6/2/2005Douglas Fields1 Measuring Orbital Angular Momentum through Jet k T Douglas Fields University of New Mexico/RBRC Jan Rak, Rob Hobbs, Imran Younus.

Slides:



Advertisements
Similar presentations
Silicon Verterx Tracker Upgrade of PHENIX Experiment at RHIC Y. Akiba (RIKEN) CIPANP2003 New York, New York May 2003.
Advertisements

CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Jin Huang PhD Candidate, MIT For MENU 2010 May 31, Williamsburg.
DIS 2008, London Transverse Spin Physics at PHENIX Douglas Fields (University of New Mexico) For the PHENIX Collaboration 4/9/20081 Douglas Fields for.
» Drell RHIC « Oleg Eyser ECT* Workshop on Drell Yan Physics and the Structure of Hadrons May 21-25, 2012, Trento, Italy.
Xiaorong Wang, Heavy Flavor Workshop at UIC, June, Heavy Flavor and Spin Program at Xiaorong Wang New Mexico State University Heavy Flavor workshop.
PHENIX Decadal Plan o Midterm upgrades until 2015 o Long term evolution after 2015 Dynamical origins of spin- dependent interactions New probes of longitudinal.
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.
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.
Ali Hanks - APS Two Particle Correlations in PHENIX Ali Hanks July 7 th, 2008 Journal Club.
Double Helicity Dependence of Jet Properties Douglas Fields University of New Mexico.
J. Seele - WWND 1 The STAR Longitudinal Spin Program Joe Seele (MIT) for the Collaboration WWND 2009.
Source Dynamics from Deuteron and Anti-deuteron Measurements in 200 GeV Au+Au Collisions Hugo E Valle Vanderbilt University (For the PHENIX Collaboration)
Non-photonic electron production in STAR A. G. Knospe Yale University 9 April 2008.
Douglas Fields University of New Mexico. Direct vs. Indirect Measurement Width of room Tape measure Spin ½ of proton Stern-Gerlach experiment ΔΣ DIS ΔG.
Nov 2001 Craig Ogilvie 1 Angular Correlations at High pt: Craig Ogilvie for the Phenix Collaboration Energy-loss: increased medium-induced gluon-radiation.
PHENIX Fig1. Phase diagram Subtracted background Subtracted background Red point : foreground Blue point : background Low-mass vector mesons (ω,ρ,φ) ~
Polarimetry of Proton Beams at RHIC A.Bazilevsky Summer Students Lectures June 17, 2010.
Status of W analysis in PHENIX Central Arm Kensuke Okada (RBRC) For the PHENIX collaboration RHIC Spin Collaboration meeting November 21, /21/20091K.Okada.
Hard vs. Soft Physics at RHIC - Insights from PHENIX l Why hard vs. soft? l Soft physics: thermal, flow effects l Hard processes at RHIC l Conclusion Barbara.
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.
BNL/ Tatsuya CHUJO CNS workshop, Tokyo Univ. Identified Charged Single Particle Spectra at RHIC-PHENIX Tatsuya Chujo (BNL) for the PHENIX.
Motivation. Why study ground state hyperon electroproduction? CLAS detector and analysis. Analysis results. Current status and future work. M. Gabrielyan.
 Production at forward Rapidity in d+Au Collisions at 200 GeV The STAR Forward TPCs Lambda Reconstruction Lambda Spectra & Yields Centrality Dependence.
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.
Transverse Spin Physics with PHENIX 1 Transverse Spin Physics with the current PHENIX K. Oleg Eyser UC Riverside RHIC Spin: The next decade May 14-16,
Radiative penguins at hadron machines Kevin Stenson University of Colorado.
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.
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.
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)
Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Aug 15, 2003 Lepton-Photon 2003.
Measurement of photons via conversion pairs with PHENIX at RHIC - Torsten Dahms - Stony Brook University HotQuarks 2006 – May 18, 2006.
Transverse Single-Spin Asymmetries Understanding the Proton: One of the fundamental building blocks of ordinary matter! Spin decomposition of proton still.
N. N. Ajitanand Nuclear Chemistry, SUNY Stony Brook For the PHENIX Collaboration RHIC & AGS Users Meeting June Investigation of Parity Violation.
 Measurement of  x E  (Fig. 4) Assorted correlations between a fixed high-p T trigger hadron (  p Ttrig  =4.7GeV/c) and lower p T associated hadrons.
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.
Feasibility study of Heavy Flavor tagging with charged kaons in Au-Au Collisions at √s=200 GeV triggered by High Transverse Momentum Electrons. E.Kistenev,
TMD flavor decomposition at CLAS12 Patrizia Rossi - Laboratori Nazionali di Frascati, INFN  Introduction  Spin-orbit correlations in kaon production.
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.
Oct. 12, 2007 Imran Younus k T Asymmetry in Longitudinally Polarized p +p Collisions at PHENIX.
BNL/ Tatsuya CHUJO JPS RHIC symposium, Chuo Univ., Tokyo Hadron Production at RHIC-PHENIX Tatsuya Chujo (BNL) for the PHENIX Collaboration.
Inclusive cross section and single transverse-spin asymmetry of very forward neutron production at PHENIX Spin2012 in Dubna September 17 th, 2012 Yuji.
Study of Charged Hadrons in Au-Au Collisions at with the PHENIX Time Expansion Chamber Dmitri Kotchetkov for the PHENIX Collaboration Department of Physics,
Overview of the sea quark polarization measurements of PHENIX at RHIC DIS April 12, Rusty Towell Abilene Christian University on behalf of the PHENIX.
08-Sep-00PHENIX Upgrades PHENIX has a phased strategy to q Complete the current detector q Enhance its capabilities q Extend its physics reach.
Ran HAN Peking University For PHENIX The Polarization of Anti-Lambda Produced In sqrt(s)=200GeV Polarized Proton-Proton Collision.
Direct Photon v 2 Study in 200 GeV AuAu Collisions at RHIC Guoji Lin (Yale) For STAR Collaboration RHIC & AGS Users’ Meeting, BNL, June 5-9.
Timelike Compton Scattering at JLab
Richard Petti For the PHENIX Collaboration
Luciano Pappalardo for the collaboration
Tatia Engelmore, Columbia University
Prague 2007 Collins and Sivers asymmetries
Takafumi Niida from Univ. of Tsukuba for the PHENIX Collaborations
Measuring Orbital Angular Momentum through Jet kT
kT Asymmetry in Longitudinally Polarized Collisions
Takafumi Niida from Univ. of Tsukuba for the PHENIX Collaborations
Spin Physics at RHIC Kieran Boyle (RBRC).
Quark and Gluon Sivers Functions
Single Spin Asymmetry with a Transversely Polarized
kT Asymmetry in Longitudinally Polarized pp Collisions
J. Rak (for R. Hobbs) For the PHENIX collaboration
High-pT Identified Charged Hadrons in √sNN = 200 GeV Au+Au Collisions
Identified Charged Hadron
Identified Charged Hadron Production at High pT
APS/JPS Second Joint Meeting Sep. 19, 2005
Masahiro Konno (Univ. of Tsukuba) for the PHENIX Collaboration Contact
Presentation transcript:

6/2/2005Douglas Fields1 Measuring Orbital Angular Momentum through Jet k T Douglas Fields University of New Mexico/RBRC Jan Rak, Rob Hobbs, Imran Younus

6/2/2005Douglas Fields2 Idea came from me trying to understand Sivers effect –Quantum Fan Level Description –This is a double spin asymmetry –This is for longitudinally polarized protons Rotating partons around spin direction Two classes of collisions: –Like helicity, i.e., –Un-like helicity, i.e., Basic Picture Positive Helicity Negative Helicity

6/2/2005Douglas Fields3 Like Helicity (Positive on Positive Helicity) Central Collisions Smaller Peripheral Collisions Larger Integrate over b, left with some residual k T Measure jet Peripheral Collisions Larger

6/2/2005Douglas Fields4 Un-like Helicity (Positive On Negative Helicity) Peripheral Collisions Smaller Central Collisions Larger Integrate over b, left with some different residual k T

6/2/2005Douglas Fields5 History Talked to many people – Werner pointed me to a paper by Meng Ta-chung et al. Experiment B – similar idea, only for Drell-Yan

6/2/2005Douglas Fields6 From Meng Ta-Chung et al. Phys Rev. D40, p769, (1989) For a particular impact parameter, b, the average transverse momentum Where, is the product of the Jacobian and the density profile of partons, and D(b) is the overlap region. Total transverse momentum squared of partons k TR k PR

6/2/2005Douglas Fields7 From Meng Ta-Chung et al. Phys Rev. D40, p769, (1989) The constant terms in p t cancel and we have We can now helicity separate: b We can then average over the impact parameter k TR k PR k TR k PR Like Helicity Un-like Helicity

6/2/2005Douglas Fields8 From Meng Ta-Chung et al. Phys Rev. D40, p769, (1989) This paper makes the following assumptions: 1)Uniform spherical density F(b,θ P,θ T ) 2)k PR ~k TR ~k R (no dependence on b, θ P, θ T.) Then, Evaluated numerically

6/2/2005Douglas Fields9 How Large an Effect Can We Expect?

6/2/2005Douglas Fields10 Pause For Feedback Need theoretical guidance! Would be nice to have experimental handle on impact parameter: –Multiplicity Forward or central Underlying event… but, not explicitly necessary.

6/2/2005Douglas Fields11 How do we measure k t ? Intra-jet pairs angular width : N j T Inter-jet pairs angular width : A j T k T 0 - h azimuthal correlation functions Trigger 0

6/2/2005Douglas Fields12 PHENIX Detector Overview East Arm tracking: –DC, PC1, TEC, PC3 electron & hadron ID: –RICH,TEC/ TRD, –TOF, EMCal photons: –EMCal West Arm tracking: –DC,PC1, PC2, PC3 electron ID: –RICH, –EMCal photons: –EMCal

6/2/2005Douglas Fields13 π 0 Identification PHENIX has central arm EMCal with electron rejection in RICH. Used shower profile cut. Good S/B at higher p t (>2GeV).

6/2/2005Douglas Fields14 Charged Particles Tracks in the Drift Chamber Hits in the Pad Chambers RICH veto for low momentum Shower shape cut at high momentum

6/2/2005Douglas Fields15 Correlation Functions dN real Δφ distribution from particles in the same event dN mixed Δφ distribution from particles in different events with similar vertex position Norm = Fit to two gaussians plus a constant term 3.0<p T <4.0 Fit = const + Gauss(0)+Gauss( ) 1.5<p T <2.0 Intra-jet pairs angular width : N j T Inter-jet pairs angular width : A j T k T

6/2/2005Douglas Fields16 Jet Kinematics

6/2/2005Douglas Fields17 How accurately can we measure ? is extracted from and fragmentation functions which are extracted from the inclusive distributions.

6/2/2005Douglas Fields18 How accurately can we measure Δ ? Z T uncertainties should cancel in the difference Bunch Shuffling in Run3 (PHENIX) –δ Δ ~ 80MeV

6/2/2005Douglas Fields19 For Run5 ~10-20 times more statistics than Run3 –Statistical errors smaller by factor of 3-5 Polarization in Run5 ~55% –Effect larger by factor of ~5 (P Y *P B ) than Run3

6/2/2005Douglas Fields20 Summary We can make a measurement of the double-longitudinal spin dependence of jet. This may be sensitive to orbital angular momentum. These effects (if really there) may also influence the double-longitudinal cross- section asymmetry. Need theoretical guidance…