PHENIX Measurement of Parity-Violating Single Spin Asymmetry in W Production in p+p Collisions at 500 GeV Stephen Pate (for the PHENIX Collaboration) New.

Slides:



Advertisements
Similar presentations
Longitudinal Spin at RHIC 29 th Winter Workshop on Nuclear Dynamics February 7, 2013 Cameron McKinney.
Advertisements

Determination of the gluon polarisation at COMPASS & RHIC Sébastien Procureur (CEA - Saclay) Determination of  G at COMPASS & RHICPAVI06, Milos S.Procureur.
Commissioning the PHENIX RPC Forward Trigger Upgrade Michael Daugherity Abilene Christian University for the PHENIX Collaboration.
» Drell RHIC « Oleg Eyser ECT* Workshop on Drell Yan Physics and the Structure of Hadrons May 21-25, 2012, Trento, Italy.
1 Run 9 PHENIX Goals and Performance John Haggerty Brookhaven National Laboratory June 4, 2009.
PHENIX Decadal Plan o Midterm upgrades until 2015 o Long term evolution after 2015 Dynamical origins of spin- dependent interactions New probes of longitudinal.
Carl Gagliardi – DIS2008 – Jets in pp at RHIC 1 Jet Production in Polarized pp Collisions at RHIC Carl A. Gagliardi Texas A&M University for the Collaboration.
Constraining the polarized gluon PDF in polarized pp collisions at RHIC Frank Ellinghaus University of Colorado (for the PHENIX and STAR Collaborations)
09/30/'06SPIN2006, T. Horaguchi1 Measurement of the direct photon production in polarized proton-proton collisions at  s= 200GeV with PHENIX CNS, University.
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.
Forward Calorimeter Upgrades in PHENIX: Past and Future Richard Hollis for the PHENIX Collaboration University of California, Riverside Winter Workshop.
J. Seele - WWND 1 The STAR Longitudinal Spin Program Joe Seele (MIT) for the Collaboration WWND 2009.
Mar. 17, 2006 Imran Younus Probing Gluon Polarization with Longitudinally Polarized p+p Collisions at  s = 200 GeV.
The Physics Potential of the PHENIX VTX and FVTX Detectors Eric J. Mannel WWND 13-Apr-2012.
Sourav Tarafdar Banaras Hindu University For the PHENIX Collaboration Hard Probes 2012 Measurement of electrons from Heavy Quarks at PHENIX.
1 The Study of D and B Meson Semi- leptonic Decay Contributions to the Non-photonic Electrons Xiaoyan Lin CCNU, China/UCLA for the STAR Collaboration 22.
Xiaoyan LinQuark Matter 2006, Shanghai, Nov , Study B and D Contributions to Non- photonic Electrons via Azimuthal Correlations between Non-
Status of W analysis in PHENIX Central Arm Kensuke Okada (RBRC) For the PHENIX collaboration RHIC Spin Collaboration meeting November 21, /21/20091K.Okada.
Spin of the proton and its transverse spin structure at RHIC HERMES seminar at Tokyo Tech November 9, 2005 Yuji Goto (RIKEN)
Single Electron Measurements at RHIC-PHENIX T. Hachiya Hiroshima University For the PHENIX Collaboration.
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.
Longitudinal Spin Physics at RHIC and a Future eRHIC Brian Page Brookhaven National Laboratory CIPANP 2015 – Vail, CO.
1 RSC2006—Sept. 30, 2006 Kieran Boyle Recent Results from PHENIX Longitudinal Spin Program Kieran Boyle (Stony Brook U.) for the PHENIX Collaboration Outline:
PHENIX Local Polarimeter PSTP 2007 at BNL September 11, 2007 Yuji Goto (RIKEN/RBRC)
Spin Physics with PHENIX (an overview, but mainly  G) Abhay Deshpande Stony Brook University RIKEN BNL Research Center July 28, 2011.
Heavy flavor production at RHIC Yonsei Univ. Y. Kwon.
What can we learn from η production in proton-proton collisions? Joe Seele MIT and University of Colorado.
The W program at PHENIX R. Seidl (University of Illinois and RBRC) for the PHENIX Collaboration Workshop on Parity Violating Spin Asymmetries BNL, April.
ECT* workshop “Flavor structure of the nucleon sea” Trento July 1 st, 2013 Ralf Seidl (RIKEN)
Recent Charm Measurements through Hadronic Decay Channels with STAR at RHIC in 200 GeV Cu+Cu Collisions Stephen Baumgart for the STAR Collaboration, Yale.
Neutral Current Deep Inelastic Scattering in ZEUS The HERA collider NC Deep Inelastic Scattering at HERA The ZEUS detector Neutral current cross section.
GGGG 05/27/2008 5/27/08 The STAR Longitudinal Spin Program Outline: 1) The Spin Puzzle 2) The STAR Experiment 3) Inclusive Jet Results 4) Inclusive.
Searching for Polarized Glue at Brian Page – Indiana University For the STAR Collaboration June 17, 2014 STAR.
J/  production in p+p collisions at PHENIX and gluon distribution QWG meeting at FNAL September Hiroki Sato (Kyoto University) for the PHENIX collaboration.
Oct 6, 2008Amaresh Datta (UMass) 1 Double-Longitudinal Spin Asymmetry in Non-identified Charged Hadron Production at pp Collision at √s = 62.4 GeV at Amaresh.
2004 Fall JPS meeting (English version) K.Okada1 Measurement of prompt photon in sqrt(s)=200GeV pp collisions Kensuke Okada (RIKEN-BNL research center)
Kyoto Univ. RIKEN Katsuro Nakamura (Kyoto University) 2012/ 2/ 13 Kyoto University GCOE Symposium 2012/2/131 Kyoto University GCOE Symposium.
Recent Open Heavy Flavor Results from ATLAS and CMS Experiment at LHC
Transverse Single-Spin Asymmetries Understanding the Proton: One of the fundamental building blocks of ordinary matter! Spin decomposition of proton still.
First measurement and future prospects for measurements of single spin asymmetries in W production with the PHENIX experiment at RHIC Young Jin Kim for.
1/27/2016 R.Seidl: status of simulation1 W muon analysis in PHENIX Status of the background understanding, signal, smearing and asymmetries R.Seidl (RBRC)
MPC-EX hardware design and capability The MPC-EX detector system is an extension of the existing Muon Piston Calorimeters (MPCs) of the PHENIX experiment.
Longitudinal Spin Asymmetry and Cross Section of Inclusive  0 Production in Polarized p+p Collisions at 200 GeV Outline  Introduction  Experimental.
 Production and Suppression in Heavy Ion Collisions at STAR Anthony Kesich University of California, Davis STAR Collaboration February 5, 2013.
JPS/DNPY. Akiba Single Electron Spectra from Au+Au collisions at RHIC Y. Akiba (KEK) for PHENIX Collaboration.
10/27/2005J. Lajoie - PANIC '051 The PHENIX Forward Upgrade Topics: A (Brief) Spin Physics Motivation Antiquark Spin Contribution with W +/- bosons The.
W Boson Production in Polarized p+p Collisions at th Justin Stevens LANL P-25 Seminar.
Measurement of the Double Longitudinal Spin Asymmetry in Inclusive Jet Production in Polarized p+p Collisions at 200 GeV Outline Introduction RHIC.
Gluon Polarization Errors at PHENIX Spin Discussion Mar. 24 & Apr. 14, 1998 Yuji Goto, RIKEN.
1 STAR Double Longitudinal Spin Asymmetries of Inclusive Charged Pion Production in Polarized p+p Collisions at 200 GeV Adam Kocoloski, MIT For the STAR.
Oct. 12, 2007 Imran Younus k T Asymmetry in Longitudinally Polarized p +p Collisions at PHENIX.
Longitudinal Spin Asymmetry Measurements at PHENIX DNP/JPS joint meeting in Hawaii September 18, 2005 Yuji Goto (RIKEN/RBRC) for the PHENIX collaboration.
1 Prompt Photon Production from Proton - proton Collisions at √s = 62.4 GeV in PHENIX ( PHENIX 実験における重心系 62.4 GeV での陽子 - 陽子衝突からの 直接光子の生成断面積の測定 ) JPS meeting.
Spin Physics with PHENIX (an overview, but mainly  G) Abhay Deshpande Stony Brook University RIKEN BNL Research Center PANIC’11 at MIT July 28, 2011.
Reduction of Background in Observation of W Decay Using the Forward Vertex (FVTX) detector at PHENIX Abraham Meles New Mexico State University APS April.
Inclusive cross section and single transverse-spin asymmetry of very forward neutron production at PHENIX Spin2012 in Dubna September 17 th, 2012 Yuji.
Gluon polarization and jet production at STAR Pibero Djawotho for the STAR Collaboration Texas A&M 4 June 2013.
Overview of the sea quark polarization measurements of PHENIX at RHIC DIS April 12, Rusty Towell Abilene Christian University on behalf of the PHENIX.
Jamaica 11 Jan.8, 2009 Muon Trigger Upgrade at PHENIX RIKEN/RBRC Itaru Nakagawa RIKEN/RBRC Itaru Nakagawa.
Reduction of background in observation of W – decay using FVTX tracker Abraham Meles New Mexico State University DNP2012 – Newport Beach, CA. Oct 25, 2012.
Recent Results on Proton Helicity Structure Studies from PHENIX
First physics from the ALICE electromagnetic calorimeters
Kieran Boyle (Stony Brook University) for the PHENIX Collaboration
Transverse Spin Physics at PHENIX
Mickey Chiu University of Illinois at Urbana-Champaign
Katarzyna Kowalik (LBNL) For the STAR Collaboration
Kazuya Aoki For the PHENIX Collaborations. Kyoto Univ. / RIKEN
APS/JPS Second Joint Meeting Sep. 19, 2005
Run 12 Sea Quark Polarization:
Inclusive p0 Production in Polarized pp Collisions using the STAR Endcap Calorimeter Jason C. Webb, Valparaiso University, for the STAR Collaboration Outline.
Presentation transcript:

PHENIX Measurement of Parity-Violating Single Spin Asymmetry in W Production in p+p Collisions at 500 GeV Stephen Pate (for the PHENIX Collaboration) New Mexico State University 12 September 20101Diffraction 2010

12 September 2010Diffraction DSSV Global Fit -- PRD80 (2009) [ ] Over many years, the worldwide program of form factor measurements, inclusive deep- inelastic and semi-inclusive deep-inelastic scattering has made possible a definitive measurement of the polarized PDFs of the u and d quarks. But the contribution of the sea and gluons to the spin of the proton remains relatively unclear.

12 September 2010Diffraction l+l+ is measuring asymmetries in W production that are sensitive to the light quark sea contribution to the proton spin.

Diffraction STAR RHIC-PHENIX 2009 run Run 09: First 500 GeV Run, March 17-April 13, 2009 Machine development in parallel with physics running to increase luminosity, polarization Integrated luminosity (with vertex cut) is  Ldt=8.6 pb -1 Polarization is =0.39±0.04 (scale uncertainty) Spin Rotators Siberian Snake pC and H-jet polarimeters Siberian Snake 12 September 2010

Polarization Measured with two polarimeters – CNI polarimeter measurements available during run – H jet polarimeter provides absolute polarization – Measured residual polarization in real time after rotation at PHENIX 12 September Polarization measured by CNI polarimeters fill-by-fill P P Diffraction 2010

6 EMC 4x4 Tower Sum Trigger ±30 cm vertex cut High energy EM Calorimeter clusters matched to charged track Loose timing cut to reduce cosmic ray bkg Loose E/p cut PHENIX Central arm: W  e  Central Arm Acceptance : |  |<0.35 in rapidity 2 arms covering  =  e Fully efficient at 12 GeV 12 September 2010

Diffraction Clusters Smooth spectrum of EMC clusters after removing bad towers Effect of Cuts 12 September 2010

Diffraction Clusters Good track match Smooth spectrum of EMC clusters after removing bad towers Have a good track pointing to an EMC cluster 12 September 2010 Effect of Cuts

Diffraction Clusters Good track match TOF cut Smooth spectrum of EMC clusters after removing bad towers Have a good track pointing to an EMC cluster Timing within start time of collision Reduces out of time backgrounds (cosmics) by ~80% 12 September 2010 Effect of Cuts

Diffraction Clusters Good track match TOF cut E/p Smooth spectrum of EMC clusters after removing bad towers Have a good track pointing to an EMC cluster Timing within start time of collision Reduces out of time backgrounds (cosmics) by ~80% E/P cut 12 September 2010 Effect of Cuts

Diffraction QCD provides the most obvious background (W. Vogelsang) Not shown here but very important Cosmics and photons (from meson decays and direct), which can have accidental matches to tracks or conversions c/b relatively small above 30 GeV, calculated at FONLL (Matteo Carciari) Z/  * background is estimated from PYTHIA (~1 count is expected in Run09). W  e is also small 12 September 2010 Signal and Background

Diffraction QCD provides the most obvious background (W. Vogelsang) Not shown here but very important Cosmics and photons (from meson decays and direct), which can have accidental matches to tracks or conversions c/b relatively small above 30 GeV, calculated at FONLL (Matteo Carciari) Z/  * background is estimated from PYTHIA (~1 count is expected in Run09). W  e is also small 12 September 2010 Hadron spectrum suppressed by poor response of EMC to hadrons Signal and Background

12 September 2010Diffraction Background subtracted spectra of positron and electron candidates Gray bands = range of background estimates. Compared to spectrum of W and Z decays from a NLO calculation [D. de Florian and W. Vogelsang, Phys. Rev. D81, (2010). P. M. Nadolsky and C. P. Yuan, Nucl. Phys. B666, 31 (2003)] These yields were used for cross section results. For the asymmetry measurement, additional cuts were applied to make the background contribution negligible.

12 September 2010Diffraction Isolation Cut – use fact that lepton from W decay is not from a jet  E < 2GeV Sum up energy in a cone around electron/positron >80% of signal is kept (blue dashed line) Factor ~4 reduction in background

12 September 2010Diffraction Signal for Asymmetry Measurement After Isolation Cut Positrons: 42 signal events (background 1.7  1.0) Electrons: 13 signal events (background 1.6  1.0) Signal region is 30 < p T < 50 GeV/c

12 September 2010Diffraction Longitudinal spin asymmetry A L Parity-violating longitudinal single spin asymmetry N + = right-handed production of W N - = left-handed production of W P = Polarization R = relative luminosities of the helicity states D = dilution by background and Z 0

12 September 2010Diffraction Parity-violating Asymmetries In W Production in PHENIX Final Results for RHIC 2009 Run [arXiv: ] Direct observation of parity-violation in W production. Likelihood function used to determine value and limits for A L (low statistics)

Muon Trigger Upgrade muID north muID south muTr north muTr south Existing Muon Arms: muID (triggering) muTr (tracking) trigger rejection ~ September Diffraction 2010

Muon Trigger Upgrade RPC1(a,b) RPC3 muID north muID south muTr north muTr south muTr-trigger Existing Muon Arms: muID (triggering) muTr (tracking) trigger rejection ~ Upgrade: 1) muTr trigger electronics: muTr 1-3  send tracking info to level-1 trigger 2) RPC stations: RPC 1+3  tracking + timing info to level-1 trigger Trigger idea: Reject low momen- tum muons Cut out-of-time beam background 12 September Diffraction 2010

RPCs: trigger level timing Timing used in Run-9 to characterize background RPC3-N installed for Run- 10 Commissioned & ready From collision or out going beam From beam background Test assembly of RPC-3 half octant support structure at UIUC 12 September Diffraction 2010

MUTRIG ready for physics in 2011 Run Minimum Ionizing Particle Good efficiency for MIPs MUTR.N installed for Run-9 MUTR.s installed for Run-10 ready to go Station 1 Station 2 Station 3 12 September Diffraction 2010

12 September 2010Diffraction Expectation for uncertainties in parity- violating asymmetries in high-p T muon production Assuming: 50 pb -1 50% polarization S/B = 0.3

12 September 2010Diffraction Expectation for uncertainties in parity- violating asymmetries in high-p T muon production Assuming: 50 pb -1 50% polarization S/B = 3.0

12 September 2010Diffraction Expectation for uncertainties in parity- violating asymmetries in high-p T muon production Assuming: 150 pb -1 50% polarization S/B = 3.0

Summary PHENIX has observed a non-zero parity- violating asymmetry in W production in pp collisions at 500 GeV Future measurements with greater precision will allow a measurement of the light quark sea contribution to the spin of the proton, using a technique complementary to that used in leptonic SIDIS 12 September 2010Diffraction

12 September 2010Diffraction

12 September 2010Diffraction Cross Sections for W Production in PHENIX Final Results for RHIC 2009 Run [arXiv: ]