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1 11 April 6 2011 A.Magnon IWHSS’11 4-6 April 2011 PARIS

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Page 1: 1 IWHSS_11 April 6 2011 A.Magnon IWHSS’11 4-6 April 2011 PARIS

1IWHSS_11 April 6 2011 A.Magnon

IWHSS’11 4-6 April 2011 PARIS

Page 2: 1 IWHSS_11 April 6 2011 A.Magnon IWHSS’11 4-6 April 2011 PARIS

2IWHSS_11 April 6 2011 A.Magnon

Monday Morning

A.Bachetta A.Martin

M.Burkardt Z.E.Meziani

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3IWHSS_11 April 6 2011 A.Bachetta

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4IWHSS_11 April 6 2011 A.Bachetta

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5IWHSS_11 April 6 2011 A.Magnon

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6IWHSS_11 April 6 2011 A.MagnonIWHSS_11 April 6 2011 A.Bachetta 6

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7IWHSS_11 April 6 2011 A.MagnonIWHSS_11 April 6 2011 A.Bachetta 7

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8IWHSS_11 April 6 2011 A.MagnonIWHSS_11 April 6 2011 A.Bachetta 8

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Transverse Spin and Momentum Structure of the Nucleon

SIDIS off transversely polarised targets: DESY (HERMES)

CERN (COMPASS) JLab Z.-E. Meziani

and eRHIC, EIC, ENC

hard polarised pp scatteringRHIC / BNL M. Grosse-Perdekamp

and several (future) projects for (polarised) Drell-Yan:

CERN (COMPASS) FNAL, JParc, RHIC, JINR, IHEP, GSI J.-C. Peng, A. Ogawa, A. Ferrero

p

ph

X

a large international theoretical and experimental effort

h

N

'

X

IWHSS_11 April 6 2011 A.Martin 9

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KINEMATICAL REGION

27.5 GeV160 GeV

JLab 6 GeV

IWHSS_11 April 6 2011 A.Martin 10

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IWHSS’11

same sign and strength: a very important, not obvious result!

π-

π+

h-

h+

Collins asymmetry - proton

indication for: not a higher twist effect,weak Q2 dependence of the Collins FF

COMPASS sign conventionIWHSS_11 April 6 2011 A.Martin 11

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IWHSS’11

Sivers asymmetry - proton

π-h-

• same sign

• COMPASS results in the overlap region smaller by a factor ~ 2

π+

h+

good agreements

IWHSS_11 April 6 2011 A.Martin 12

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E06‑010 JLAB Experiment to access the neutron

• Polarized 3He Target• Polarized Electron Beam

– ~80% Polarization– Fast Flipping at 30Hz– PPM level charge Asymmetry

controlled by online feed back• BigBite at 30º as Electron Arm

– Pe = 0.7 ~ 2.2 GeV/c • HRSL at 16º as Hadron Arm

– Ph = 2.35 GeV/c

Beam Polarimetry(Møller + Compton)

LuminosityMonitor

Students: Xin Qian (Duke), Chiranjib Dutta (Kentucky), and Kalyan Allada (Kentucky)

Spokespeople: X. Jiang (Los Alamos), J.-P. Chen (JLab), H. Gao (Duke), J.C. Peng (UIUC),

IWHSS_11 April 6 2011 Z.E.Meziani 13

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Preliminary Neutron Collin/Sivers Asymmetries

Systematic uncertainty is still under study Curves: Diquark-quark Model (Ma), Global Fit

(Anselmino), Light-Cone quark model (Pasquini)

Collins

Sivers

IWHSS_11 April 6 2011 Z.E.Meziani 14

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Courtesy of H. Avakian

E12-06-112: Pion SIDIS E12-09-008: Kaon SIDIS

E12-07-107: Pion SIDIS E12-09-009: Kaon SIDIS

LOI12-06-108: Pion SIDISLOI12-09-004: Kaon SIDIS

PAC approved experiments & LoIN

q

U

L

T

Complete program of TMDs studies for pions and kaons

Kaon measurements crucial for a better understanding of the TMDs “kaon puzzle”

Kaon SIDIS program requires an upgrade of the CLAS12

detector PID RICH detector to replace LTCCProject under development

TMDs program @ 12 GeV in Hall B

IWHSS_11 April 6 2011 Z.E.Meziani 15

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16IWHSS_11 April 6 2011 M.Burkardt 16

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17IWHSS_11 April 6 2011 M.Burkardt 17

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18IWHSS_11 April 6 2011 M.Burkardt 18

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19IWHSS_11 April 6 2011 A.Magnon

Monday Afternoon

D. De Florian Ph. Haegler

M. Grosse Perdekamp C. Franco

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20IWHSS_11 April 6 2011 A.Magnon 20

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IWHSS_11 April 6 2011 D. De Florian 21

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IWHSS_11 April 6 2011 D. De Florian 22

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IWHSS_11 April 6 2011 D. De Florian 23

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Nucleon parton distributions from lattice QCD

Philipp Hägler

supported by

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Not quite as trivial as it might appear...

Typical „measurements“ on the lattice

IWHSS_11 April 6 2011 Ph. Haegler 25

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Ju, Jd template figure (update)

LHPC arXiv:1001.3620

LHPC PRD `08 0705.4295

QCDSF (Ohtani et al.) 0710.1534

Goloskokov&Kroll EPJC`09 0809.4126

Wakamatsu 0908.0972

DiFeJaKr EPJC `05 hep-ph/0408173

(Myhrer&)Thomas PRL`08 0803.2775

[JLab Hall A PRL`07; HERMES JHEP`08]

[non-singlet, connected only; add. uncertainties due to chiral extrapolations, renormalization]*

**

*QCDSF/UKQCD preliminary*,1

1Sternbeck, Pleiter, Zanotti et al. 2011

lattice results fromcovariant BChPT extrapolations[Dorati, Gail, Hemmert NPA 2008]

lattice results fromcovariant BChPT extrapolations[Dorati, Gail, Hemmert NPA 2008]

IWHSS_11 April 6 2011 Ph. Haegler 26

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Ph. Hägler, IWHSS, Paris 04/11

27

Sivers transverse momentum shift

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28IWHSS_11 April 6 2011 M. Grosse-Perdekamp

Spin Physics Results from RHIC

Preliminaries: Facility Status QCD & PDFs vs Data

Gluon spin distribution Inclusive hadron and jet results QCD analysis Low x & x-dependence with di-jets and rapidity separated di-hadrons

W-production in polarized p-p First results from pp W eν

Transverse Spin Inclusive AN

Channels isolating Collins or Sivers effects

Drell Yan measurements in Akio Owaga’s talk

M. Grosse-Perdekamp UIUC

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ΔG(x) from DSSV Global QCD Analysis

RHIC

Range

0.05<x<0.2

Large-x

x≥0.2

Small-x

x≤0.05

ΔGtrunc[0.05,0.2] ≈ 0 since node at x≈0.1

Data constrains only truncated first moment of ΔG(x) in x-interval [0.05,0.2], but not functional form at low or high x

ΔGtrunc in large-x region constrained to be small by requirement that ΔG(x) ≤ G(x); at Q2=10 GeV2: ΔGtrunc[0.3,1.0] ≤ 0.03

At small x, ΔG(x) can differ from DSSV beyond errors without violating funda-mental constraints

ΔGtrunc[0.05,0.2] = ∫ ΔG(x) dx = 0.0050.2

0.05

+0.051

-0.058-0.058-0.058-0.058

x ΔG(x)

de Florian, Sassot, Stratmann,Vogelsang PRD 80:034030,2009 

IWHSS_11 April 6 2011 M. Grosse-Perdekamp 29

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pT,1>3 GeV, pT,2 > 1.5 GeV error bars are statistical only

Projected ALL(π0) in MPC for different ΔG(x) at low x

for ∫Ldt = 300 pb-1, √s = 500 GeV (RHIC W program, 2011 to 2015)

Increasing Δgtrunc [10-4,0.05]

ΔGtrunc= -.1 ΔGtrunc= -.2 ΔGtrunc= -.5

ΔGtrunc [10-4,0.05] = -0.1 will be observableIWHSS_11 April 6 2011 M. Grosse-Perdekamp 30

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Summary

o Gluon Spin contribution constraint for 0.05 < x < 0.2 use di-jet and di-hadron measurements to probe x-dependence ΔG(x) and forward jet production to reach low x, x~0.001.

o W-program has started with electrons (STAR & PHENIX) and muons (PHENIX). Luminosity accumulation will take 3-4 runs.

o Precision data on AN are available. Exciting new Drell Yan experiment at IP2: AnDY (see Akio Ogawa’s talk). Initial measurements to isolate Collins -and Sivers- asymmetries. Much improvement from detector upgrades and increased statistics.

31IWHSS_11 April 6 2011 M. Grosse-Perdekamp

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32

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33IWHSS_11 April 6 2011 C. Franco

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34IWHSS_11 April 6 2011 C. Franco

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35IWHSS_11 April 6 2011 C. Franco

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36IWHSS_11 April 6 2011 A.Magnon

Tuesday Morning

J. Friedrich D. Drechsel D. Bugg G. Bali A. Szczepaniak

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37IWHSS_11 April 6 2011 J. Friedrich

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38IWHSS_11 April 6 2011 J. Friedrich

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39IWHSS_11 April 6 2011 J. Friedrich

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40IWHSS_11 April 6 2011 J. Friedrich

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41IWHSS_11 April 6 2011 D. Drechsel

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42IWHSS_11 April 6 2011 D. Drechsel

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43IWHSS_11 April 6 2011 D. Drechsel

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David Bugg, Queen Mary, London

Topics in meson spectroscopy for Compass

(i) Look for the I=0 JPC=1-+ partner of p1(1600/1662)

(ii) Measure (4 )/ (2 ) s p s p from 1200-2000 MeV for JP=0+,1-,2+.

Sort out f0(1370), f2(1565) and r(1450). Check if f2(1810) exists or is really f0(1790).(iii) Check if p1(1405) is resonant or just a threshold

cusp.

IWHSS_11 April 6 2011 D. Bugg

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The p1(1600/1660) looks a good hybrid candidate.It ought to have an I=0 partner of similar mass.The only likely decay mode is to a1(1260) :p JPC = 1++ + 0-+ = 1-+.

This is NOT easy because no angular dependence: there are only the r and a1 signals to go on, and the a1 is broad. However, other JPC will have angular dependence.

There exist possible partners with JPC = 2-+:h2(1860) and p2(1880); also (1800), p 0-+

Topics in meson spectroscopy for Compass

IWHSS_11 April 6 2011 D. Bugg

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CONCLUSION: There is still lots to do and learn in meson spectroscopy. I doubt that heavy meson spectroscopy can go beyond narrow states, but it is important to complete light meson spectroscopy and baryon spectroscopy and learn what we can about hybrids and glueballs. Good luck !

The spectroscopy of I=1, C = +1 states and C=-1 states with I=0 and 1 could be completed by measuring polarisation in pp -> 3p0, , ; hhp hp wp and whp0; wh and wp0p0 at the forthcoming Fair facility. It just needs an extracted p beam of 5 x 104 p/s.

Topics in meson spectroscopy for Compass

IWHSS_11 April 6 2011 D. Bugg

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47IWHSS_11 April 6 2011 G. Bali

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48IWHSS_11 April 6 2011 G. Bali

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49IWHSS_11 April 6 2011 A. Szczepaniak

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50IWHSS_11 April 6 2011 A. Szczepaniak

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51IWHSS_11 April 6 2011 A.Magnon

Tuesday Afternoon

J.C. Peng A. Ogawa

V. Barone

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52IWHSS_11 April 6 2011 J.C. Peng

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53

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54IWHSS_11 April 6 2011 J.C. Peng

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Future Drell-Yan Experiments

Akio Ogawa2011 Apr 5

IWHSS Paris 2011

55

at

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The Relativistic Heavy Ion Collider

PHENIXSTAR

IP2(AnDY, IT)

Au+Au

Polarized p+p

d+Au

RHIC is a QCD lab

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57

E.C.Aschenauer, A. Bazilevsky, L.C. Bland, K. Drees, C. Folz, Y. Makdisi, A. Ogawa, P. Pile, T.G. Throwe

Brookhaven National LaboratoryH.J. Crawford, J.M. Engelage, E.G. Judd

University of. California, Berkeley/Space Sciences Laboratory

C.W. PerkinsUniversity of. California, Berkeley/Space Sciences

Laboratory /Stony Brook UniversityA. Derevshchikov, N. Minaev, D. Morozov, L.V. Nogach

Institute for High Energy Physics, ProtvinoG. Igo, S. Trentalange

University of California, Los AngelesM. Grosse PerdekampUniversity of Illinois

M.X. LiuLos Alamos National Laboratory

H. AvakianThomas Jefferson National Accelerator Facility

E.J.BrashChristopher Newport University and TJNAF

C.F.PerdrisatCollege of William and Mary

V. PunjabiNorfolk State University

Li, XuanShandong University, China

Mirko Planinic, Goran Simatovic University of Zagreb, Croatia

ANDY at IP2“Feasibility Test of Large Rapidity Drell

Yan Production at RHIC”

Letter of Intent submitted 24 May 2010

http://www.bnl.gov/npp/docs/pac0610/Crawford_LoI.100524.v1.pdf

PAC presentation: http://www.bnl.gov/npp/docs/pac0610/aschenauer_DY-collider_june10.pdf

• Timeliness – Run when STAR & PHENIX is doing W program (2012-13)

• Acceptance/background rejection – Severe space constraints at STAR and PHENIX require major changes in the forward direction to do DY

• Is charge sign a requirement? – feed back to STAR/PHENIX forward upgrade plans

IWHSS_11 April 6 2011 A. Ogawa

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AN for jets

58

arXiv:1103.1591 jet AN measurements are required to clarify signs of quark/gluon correlators related to Sivers functions.

from p+pp

“old” Sivers function

“new” Sivers function

s=200 GeV

STAR FMS ECal only “jet-like” event Positive AN for jet-like events Lack of cos(γ) dependence AN for jets will be non-0 ?

ANDY is taking HCal jet trigger right now(~500M jet trigger events as of last week)We have ~1/pb as of last weekNeed >5x more (possible in 1 week if 3IP collisions from start of fill)

Determine whether AN(jet) is non-0 isa requirement for AN(DY) sign-flip measurement

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Letter of Intent: Measurement of Dimuons from Drell-Yan Process with Polarized Proton Beams and an Internal Target at RHIC

– http://www.bnl.gov/npp/docs/pac0610/Goto_rhic-drell-yan.pdf– Academia Sinica (Taiwan): W.C. Chang– ANL (USA): D.F. Geesaman, P.E. Reimer, J. Rubin– UC Riverside (USA): K.N. Barish– UIUC (USA): M. Groose Perdekamp, J.-C. Peng– KEK (Japan): N. Saito, S. Sawada– LANL (USA): M.L. Brooks, X. Jiang, G.L. Kunde, M.J. Leitch, M.X.

Liu, P.L. McGaughey– RIKEN/RBRC (Japan/USA): Y. Fukao, Y. Goto, I. Nakagawa, K.

Okada, R. Seidl, A. Taketani– Seoul National Univ. (Korea): K. Tanida– Stony Brook Univ. (USA): A. Deshpande– Tokyo Tech. (Japan): K. Nakano, T.-A. Shibata– Yamagata Univ. (Japan): N. Doshita, T. Iwata, K. Kondo, Y. Miyachi

IWHSS_11 April 6 2011 A. Ogawa

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60IWHSS_11 April 6 2011 V. Barone

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61IWHSS_11 April 6 2011 V. Barone

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62

Fracture Functions

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63IWHSS_11 April 6 2011 A.Magnon

Wednesday Morning

A. Ferrero E. Leader B. Pire

A.M

Just Now … !

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64

Get Up ….

… for Compass-II

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65IWHSS_11 April 6 2011 J.C. Peng