Summay of Session 2 QCD spin structure of nucleons

36
Summay of Session 2 QCD spin structure of nucleons

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Summay of Session 2 QCD spin structure of nucleons. Summary Session 2. Introduction Helicity distributions Gluon polarisation transversity. Summary of Session 2. six excellent plenary talks: Metz, Barone, Garçon, Hasch, Bressan, Saito 55 talks in parallel sessions, 16 h - PowerPoint PPT Presentation

Transcript of Summay of Session 2 QCD spin structure of nucleons

Page 1: Summay of Session 2 QCD spin structure of nucleons

Summay of Session 2

QCD spin structure of nucleons

Page 2: Summay of Session 2 QCD spin structure of nucleons

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G. Mallot/CERN

Summary Session 2

IntroductionHelicity distributionsGluon polarisation

transversity

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• six excellent plenary talks:

Metz, Barone, Garçon, Hasch, Bressan, Saito

• 55 talks in parallel sessions, 16 h– half experiment / half theory

• exp. talks: about 2/3 ℓp, 1/3 pp• theo. talks: about 1/3 on transversity and SSA

Apologies for not being able to cover everything appropriately

Summary of Session 2

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HELICITY DISTRIBUTIONS

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Final g1 for p, d, n

• quasi final data set for p and d

• corrected for smearing (radcor, detector)

Riedl

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Quark helicity distributions

Rubin

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Inclusive asymmetries

• COMPASS deuteron data 2002 – 2003

• most precise data for x<3x10-2

• 2004 similar precision

• kaon/pion asymmetries to come

Peshekhonovinclusive

+ve hadrons

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• method using A and moments to determine

• model-independent determination of from incl. and semi-incl. asym. in LO and NLO. Fragmentations functions cancel in

needs very precise data (Jlab)

Δq - Theory

Christova

Shevchenko

remark: A exp. diffcult with magnetic spectrometers

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Δq - JLAB

• under construction (2006-2007)• expect very precise data for

x > 0.1

• apply method

JiangSemi-SANE E04-113

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Evolution

Stamenov

Ermolaev

Goshtasbpour

Ramsey

•parametrisation-independent matrix solution of DGLAP

•estimates of ΔG/G and Lq ranges

• role of higher twist in the determination of PDF. HT cancels largely in A1

.

• small-x evolution: double logarithm resummation important for g1 for x ≤ 10-3 -10-4

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GLUON POLARISATION

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ΔG/G - Photon-Gluon Fusion

measured

aLL: calculable partonic asymmetriesR: Monte-Carlo (Lepto for Q2 > 1 GeV2)

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ΔG/G - SMC

• event selection high-pT pairs– Q2 > 1 GeV2

– neural network

– ΣpT2 > 2.5 GeV2

• RPGF = 0.32

Rondio

SMC Hermes (all Q2)

NN pT12+pT2

2

xg

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ΔG/G - COMPASS

• Analysis a la SMC– ΣpT

2 > 2.5 GeV2, Q2 > 1 GeV2

• open charm signal10% ofstatistics

Schill

Hermes

SMC

Compass2002/3

PGF: cc open charm

2002/3

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ΔG/G – RHIC pp

π0

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ΔG/G - Phenix: ALL for π0

Fukao

Outlook 2005/72003/4

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ΔG/G – Star: ALL jets (2005)

STARSTAR Sowinski

0 5 10 15 20 25 30

0.2

0.4

0.6

0.8

1.0

0.0

gg qq

qg

Inclusive Jets :LOW. Vogelsang

pT (GeV)

2005

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• Resummation of NLL important for single-inclusive processes ( , )

• Crucial for lower energy fixed target

• Excellent agreement of NLO + NNL calculations with collider data!

• prompt photons good probe for ΔG/G at RHIC

NLO and NLLVogelsang

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Prompt photons/π0

Vogelsang, Okada

prompt γπ0

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RHIC detector upgrades

Tungsten-Silicon sampling calorimeter

prompt photon central arms

GS95

x

NCC

Kinney TogawaSilicon vertex barrel detector

• important enlargement of xg coverage first moment

2007-20082009

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• Spintransfer in Hyperon production in pp

Xu, Rykov

• Polarised DY p↑ p↑at GSI (transversity)

Efremov

Proposals

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TRANSVERSE SPIN

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AN for pp -> π0X

STARSTAR OgawaMakdisi

xF = 0

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SSA and intrinsic kT

• A generalized pQCD approach to SSA and unpol. cross sections: LO.pQCD + spin and new kT-dependent PDF and FF

• AN (p↑pπX): – Sivers effect contributes, Collins effect suppressed

– suppressed for xF<0 for all mechanisms

– good agreement with STAR data AN (p↑pπ0X)

Murgia, D’Alesio

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Intrinsic kT (continued)

In the same model it was shown that

• AN(p↑pDX) is an ideal process to study the Sivers distribution functions of quarks and gluons

• The Hermes data can be described as well as the unpolarised Cahn asymmetries from EMC using

Boglione

Prokudin

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p↑ p↑ cross section in NLO

• first NLO calculation• example: prompt photon

at Phenix• scale dependence

significantly reduced

• study of K-factors for DY

Mukherjee

Ratcliffe

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Hermes Collins & Sivers

Schnell

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COMPASS Collins & Sivers

Pagano

Collins Sivers

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Dihadron fragmentation

• New quark polarimeter

h1

h2

quark

TR

Bacchetta

• simpler, no kT

convolution, cf

van der Nat

Joosten

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More Asymmetries

• Boer-Mulders function

• AUL

• Model for transversity and intrinsic motion of quarks

• Chiral-odd twist-3 DF e(x)

• New observables from color gauge invariance

Gamberg

Kinney

Zavada

Wakamatsu

Pijlman

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Spin transfer to Λ

Alexakhin • Spin transfer to Λ

• transverse Λ polarisation

Friedrich Belostotski

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• SDME:

• Model

Exclusive ρ production

Neyret

Goloskokov

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• DVCS Beam Charge Asymmetry new: deuteron

• Hard exclusive ππ• Exclusive π and vector mesons• Hermes recoil detector

GPDs

Marukyan

Fabbri

Rostomyan

Stewart

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More from theory

• Spin sum rule revisited– problem in derivation of

– rigorous treatment yields miraculously same SR– new sum rule for transverse spin

• Higher twist resummation

• Asymmetries in SIDIS

Leader

Teryaev

Di Salvo

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• Determination of polarised fragmentation from Belle data in progress

• Possible difficulties with LUND fragmentation at low energies

• Q2 dependence of GDH

Fragmentation functions

Seidl

Kotzinian

Nagaitsev

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Personal Impression

• Two new facilities are working perfectly:

RHIC and COMPASS• Enormous progress on theory of

transverse spin and SSA

• Is ΔG/G small?

Exciting times ahead