1 NCC Task Force Richard Seto NCC Task Force Meeting Jan 8, 2007 BNL.

Slides:



Advertisements
Similar presentations
Tentative flow chart of CMS Multi-Muon analysis 1 – DATASETS 2 - RESOLUTIONS 3 – FAKE RATES 4 – NUCLEAR INT MODEL 5 – IP TEMPLATES MODEL 6 – SAMPLE COMPOSITION.
Advertisements

Measurement of charmonia at mid-rapidity at RHIC-PHENIX  c  J/   e + e -  in p+p collisions at √s=200GeV Susumu Oda CNS, University of Tokyo For.
10/03/'06 SPIN2006, T. Horaguchi 1 Measurement of the direct photon production in polarized proton-proton collisions at  s= 200GeV with PHENIX CNS, University.
Xiaorong Wang, SQM Measurement of Open Heavy Flavor with Single Muons in pp and dAu Collisions at 200 GeV Xiaorong Wang for PHENIX collaboration.
Status Analysis pp -> D s D s0 (2317) Overview Reconstruction Some QA plots Figure of merit First approach/strategy.
Ali Hanks - APS Direct measurement of fragmentation photons in p+p collisions at √s = 200GeV with the PHENIX experiment Ali Hanks for the PHENIX.
Forward Calorimeter Upgrades in PHENIX: Past and Future Richard Hollis for the PHENIX Collaboration University of California, Riverside Winter Workshop.
Cold Nuclear Matter Effects on Open Heavy Flavor at RHIC J. Matthew Durham for the PHENIX Collaboration Stony Brook University
Sept 30 th 2004Iacopo Vivarelli – INFN Pisa FTK meeting Z  bb measurement in ATLAS Iacopo Vivarelli, Alberto Annovi Scuola Normale Superiore,University.
A simulation study of the rapidity distributions of leptons from W boson decays at ATLAS Laura Gilbert.
Sourav Tarafdar Banaras Hindu University For the PHENIX Collaboration Hard Probes 2012 Measurement of electrons from Heavy Quarks at PHENIX.
1 NCC Task Force Richard Seto NCC Task Force Meeting Dec 14, 2007 BNL.
M. Brooks, LANL 1 Physics and Simulation Status and To-Dos Physics Section could probably use a top-down re-write. Most of the info is probably there but.
Alexander Khanov 25 April 2003 DIS’03, St.Petersburg 1 Recent B Physics results from DØ The B Physics program in D Ø Run II Current analyses – First results.
Sevil Salur for STAR Collaboration, Yale University WHAT IS A PENTAQUARK? STAR at RHIC, BNL measures charged particles via Time Projection Chamber. Due.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
Single Electron Measurements at RHIC-PHENIX T. Hachiya Hiroshima University For the PHENIX Collaboration.
Direct photons at low p t measured in PHENIX D.Peressounko RRC “Kurchatov institute” for the PHENIX collaboration.
Mock Data Challenge PbPb collisions - July 2010 Prashant Shukla Nuclear Physics Division BARC, Mumbai India 1 India CMS, July 2010, BARC, Mumbai.
Observation of W decay in 500GeV p+p collisions at RHIC Kensuke Okada for the PHENIX collaboration Lake Louise Winter Institute February 20, /20/20101.
R CP Measurement with Hadron Decay Muons in Au+Au Collisions at √s NN =200 GeV WooJin Park Korea University For the PHENIX Collaboration.
 Production at forward Rapidity in d+Au Collisions at 200 GeV The STAR Forward TPCs Lambda Reconstruction Lambda Spectra & Yields Centrality Dependence.
Charmonium feasibility study F. Guber, E. Karpechev, A.Kurepin, A. Maevskaia Institute for Nuclear Research RAS, Moscow CBM collaboration meeting 11 February.
Heavy flavor results from PHENIX at RHIC Raphaël Granier de Cassagnac on behalf of the PHENIX collaboration LLR – École polytechnique / IN2P3 Deep Inelastic.
Preliminary analysis of p-Pb data update n. 6 Lorenzo Bonechi LHCf Catania meeting – 19 December 2013.
Open charm hadron production via hadronic decays at STAR
Recent Charm Measurements through Hadronic Decay Channels with STAR at RHIC in 200 GeV Cu+Cu Collisions Stephen Baumgart for the STAR Collaboration, Yale.
M. Brooks, 17-Jul-03 PHENIX Review July 17, 2003 p-p Physics from Muon Arm—J/  Melynda Brooks RHIC and the PHENIX Detector Physics Goals of the PHENIX.
Charm and J/PSI measurement at RHIC Y. Akiba (KEK) August 9, 2002 Riken Summer study 2002.
Measurement of J/  -> e + e - and  C -> J/  +   in dAu collisions at PHENIX/RHIC A. Lebedev, ISU 1 Fall 2003 DNP Meeting Alexandre Lebedev, Iowa State.
Measurements of thermal photons in heavy ion collisions with PHENIX - Torsten Dahms - Stony Brook University February 8 th, 2008 Real photons at low p.
DPF2000, 8/9-12/00 p. 1Richard E. Hughes, The Ohio State UniversityHiggs Searches in Run II at CDF Prospects for Higgs Searches at CDF in Run II DPF2000.
Prospects in ALICE for  mesons Daniel Tapia Takaki (Birmingham, UK) for the ALICE Collaboration International Conference on STRANGENESS IN QUARK MATTER.
M. Muniruzzaman University of California Riverside For PHENIX Collaboration Reconstruction of  Mesons in K + K - Channel for Au-Au Collisions at  s NN.
2004 Fall JPS meeting (English version) K.Okada1 Measurement of prompt photon in sqrt(s)=200GeV pp collisions Kensuke Okada (RIKEN-BNL research center)
Measurement of photons via conversion pairs with PHENIX at RHIC - Torsten Dahms - Stony Brook University HotQuarks 2006 – May 18, 2006.
LHCb: Xmas 2010 Tara Shears, On behalf of the LHCb group.
Ralf Averbeck Stony Brook University Hot Quarks 2004 Taos, New Mexico, July 19-24, 2004 for the Collaboration Open Heavy Flavor Measurements with PHENIX.
STAR J/  Trigger in dA Manuel Calderon for the Heavy-Flavor Group Trigger Workshop at BNL October 21, 2002.
Mike Miller First measurement of the inclusive jet cross section in p+p collisions at E CM =200 GeV M.L. Miller (MIT) Motivations: 1.Baseline for inclusive.
JPS 2003 in Sendai Measurement of spectral function in the decay 1. Motivation ~ Muon Anomalous Magnetic Moment ~ 2. Event selection 3. mass.
STAR Collaboration Meeting, BNL – march 2003 Alexandre A. P. Suaide Wayne State University Slide 1 EMC Update Update on EMC –Hardware installed and current.
STAR Analysis Meeting, BNL – oct 2002 Alexandre A. P. Suaide Wayne State University Slide 1 EMC update Status of EMC analysis –Calibration –Transverse.
Longitudinal Spin Asymmetry and Cross Section of Inclusive  0 Production in Polarized p+p Collisions at 200 GeV Outline  Introduction  Experimental.
Search for High-Mass Resonances in e + e - Jia Liu Madelyne Greene, Lana Muniz, Jane Nachtman Goal for the summer Searching for new particle Z’ --- a massive.
NCC simulation update DC meeting Oct 3, 2007 BNL.
NCC meeting Aug 5, 2008 richard seto. doe report received /
PHENIX results on J/  production in Au+Au and Cu+Cu collisions at  S NN =200 GeV Hugo Pereira Da Costa CEA Saclay, for the PHENIX collaboration Quark.
1 NCC CDR prep and Physics strategy Richard Seto UCR DC Upgrades meeting Feb 8, 2006.
Mike HildrethEPS/Aachen, July B Physics Results from DØ Mike Hildreth Université de Notre Dame du Lac DØ Collaboration for the DØ Collaboration.
Penny Kasper Fermilab Heavy Quarkonium Workshop 21 June Upsilon production DØ Penny Kasper Fermilab (DØ collaboration) 29 June 2006 Heavy Quarkonium.
06/2006I.Larin PrimEx Collaboration meeting  0 analysis.
Mid-rapidity pi0 production in pp collisions at sqrt(s)=62 and 200 GeV measured by the PHENIX detector at RHIC A.Bazilevsky Brookhaven National Laboratory.
HI July Exercise and Muon DQM preparation Mihee Jo Mihee Jo / Lab meeting.
 -jet measurements Table of Contents:  Motivation  Preliminary QA of  -trigger Data  Shower Shape Analysis  Experimental Challenges  Summary  
Measurement of photons via conversion pairs with the PHENIX experiment at RHIC - Torsten Dahms - Master of Arts – Thesis Defense Stony Brook University.
Belle General meeting Measurement of spectral function in the decay 1. Motivation 2. Event selection 3. mass spectrum (unfolding) 4. Evaluation.
Systematic measurement of light vector mesons at RHIC-PHNEIX Yoshihide Nakamiya Hiroshima University, Japan (for the PHENIX Collaboration) Quark Matter.
Masashi Kaneta, RBRC, BNL 2003 Fall Meeting of the Division of Nuclear Physics (2003/10/31) 1 KANETA, Masashi for the PHENIX Collaboration RIKEN-BNL Research.
V. Pozdnyakov Direct photon and photon-jet measurement capability of the ATLAS experiment at the LHC Valery Pozdnyakov (JINR, Dubna) on behalf of the HI.
I'm concerned that the OS requirement for the signal is inefficient as the charge of the TeV scale leptons can be easily mis-assigned. As a result we do.
PHENIX J/  Measurements at  s = 200A GeV Wei Xie UC. RiverSide For PHENIX Collaboration.
Quark Matter 2002, July 18-24, Nantes, France Dimuon Production from Au-Au Collisions at Ming Xiong Liu Los Alamos National Laboratory (for the PHENIX.
Upsilon production and μ-tagged jets in DØ Horst D. Wahl Florida State University (DØ collaboration) 29 April 2005 DIS April to 1 May 2005 Madison.
Performance Evaluation for Open Charm and Beauty Measurement at LHC ALICE PID capability from λ and K s 0 measurement at LHC ALICE 筑波大学数理物質科学研究科 Kengo.
Elena Bruna Yale University
Quarkonium production in ALICE
Kazuya Aoki For the PHENIX Collaborations. Kyoto Univ. / RIKEN
20th International Conference on Nucleus Nucleus Collisions
Inclusive p0 Production in Polarized pp Collisions using the STAR Endcap Calorimeter Jason C. Webb, Valparaiso University, for the STAR Collaboration Outline.
Presentation transcript:

1 NCC Task Force Richard Seto NCC Task Force Meeting Jan 8, 2007 BNL

2 Agenda Assessment of where we are and time schedule - plans for work over the holiday. I would like to hear reports from everyone as usual. 1) Dave/stefan - pi0's - could I get a plot or something to show (or a slide)to the DC and an update 2) Ken/Paul/Todd - same for spin 3) Takao - plan for the direct photon. (a slide or so for summary to the DC)

3 The Document The goals in simplest terms for the NCC task force is to produce the following figure of merit (FOM) plots from realistic physics simulations. Realistic means a full simulation using PISA with detector response, reconstruction, and data analysis. a) R_AA for pi0 as a function of pt for various centralities in AuAu and dAu collisions b) Direct photons cross sections, and likewise R_AA. c) R_AA for the Chi_C via its decay to J/psi photon as a function of pt for various centralities. Very likely we will limit this to rapidity d) A_LL(pt) for direct photons in 500 GeV polarized pp collisions d') Because we already have jet reconstruction going in pp collisions we should easily be able to use this information to get A_LL(x) giving a greater sensitivity to low-x e) a demonstration that we can we can extract pi0's at various angles in various centrality collisions with a known efficiency - This should answer the projective Geometry question. Schedule To collaboration – Jan 20 To DOE – End of Jan HI spin answer to committee

4 comments from axel What is missing all together are slides addressing b) the direct photons and more specifically e). For e) one more technical slide explaining that the NCC has "tracking capability" and showing reconstruction efficiencies as function of function of impact angle for different pt and maybe vertex positions should be sufficient to address the issue. For the next two the single track pi0 is critical b) you might consider, and I do not know how much work that is, comparing a MC input spectrum for single photons with the reconstructed one plus and R_AA plot. Spin(RKS added this)

5 Status of simulation effort Full GEANT based simulation (PISA) Full reconstruction and PID pattern recognition of showers in PADS (stripixels have not been incorporated into pattern recongnition stage) energy and rapidity dependent calibrations of sampling fraction and energy corrections Particle Identification using longitudinal and transverse shower shapes – also function of energy and rapidity – transverse shower shapes using both pads and stripixels Single track pi0 using stripixels done generation of signal and underlying event – with signal being embedded into underlying event when necessary. Analysis of events. Mixed event technique used to extract backgrounds

6 Critical simulation analysis goals reconstruction pi0’s in pp to AuAu From this projective geometry question can be answered R_AA can be formed From this direct photons can be extracted for heavy ion direct photon analysis for Delta G from direct photon A_LL status: 2 gamma complete – this will take us to pt~4 GeV single gamma is running at RCF reconstruct chic pp to AuAu R_AA for chic status: complete to mid-central AuAu central AuAu running at RCF

7 π 0  2 γ pp to central AuAu 10K events simulated for AuAu (real data ~10 9 events) AuAu 40-50% AuAu 20-30% AuAu 10-20% AuAu 0-10% AuAu 60-80% y=1-1.5 pt=2-2.5 dAu mb dAu cent 20% y=1-1.5 pt=1.5-2 ppmb 200 GeV ppmb 200 GeV y= pt= y=1-1.5 pt=1.5-2 pp mb 500 GeV pp mb 500 GeV y=1.5-2 pt= pp mb y=1-1.5 pt=2-2.5 y=1-1.5 pt=2.5-3 y=1-1.5 pt=2.5-3 y=1-1.5 pt=2.5-3 y=1-1.5 pt=2-2.5 y=1-1.5 pt=2-2.5 y=1-1.5 pt=2-2.5

8 Single track pi0’s Jobs running at RCF

9 R_AA stat error only – 2 gamma y=1-1.5 single track takes over Assumed AuAu – 10B min bias events (since is 10% of cross section) scale error bars by 3 for 1B

10 χ C pp to AuAu 40-50% central Embed χ C and J/  in appropriate ratio where χ C  J/  + γ in pp min bias Dimuon decay of J/  measured in muon arms plot J/  + γ mass – J/  mass Mixed bkg: J/  + γ mass – J/  +γ mass mixed event, normalized above 1.6 MeV mixed bkg foreground All y – (jobs for lower pt, y bins, and most central AuAu running at RCF) pt=5-6 pt=7-8 pt=9-10 pt=5-6 pt=7-8 pt=9-10 pt=5-6 pt=7-8 pt=9-10 pt=5-6 pt=7-8 pt=9-10 ppmb dAu mb dAu 0-20% AuAu 40-50% M(J/  +γ)-M(J/  ) subtracted χCχC

11 Chi_C R_AA should be straightforward once RCF jobs complete latest error on this point (stat) is 8% using pt>3 i.e old prediction is unchanged R_AA of chic present J/psi r_AA data 50-60% central

12 sweet spot note change in scale for GSC pi0 ~ little asymmetry Done Weight scheme to input spin info implemented Prompt photon events generated and made to be consistent with NLO pQCD calculations. A LL vs. p T done for PYTHIA and in agreement with earlier calculations. Error bars assuming no background GRSV models added to weighting scheme Note: for pi0 we find very little asymmetry (consistent with Volgesang)  pi0 background will not contaminate direct photon asymmetry To do Calculate error bars with background using reconstructed direct photons Plot vs reconstructed p T Spin update