Single-Spin Asymmetry in pp  X at RHIC Werner Vogelsang BNL Nuclear Theory RSC meeting, RIKEN, 09/29/2006.

Slides:



Advertisements
Similar presentations
Transverse Single Spin Asymmetries in Large-x F Production at STAR A Review of Several Mysteries L.C. Bland Brookhaven National Laboratory 31 July 2007.
Advertisements

June 21, 2005 RHIC & AGS USER MEETING-SPIN 1 (Single) Transverse Spin Physics -- from DIS to hadron collider Feng Yuan, RBRC, Brookhaven National Laboratory.
Longitudinal Spin at RHIC 29 th Winter Workshop on Nuclear Dynamics February 7, 2013 Cameron McKinney.
Pawan Kumar NetrakantiPANIC-2005, Santa Fe1 Pion, proton and anti-proton transverse momentum spectra in p+p and d+Au collisions at  s NN = 200 GeV Outline:
Mauro Anselmino, Prague, August 1, 2005 Hadron Structure and Hadron Spectroscopy Transversity (transverse spin and transverse motion) Transversity distributions.
Constraining the polarized gluon PDF in polarized pp collisions at RHIC Frank Ellinghaus University of Colorado (for the PHENIX and STAR Collaborations)
Carl Gagliardi – WWND – Trans Spin at RHIC 1 Transverse Spin Physics in pp Collisions at RHIC Carl A. Gagliardi Texas A&M University Outline Introduction.
Overview of Orbital Angular Momentum via TMD Measurements in Hadronic Collisions L.C. Bland Brookhaven National Lab ECT*, Trento 28 August 2014 OUTLINE.
Cold nuclear matter effects on dilepton and photon production Zhong-Bo Kang Los Alamos National Laboratory Thermal Radiation Workshop RBRC, Brookhaven.
QCD Resummations for Hadronic Collisions Werner Vogelsang RBRC and BNL Nuclear Theory RHIC/AGS Users’ Meeting 2005.
9/19/20151 Semi-inclusive DIS: factorization Feng Yuan Lawrence Berkeley National Laboratory RBRC, Brookhaven National Laboratory.
Carl Gagliardi – QCD at High Energy/Small x 1 QCD at High Energy/Small x Experimental Overview Outline What do we know? Things to learn from the next RHIC.
Constraining the Sivers Functions using Transverse Spin Asymmetries at STAR XII International Workshop on Deep Inelastic Scattering, Strbske Pleso, High.
1 Transverse Spin Measurements at PHENIX John Koster for the PHENIX collaboration University of Illinois at Urbana-Champaign DIS /04/27.
Hiroyuki Kawamura (RIKEN) QCD Prediction of A TT for small Q T dimuon production in pp and ppbar collisions Hiroyuki Kawamura (RIKEN) Jiro Kodaira (KEK)
Hiroyuki Kawamura (RIKEN) QCD Prediction of A TT for Small Q T Dimuon Production in pp and ppbar Collisions Hiroyuki Kawamura (RIKEN) Jiro Kodaira (KEK)
J/ψ Production in pPb Collisions at the LHC Zhang, Hong-Fei Third Military Medical University.
Quark Helicity Distribution at large-x Collaborators: H. Avakian, S. Brodsky, A. Deur, arXiv: [hep-ph] Feng Yuan Lawrence Berkeley National Laboratory.
High-Energy QCD Spin Physics Xiangdong Ji Maryland Center for Fundamental Physics University of Maryland DIS 2008, April 7, 2008, London.
Columbia University Christine Aidala September 4, 2004 Solving the Proton Spin Crisis at ISSP, Erice.
6/1/20161 TMD Evolution Feng Yuan Lawrence Berkeley National Laboratory.
May 18-20, 2005 SIR05 JLab 1 P ? Dependence of SSA -- from nonpert. to pert. Feng Yuan, RBRC, Brookhaven National Laboratory References: Ji, Ma, Yuan,
Zhongbo Kang Los Alamos National Laboratory QCD structure of the nucleon and spin physics Lecture 5 & 6: TMD factorization and phenomenology HUGS 2015,
1 Cross Sections and Spin Asymmetries in Hadronic Collisions Jianwei Qiu Brookhaven National Laboratory KEK theory center workshop on high-energy hadron.
Oct 3 Spin2006 J.H. Lee (BNL) 1/29 SSA in BRAHMS J.H. Lee and F. Videbaek Physics Department Brookhaven National Laboratory for BRAHMS Collaboration Preliminary.
1 SSA in BRAHMS J.H. Lee (BNL) for BRAHMS Collaboration Preliminary Results on ,K,p Transverse Single Spin Asymmetries  at 200 GeV and 62 GeV  at high-x.
Measurements of Transverse Spin Effects with the Forward Pion Detector of STAR Larisa Nogach Institute of High Energy Physics, Protvino for the STAR collaboration.
Transverse Spin Physics: Recent Developments
PQCD mechanisms for single (transverse) spin asymmetry in Drell-Yan production PQCD mechanisms for single (transverse) spin asymmetry in Drell-Yan production.
12/13/20151 Transverse Spin Overview: Theory Perspective Feng Yuan Lawrence Berkeley National Laboratory RBRC, Brookhaven National Laboratory.
Single- and double-spin asymmetries in inelastic proton-proton collisions Daniel A. Pitonyak Department of Physics Temple University, Philadelphia, PA.
Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Aug 15, 2003 Lepton-Photon 2003.
Transverse spin phenomena in pp and polarized fragmentation Akio Ogawa, BNL 2006 Oct 3.
JPARC DY Workshop, April 7 Ralf Seidl (RBRC) R.Seidl: Transverse Spin 1RIKEN, April 7 In JPARC Drell Yan accessible with: UU(unpolarized beam, unpolarized.
Spin physics with STAR at RHIC
Twist-3 predictions for single spin asymmetry for light-hadron productions at RHIC Koichi Kanazawa (Niigata Univ) ・ KK and Y. Koike, PRD 83, (2011)
Collins effect in the collinear factorization approach Jian Zhou (ShanDong University, China & LBNL, US) Collaborators: Feng Yuan (LBNL, US) Based on the.
Transverse Spin Asymmetries at RHIC Access to transverse momentum dependent distributions L.C. Bland Brookhaven National Laboratory 11 June 2007.
2/10/20161 What can we learn with Drell-Yan in p(d)-nucleus collisions Feng Yuan Lawrence Berkeley National Laboratory RBRC, Brookhaven National Laboratory.
Single Transverse-Spin Asymmetries and Twist-3 Factorization J.P. Ma, ITP, Beijing Weihai,
October 22, 2004 Single Spin Asymmetries at RHIC 1 F.Videbaek Physics Department, Brookhaven National.
The transverse structure of the nucleon (resolving the quark motion inside a nucleon) Mauro Anselmino, Torino University and INFN, JLab, December 15, 2006.
Azimuthal correlations of forward di-hadrons in d+Au collisions at RHIC Cyrille Marquet Theory Division - CERN Based on :C.M., Nucl. Phys. A796 (2007)
Spin Physics at RHIC Ming Xiong Liu Los Alamos National Lab 8/3/091Ming Xiong Liu OCPA06.
Hiroyuki Kawamura (RIKEN) Transverse double-spin asymmetries for small Q T Drell-Yan pair production in pp and ppbar collisions Hiroyuki Kawamura (RIKEN)
Hiroyuki Kawamura (RIKEN) Soft-gluon resummation in Drell-Yan dilepton (and vector boson) production at small transverse momentum: spin asymmetries and.
1 Small x and Forward Physics in pp/pA at RHIC STAR Forward Physics FMS Steve Heppelmann Steve Heppelmann Penn State University STAR.
6/28/20161 Future Challenges of Spin Physics Feng Yuan Lawrence Berkeley National Laboratory.
RBRC & BNL Nuclear Theory
Single-Transverse Spin Asymmetries in Hadronic Scattering
Luciano Pappalardo for the collaboration
Physics with polarized antiprotons at GSI-PAX
Strangeness and Spin in Fundamental Physics
Semi-inclusive DIS at Small-x
JSA/HUGS Fellowship Seminar-2016
Can We Learn Quark Orbital Motion from SSAs?
Unique Description for SSAs in DIS and Hadronic Collisions
Masanori HIRAI 2006, Nov 9, Tokyo-u
RBRC and BNL Nuclear Theory
Daniel A. Pitonyak Department of Physics, Temple University
Quark and Gluon Sivers Functions
Searching for intrinsic motion effects in SIDIS
Yuji Koike (Niigata Univ.)
Unique Description for Single Transverse Spin Asymmetries
New d+Au RHIC data show evidence for parton saturation
Spin effects and partonic intrinsic k┴
Unifying the Mechanisms for SSAs in Hard Process
QT resummation in transversely polarized Drell-Yan process
Yuji Koike (Niigata Univ.)
Introduction to pQCD and TMD physics Lecture 2: perturbative QCD (II)
Presentation transcript:

Single-Spin Asymmetry in pp  X at RHIC Werner Vogelsang BNL Nuclear Theory RSC meeting, RIKEN, 09/29/2006

Outline: Phenomenological study of pp  h X Conclusions Some further predictions New theoretical calculation Introduction Work with C. Kouvaris, J.W. Qiu, F. Yuan hep-ph/

I. Introduction

L R  strikingly large asymmetries at forward angles important: A N in pp  h X is power-suppressed ~1/p  Kane, Pumplin, Repko ‘78 single-inclusive observable, collinear factorization

Brahms prel. STAR

 Resummation of important higher-order corrections beyond NLO de Florian, WV √s=23.3GeV Bourrely and Soffer Apanasevich et al.

II. New theoretical calculation

analysis of power-suppressed effects in QCD (Qiu,Sterman; Efremov,Teryaev) x1x1 x2x2 x 2 -x 1 Phase from imaginary part of propagator ~ i  (x 1 -x 2 ) quark-gluon correlation function T F (x 1, x 2 ) provides helicity flip unpol. pdf

full structure: Kanazawa,Koike Qiu,Sterman Transversity

Position of pole may depend on k  of initial partons

“derivative terms” on-shell condition for “unobserved” parton

Qiu & Sterman argue: “derivative terms” dominate At forward x F, collisions are asymmetric: large-x parton hits “small-x” parton  T F (x, x) mostly probed at relatively large x

 Assumptions in Qiu & Sterman : derivative terms only valence T F only, neglect gluon  pion fragmentation In view of new data, relax these. Kouvaris, Qiu, Yuan, WV

 Remarkably simple answer:

III. Phenomenological study (…still more illustrative)

 Ansatz: usual pdf  Fit to E704, STAR, BRAHMS  for RHIC, use data with p T >1 GeV  for E704, choose p T =1.2 GeV allow normalization of theory to float (~0.5)

Fit I: “two-flavor / valence” Fit II: allow sea as well

solid: Fit I, dashed: Fit II

Our T F functions:

IV. Some further predictions

p T dependence

Dependence on pion energy for fixed  :

Dependence on RHIC c.m.s. energy:

A N in jet production:

A N in prompt-photon production:

V. Conclusions

SSA for single-inclusive process: power-suppressed new calculations in Qiu/Sterman formalism: “Non-derivative” terms. Organize in simple form. Moderately important. Data from RHIC are beginning to constrain T F functions. Consistency of theory description of fixed-target and RHIC data is only qualitative Entering era of precision determinations of T F !