Study of the required DIRC resolution

Slides:



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

Phi-Psi, Feb.-Mar., 2006, S.Uehara1 Experimental studies of charmonia in two-photon collisions at Belle S.Uehara (KEK) for the Belle Collaboration e +
USE OF GEANT4 FOR LHCB RICH SIMULATION S. Easo, RAL, LHCB AND ITS RICH DETECTORS. TESTBEAM DATA FOR LHCB-RICH. OVERVIEW OF GEANT4 SIMULATION.
Anne Dabrowski Northwestern University Collaboration Meeting 22 nd February 2005 Update Kmu3 Branching Ratio measurement A. Dabrowski, February
Status Analysis pp -> D s D s0 (2317) Overview Reconstruction Some QA plots Figure of merit First approach/strategy.
Ran my analysis software for position 1-6 from 2006 run. Same data set shown by Jerry at Vienna but my own analysis code version. Still no treatment of.
Sep/15/ Search for   e/ K.Hayasaka(Nagoya U.) Belle Collaboration.
16 April 2005 APS 2005 Search for exclusive two body decays of B→D s * h at Belle Luminda Kulasiri University of Cincinnati Outline Motivation Results.
Study of the semileptonic decays at 4170 MeV Koloina Randrianarivony Marina Artuso (Syracuse University)
MC Study on B°  J/  ° With J/      °     Jianchun Wang Syracuse University BTeV meeting 03/04/01.
Anne Dabrowski Northwestern University NA48/2 Semileptonics Meeting 22 nd February 2005 Update Kmu3 Branching Ratio measurement A. Dabrowski, February.
Status of the OPERA experiment Yoshiaki Nonoyama Nagoya Univ.
Pion test beam from KEK: momentum studies Data provided by Toho group: 2512 beam tracks D. Duchesneau April 27 th 2011 Track  x Track  y Base track positions.
May 31, 2008 SuperB PID sessionMarko Starič, Ljubljana Marko Starič J. Stefan Institute, Ljubljana Report on hardware tests and MC studies in Ljubljana.
Performance of the PANDA Barrel DIRC Prototype 1 GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt 2 Goethe-Universität Frankfurt Marko Zühlsdorf.
Kinematics of  + n   p   0  p reaction Susumu Oda 2007/04/10-19.
Charmonium feasibility study F. Guber, E. Karpechev, A.Kurepin, A. Maevskaia Institute for Nuclear Research RAS, Moscow CBM collaboration meeting 11 February.
Separation power resp. mis id levels Klaus Götzen GSI Darmstadt 25. April 2008.
Mapping separation power Klaus Götzen GSI Darmstadt PID TAG Meeting 15. Feb
Status of GlueX Particle Identification Ryan Mitchell September 10, 2004.
TOP counter overview and issues K. Inami (Nagoya university) 2008/7/3-4 2 nd open meeting for proto-collaboration - Overview - Design - Performance - Prototype.
PID for super Belle (design consideration) K. Inami (Nagoya-u) - Barrel (TOP counter) - Possible configuration - Geometry - Endcap (Aerogel RICH) - Photo.
Simulations Report E. García, UIC. Run 1 Geometry Radiator (water) 1cm x 2cm x 2cm with optical properties Sensitive Volume (hit collector) acrylic (with.
Λ and Σ photoproduction on the neutron Pawel Nadel-Turonski The George Washington University for the CLAS Collaboration.
PANDA GSI 13. December 2006 PID TAG Georg Schepers PANDA Technical Assessment Group PID Status Report G. Schepers for the PID TAG GSI PID TAG.
2004 Fall JPS meeting (English version) K.Okada1 Measurement of prompt photon in sqrt(s)=200GeV pp collisions Kensuke Okada (RIKEN-BNL research center)
Status Report particle identification with the RICH detector Claudia Höhne - GSI Darmstadt, Germany general overview focus on ring radius/ Cherenkov angle.
Magnetized hadronic calorimeter and muon veto for the K +   +  experiment L. DiLella, May 25, 2004 Purpose:  Provide pion – muon separation (muon veto)
Inclusive Measurements of inelastic electron/positron scattering on unpolarized H and D targets at Lara De Nardo for the HERMES COLLABORATION.
Particle Identification. Particle identification: an important task for nuclear and particle physics Usually it requires the combination of informations.
Preliminary Measurement of the Ke3 Form Factor f + (t) M. Antonelli, M. Dreucci, C. Gatti Introduction: Form Factor Parametrization Fitting Function and.
D 0 reconstruction: 15 AGeV – 25 AGeV – 35 AGeV M.Deveaux, C.Dritsa, F.Rami IPHC Strasbourg / GSI Darmstadt Outline Motivation Simulation Tools Results.
BESIII EMC Simulation & Reconstruction He Miao
2005 Unbinned Point Source Analysis Update Jim Braun IceCube Fall 2006 Collaboration Meeting.
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)
04/06/07I.Larin pi0 systematic error 1  0 error budget Completed items (review) Updated and new items (not reported yet) Items to be completed.
Radia Sia Syracuse Univ. 1 RICH 2004 Outline:  The CLEO-III RICH Detector  Physics Requirements  CLEO-III RICH at work… Performance of the CLEO-III.
1 Performance of a Magnetised Scintillating Detector for a Neutrino Factory Scoping Study Meeting U.C. Irvine Monday 21 st August 2006 M. Ellis & A. Bross.
Elliptic flow of D mesons Francesco Prino for the D2H physics analysis group PWG3, April 12 th 2010.
Belle General meeting Measurement of spectral function in the decay 1. Motivation 2. Event selection 3. mass spectrum (unfolding) 4. Evaluation.
Peter Križan, Ljubljana Dec 7, 2007 Mini WS, SLAC Peter Križan University of Ljubljana and J. Stefan Institute Simulations for SuperBelle SuperB computing.
Open and Hidden Beauty Production in 920 GeV p-N interactions Presented by Mauro Villa for the Hera-B collaboration 2002/3 data taking:
Mitglied der Helmholtz-Gemeinschaft Hit Reconstruction for the Luminosity Monitor March 3 rd 2009 | T. Randriamalala, J. Ritman and T. Stockmanns.
14/06/2010 Stefano Spataro Status of LHE Tracking and Particle Identification Status of LHE Tracking and Particle Identification Stefano Spataro III Panda.
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,
1 The Scintillation Tile Hodoscope (SciTil) ● Motivation ● Event timing/ event building/ software trigger ● Conversion detection ● Charged particle TOF.
PhD thesis: Simulation & Reconstruction for the PANDA Barrel DIRC Official name: Open charm analysis tools Supervisor: Prof. Klaus Peters Maria Patsyuk.
PANDA Software Trigger K. Götzen Dec Challenge Required reduction factor: ~1/1000 (all triggers in total) A lot of physics channel triggers → even.
Charmless Hadronic B Decays at BaBar
for Particle Identification
First step to Reconstruction of PANDA Barrel DIRC in PandaRoot
Huagen Xu IKP: T. Randriamalala, J. Ritman and T. Stockmanns
Newt Ganugapati and Teresa Montaruli
Panagiotis Kokkas Univ. of Ioannina
JLEIC Detector Simulation Forward Ion Detection
TORCH – a Cherenkov based Time-of-Flight Detector
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Update on Geometry Tagging (01/19/17)
Software Development for the PANDA Barrel DIRC
Using Single Photons for WIMP Searches at the ILC
LHCb Particle Identification and Performance
Study of e+e- pp process using initial state radiation with BaBar
Prospects for quarkonium studies at LHCb
Backgrounds using v7 Mask in 9 Si Layers at a Muon Higgs Factory
NKS2 Meeting with Bydzovsky NKS2 Experiment / Analysis Status
Vincenzo Vagnoni INFN Bologna CKM Workshop Durham, April 8th 2003
E.A.Kravchenko on behalf Novosibirsk group
ZHH Analysis preliminary results on different detector models
Tau Lepton Flavor Violation Search at Belle, tgmg/eg
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Presentation transcript:

Study of the required DIRC resolution Based on the PID TAG report Toy MC simulation (no particle tracking, all the detector responses are parametrized) using macros from Klaus G. Basic DIRC parameters (assuming the simple geometry): SPR = 18 mrad (10 – in PID TAG report) Photodetector efficiency = 8.8 % (7.5%) Tracking resolution = 1 mrad (0 mrad) N photons is parametrized (λ1 = 290nm, λ2 = 580nm): P = 3 GeV/c, Photon yield used for PID TAG report (λ1 = 280nm, λ2 = 330nm) Most crutial region P = 3 GeV/c, blue line – PandaRoot, red – parametrization

Barrel DIRC parametrized signal Assuming gaussian signals, the DIRC output: Θ c and σ for each particle type, momentum, polar angle, σ2 = (SPR/sqrt(N γ)) + σ corr 2 Θ c (p, type, naverage) Approaches: 1. cut is defined by the separation power (as in PID TAG report) 2. the efficiency of K id is fixed to 95%, thus the cut is defined

Separation power/mis-id maps (as in PID TAG)

Mis-id maps (eff = 95%) Mis-id map for PID TAG approach to compare:

Efficiency maps (mis-id = 1%) Efficiency map for PID TAG approach to compare:

Calculation of mis-id for some channels #Lambda^{0}#bar{#Lambda}^{0} llbar DPM dpm 1.460 #phi#phi 2phi 2#pi^{+}2#pi^{-} 4pi 1.500 #phi#phi 2phi 3#pi^{+}3#pi^{-} 6pi 1.500 #Lambda^{0}#bar{#Lambda}^{0} llbar #Sigma^{0}#bar{#Sigma}^{0} 2sigma 1.914 #Lambda^{0}#bar{#Lambda}^{0} llbar #Sigma^{0}#bar{#Sigma}^{0} 2sigma 3.101 #Omega^{-}#bar{#Omega}^{+} omom DPM dpm 4.954 J/#psi2#pi^{0} jpsi2pi0 #pi^{+}#pi^{-}2#pi^{0} 2pi2pi0 5.609 J/#psi#pi^{+}#pi^{-} jpsi2pi 2#pi^{+}2#pi^{-} 4pi 5.609 #phi#phi 2phi 2#pi^{+}2#pi^{-} 4pi 6.000 #phi#phi 2phi 3#pi^{+}3#pi^{-} 6pi 6.000 #Lambda^{0}#bar{#Lambda}^{0} llbar #Sigma^{0}#bar{#Sigma}^{0} 2sigma 6.000 J/#psi#eta jpsieta 3#pi^{+}3#pi^{-} 6pi 6.080 J/#psi#eta jpsieta 2#pi^{+}2#pi^{-} 4pi 6.080 J/#psi2#pi^{0} jpsi2pi0 #pi^{+}#pi^{-}2#pi^{0} 2pi2pi0 6.232 J/#psi#pi^{+}#pi^{-} jpsi2pi 2#pi^{+}2#pi^{-} 4pi 6.232 D^{0}#bar{D}^{0}#gamma 2d0gam DPM dpm 6.488 D^{+}D^{-}#gamma 2dpm DPM dpm 6.488 J/#psi#pi^{+}#pi^{-} jpsi2pi 2#pi^{+}2#pi^{-} 4pi 6.988 J/#psi#eta jpsieta 3#pi^{+}3#pi^{-} 6pi 6.990 J/#psi#eta jpsieta 2#pi^{+}2#pi^{-}#pi^{0} 4pipi0 6.990 J/#psi#eta jpsieta 2#pi^{+}2#pi^{-} 4pi 6.990 D_{s}^{+}D_{s}^{-}#gamma 2dspmgam DPM dpm 7.314 D*^{+}D*^{-}#gamma 2dstpmgam DPM dpm 7.746 D*^{0}#bar{D}*^{0}#gamma 2dst0gam DPM dpm 7.746 D_{s}^{+}D_{s}^{-}#gamma 2dspmgam DPM dpm 7.746 #Lambda^{0}#bar{#Lambda}^{0} llbar DPM dpm 8.000 D*^{0}#bar{D}*^{0}#gamma 2dst0gam DPM dpm 8.000 D^{+}D^{-}#gamma 2dpm DPM dpm 8.000 D^{0}#bar{D}^{0}#gamma 2d0gam DPM dpm 8.000 D_{s}^{+}D_{s}^{-}#gamma 2dspmgam DPM dpm 8.000 D*^{+}D*^{-}#gamma 2dstpmgam DPM dpm 8.000 J/#psi#pi^{+}#pi^{-} jpsi2pi 2#pi^{+}2#pi^{-} 4pi 8.682 D_{s}^{+}D_{s}^{-}#gamma 2dspmgam DPM dpm 12.000 64 channels were taken into account for PID TAG report, Instead of punching out the bkg 1. overlay the signal (in p,theta coord) with the mis-id map 2. calculate the average mis-id by averaging over all signal bins located on the color map.

Mis-id for some channels (as in PID TAG report) Maximal mis-id Mis-id for some channels (as in PID TAG report) 15 channels out of 60 have mis-id>0.5% and >50 particles in the signal plot (out of 10000 ev)

Mis-id for some channels (eff=95%) Maximal mis-id Mis-id for some channels (eff=95%) 13 channels out of 60 have mis-id>0.5% and >50 particles in the signal plot (out of 10000 ev)