + X2J/ψ π 0 (?)< 11.9% χ c0 (2P) + X4,7D 0 *D 0 (>71%)32.0% χ c2 (2P) + X4,5DD (?)< 39% X(3940) + X4,5,7,8DD* 90CL)> 20% Z + (4020) + X7,8D*D* (?)< 49% ψ(4040) + X4,5DD (?)< 40% Z + (4050) + X2χ c1 π + (?)< 4.1% ψ(4160) + X4,5,7,8DD, DD*, D*D* (?)< 40% X(4160) + X7,8D*D* (?)< 49% X(4250) + X2χ c1 π + (?)< 4.1% X(4260) + X2J/ψ X (?)< 11.9% X(4350) + X2,13J/ψ φ (?)< 54.9% X(4360) + X2ψ(2S) π + π - (?)< 7.1% ψ(4415) + X4,5,6,7,8,9DD, D s + D s - (?)< 20% Z + (4430) + X2ψ(2S) π + (?)< 7.1% X(4660) + X2ψ(2S) π + π - (?)< 7.1% Mar. 2015K.Goetzen - ST status - CM Giessen6

Open Charm ReactionTrigger #via decayTaggable D 0 D 0 + X4 53.3% D 0 D 0 * + X4,7 45.0% D 0 * D 0 * + X7 35.3% D + D - + X5 39.8% D + D - * + X5,8 44.3% D + * D - * + X8 48.6% D s + D s - + X6 21.0% D s + D s - * + X6,9 20.4% D s + * D s - * + X9 19.8% D s + D s0 *(2317) - 6D s + π 0 (?) >11.1% D s + * D s0 *(2317) - 6,9D s + π 0 (?) >10.5% D s + D s1 (2460) - 6,9D s + * π 0 (48%), D s + γ (18%) 17.3% D s + * D s1 (2460) - 6,9D s + * π 0 (48%), D s + γ (18%) 16.7% D s + D s1 (2536) - 6,8D* + K 0 (85%) 32.5% D s + * D s1 (2536) - 8,9D* + K 0 (85%) 32.0% D s + D s2 *(2573) - 4,6D 0 K (?) >11.1% D s + * D s2 *(2573) - 4,9D 0 K (?) >10.5% Mar. 2015K.Goetzen - ST status - CM Giessen7

Baryons & Light Hadrons ReactionTrigger #via decayTaggable ΛΛ + X % Σ + Σ - + X % Σ 0 Σ 0 + X10Λ γ (100%) 87.0% Σ - Σ + + X-- 0.0% Ξ 0 Ξ 0 + X10Λ π 0 (99,5%) 86.7% Ξ - Ξ + + X10Λ π - (99,9%) 86.9% Ω - Ω + + X10Λ K(67,8%), Ξ 0 π - (23,6%) 82.6% Λ c + Λ c - + X % Λ c + (..), Σ c + (..), Ξ c (..)4,11Λ c X (?), p D 0 (?) ? ReactionTrigger #via decayTaggable φ + X1348.9% e + e % e + e - X % μ+ μ-μ+ μ % μ + μ - X % γ γγ γ % γ γ X % other light hadronsmin bias100.0% → Looks quite complete (at least for spectroscopy & EMP)! Mar. 2015K.Goetzen - ST status - CM Giessen8

Data Types Target data modes for individual trigger lines are defined as: E.-M. modes (10 in total) –excl.: e+e- / μ+μ- / γγ + (none, γ, π 0 ) –excl.: γπ 0 Charmonium / ϕ (up to 10 each) –cc / ϕ + X Baryons (up to 10 each) –B B + X (and c.c.) Open-Charm (up to 20 each) –D D + X / D D* + X (and c.c.) for D decays –D* D* + X / D* D + X (and c.c.) for D* decays In total: up to 791 data types (depending on E cm ) 32 ∙ 20 open charm + 15 ∙ 10 cc/ ϕ /baryons + 10 excl. – 9 (too high E cm ) Mar. 2015K.Goetzen - ST status - CM Giessen9

Event Based Efficiency T D0->Kπ m(Kπ) tag: 1,2 T Λc->pKπ m(pKπ) tag: 3 Only interested in event efficiencies 1.Event with signal X (e.g. D 0 → K π) is tagged by corresponding trigger line due to true/random candidate 2.Event with signal X is tagged by another trigger line due to random candidate (cross tagging) ε tot εXεX Events with X:1, 2, 3 True Cand: Rand. Cand: Accept region: cross tagging Mar. 2015K.Goetzen - ST status - CM Giessen10

Automatized Selection Optimisation For each trigger line each energy, apply procedure: Reconstruct signal candidates based on full event information Perform preselection: cut on inv. mass (+ D* mass diff. cut) Define variables for further selection: –Event shape variables (~ 40) –Candidate specific variables (~ 50, depending on decay) While background fraction for TL > 0.1‰ (0.05 ‰ for E cm >3.5) 1.Inspect all available variables 2.Find variable+cut with max bkg ε signal = 95% relative to previous efficiency (MC truth matched signals) 3.Apply cut on this variable → re-iterate Applied for Fast MC and Full MC Mar. 2015K.Goetzen - ST status - CM Giessen11

Total Background Level vs. E cm (Fast & Full) Mar. 2015K.Goetzen - ST status - CM Giessen12 Fast MC Full MC As expected: 4x more trigger lines 2x harder suppr./TL → 2x total background lvl

Total Efficiencies & Bgk 2.4 GeV (Fast MC) Mar. 2015K.Goetzen - ST status - CM Giessen13 Λ Σ φ e+e-e+e- μ+μ-μ+μ- γγ γπ 0 Efficiencies for different data modes Acceptance of different trigger lines on DPM data ε tot εXεX

Total Efficiencies & Bgk 2.4 GeV (Full MC) Mar. 2015K.Goetzen - ST status - CM Giessen14 Λ Σ φ e+e-e+e- μ+μ-μ+μ- γγ γπ 0 Efficiencies for different data modes Acceptance of different trigger lines on DPM data ε tot εXεX

Total Efficiencies & Bgk 5.5 GeV (Fast MC) For D modes cross tagging is strong effect D0D0 D* 0 D+D+ D* + D s (*)+ c Bary. φ E.M. Efficiencies for different data modes Acceptance of different trigger lines on DPM data Mar. 2015K.Goetzen - ST status - CM Giessen15 ε tot εXεX

Total Efficiencies & Bgk 5.5 GeV (Full MC) Full Sim looks much worse D0D0 D* 0 D+D+ D* + D s (*)+ c Bary. φ E.M. Efficiencies for different data modes Acceptance of different trigger lines on DPM data Mar. 2015K.Goetzen - ST status - CM Giessen16 ε tot εXεX

Total Signal Efficiencies (ε tot ) vs. E cm (Fast MC) (Each point → selection optimization for a energy, N=247 in total) D0D0 D* 0 D+D+ D* + D s (*)+cBary./φ E.M. Mar. 2015K.Goetzen - ST status - CM Giessen17

Total Signal Efficiencies (ε tot ) vs. E cm (Full MC) D0D0 D* 0 D+D+ D* + D s (*)+cBary./φ E.M. (Each point → selection optimization for a energy, N=247 in total) Mar. 2015K.Goetzen - ST status - CM Giessen18

Robustness of Background Level (Fast MC) Training with DPM → apply to events from FTF generator Mar. 2015K.Goetzen - ST status - CM Giessen19 training energies

Prerequisites for "reliable" prediction #SubjectIdealizedRealisticRequires 1Simulation detailFast SimFull Sim 2Simulation streamevent basedevent building (timebased) 3Reco qualityofflineonline8 4Selection observablesunlimitedonline available2,3,8 5Trigger signaturesad-hocrequested/agreed on 6Reliability of bkg shapesingle generatorvarious generators 7Pre-reco BG vetonot neededneeded (i.e. online reco impossible for all events) 2,3 8Implementationstandard PCdedicated hardware Performance expected to drop even more with more realistic simulation. AvailableNot availablePartly available Mar. 2015K.Goetzen - ST status - CM Giessen20

Computing Effort for Scenario Analysis E cm [GeV] Sum Data modes Events [M]* Optimisations Mar. 2015K.Goetzen - ST status - CM Giessen21 *per E cm : 1M bkg events + N x 50k events/signal mode Full Simulation 300,000 jobs on (1000 events/job) –1 week for simulation (2000 cores in parallel) ca. 20 TB of data constisting of –Simulation data (8.5 TB) –SoftTrigger specific output (11.5 TB) 247 automated optimisations on n-tuples & re-application –10 days additional run time

Plans Impact on signal phase space distributions (e.g. Dalitz plots) Further test of robustness of efficiencies/bkg suppression Investigate interpolation of selection algorithms w.r.t. E cm Systematic study of TMVA application –Choice of variables, TMVA types, parameter settings When according ingredients available –Impact of realistic event building & event mixing –Impact of online reco quality –Investigate pre-reco background rejection –Investigate performance issues (e.g. CPU demand) –Extend for: hypernuclei, hadrons in matter Mar. 2015K.Goetzen - ST status - CM Giessen22

Conclusion Studies of extended triggering scheme Developed tools for efficient scenario analysis –Simple configuration of trigger lines/data modes –Automated selection algorithms –Evaluation tools Results of Fast and Full MC differ significantly –Background level < 0.2% over full energy range –Fast MC: Typically ε sig > 20%, up to 50%... 90% –Full MC: Typically ε sig ≈ 10% (better for J/ψ and E.M.) Reliable predictions of performance depend on many more prerequisites not under our control/responsibility –Performance will drop even more –Do we need a plan B? Mar. 2015K.Goetzen - ST status - CM Giessen23

BACKUP

Why a Software Trigger at all? Low signal cross sections σ signal ≈ pb... nb scale → Need high luminosity to achieve enough signal statistics High lumi L = 2·10 32 cm -2 s -1 + large σ tot = mb → Reaction rate up to MHz → Signal fraction ≤ O(10 -4 ) Data rate with 10 kB/event: 200 GB/s Data amount with 50% duty cycle: 3000 PB/year → Completely unaffordable to store and keep all! → Required reduction factor ≈ 1/1000 Signal and background events look very similar Sophisticated event filter on high level information needed! Mar. 2015K.Goetzen - ST status - CM Giessen25

Event Based Efficiency Different cases for positive tag on signal/background 1.Trigger T X tags due to correctly reconstructed candidate X 2.T X tags due to random cand. from event containing signal X 3.T Y tags due to random cand. from event containing signal X 4.T i tags due to random cand. from background TXTX VXVX tag: 1,2 TYTY VYVY tag: 3,4 ε tot εXεX Events with X:1, 2, 3 Background:4 True Cand: Rand. Cand: Accept region: cross tagging Mar. 2015K.Goetzen - ST status - CM Giessen26

Recoils X under study NumberMode 00no recoil 01γ 02π0π0 03η 04π 0 05π+ π-π+ π- 06K + K - 07K0 K0K0 K0 08ηη 09π+ π- π0π+ π- π0 10 different recoils under consideration Not necessarily all recoils are accessible at the same time for a certain E cm Data sets of one signal mode with different recoils are merged → Here: Efficiencies are averaged over recoils (→ possible bias) Mar. 2015K.Goetzen - ST status - CM Giessen27

2.4 GeV (Fast MC) efficiency ε tot εXεX Bary. φ E.M. DPM Mar. 2015K.Goetzen - ST status - CM Giessen28

5.5 GeV (Fast MC) efficiency ε tot εXεX D0D0 D* 0 D+D+ D* + D s (*)+ c Bary. φ E.M. DPM Mar. 2015K.Goetzen - ST status - CM Giessen29

Trigger Line Decay Modes 100 : D0 -> K- pi+ cc 101 : D0 -> K- pi+ pi0 cc 102 : D0 -> K- pi+ pi+ pi- cc 103 : D0 -> K_S0 pi+ pi- cc 104 : D0 -> K_S0 pi+ pi- pi0 cc 110 : D*0 -> D0 [K- pi+] pi0 cc 111 : D*0 -> D0 [K- pi+ pi0] pi0 cc 112 : D*0 -> D0 [K- pi+ pi+ pi-] pi0 cc 113 : D*0 -> D0 [K_S0 pi+ pi-] pi0 cc 114 : D*0 -> D0 [K_S0 pi+ pi- pi0] pi0 cc 115 : D*0 -> D0 [K- pi+] gam cc 116 : D*0 -> D0 [K- pi+ pi0] gam cc 117 : D*0 -> D0 [K- pi+ pi+ pi-] gam cc 118 : D*0 -> D0 [K_S0 pi+ pi-] gam cc 119 : D*0 -> D0 [K_S0 pi+ pi- pi0] gam cc 120 : D+ -> K- pi+ pi+ cc 121 : D+ -> K- pi+ pi+ pi0 cc 122 : D+ -> K_S0 pi+ pi0 cc 123 : D+ -> K_S0 pi+ pi+ pi- cc 130 : D*+ -> D0 [K- pi+] pi+ cc 131 : D*+ -> D0 [K- pi+ pi0] pi+ cc 132 : D*+ -> D0 [K- pi+ pi+ pi-] pi+ cc 133 : D*+ -> D0 [K_S0 pi+ pi-] pi+ cc 134 : D*+ -> D0 [K_S0 pi+ pi- pi0] pi+ cc 135 : D*+ -> D+ [K- pi+ pi+] pi0 cc 136 : D*+ -> D+ [K- pi+ pi+ pi0] pi0 cc 137 : D*+ -> D+ [K_S0 pi+ pi0] pi0 cc 138 : D*+ -> D+ [K_S0 pi+ pi+ pi-] pi0 cc 140 : D_s+ -> K+ K- pi+ cc 141 : D_s+ -> K+ K- pi+ pi0 cc 150 : D*_s+ -> D_s+ [K+ K- pi+] gam cc 151 : D*_s+ -> D_s+ [K+ K- pi+ pi0] gam cc 200 : J/psi -> e+ e- 201 : J/psi -> mu+ mu- 220 : eta_c -> K+ K- pi0 221 : eta_c -> K_S0 K- pi+ cc 222 : eta_c -> gam gam 223 : eta_c -> K+ K- pi+ pi- pi0 224 : eta_c -> K_S0 K- pi+ pi- pi+ cc 240 : chi_0c -> pi+ pi- K+ K- 241 : chi_0c -> K+ pi- K_S0 pi0 cc 400 : Lambda0 -> proton pi- cc 410 : Sigma+ -> proton pi0 cc 420 : Lambda_c+ -> proton K- pi+ cc 421 : Lambda_c+ -> proton K- pi+ pi0 cc 422 : Lambda_c+ -> proton K_S0 pi0 cc 500 : phi -> K+ K- 600 : pbp0 -> e+ e- 601 : pbp0 -> e+ e- gam 602 : pbp0 -> e+ e- pi0 620 : pbp0 -> mu+ mu- 621 : pbp0 -> mu+ mu- gam 622 : pbp0 -> mu+ mu- pi0 640 : pbp0 -> gam gam 641 : pbp0 -> gam gam gam 642 : pbp0 -> gam gam pi0 660 : pbp0 -> pi0 gam Mar. 2015K.Goetzen - ST status - CM Giessen30

Partial tagging w/o reco + event building? Tag part of the signal channels before reco/event building? Mar. 2015K.Goetzen - ST status - CM Giessen31

Partial tagging w/o reco + event building? Tag part of the signal channels before reco/event building? Problems Even with pre reco tags for Sig 1 (≈0.01%) and Sig 2 (≈0.01%) → Full reco needed for 99.98% of events for Sig 3, 4,... Mar. 2015K.Goetzen - ST status - CM Giessen32

Partial tagging w/o reco + event building? Tag part of the signal channels before reco/event building? Problems Even with pre reco tags for Sig 1 (≈0.01%) and Sig 2 (≈0.01%) → Full reco needed for 99.98% of events for Sig 3,... Without event building: What data packages to be stored? Pre-reco tagging only useful as common bkg veto for all signals BkgSig 1Sig 2Sig 3,...Events: Mar. 2015K.Goetzen - ST status - CM Giessen33