Motivations 3 D nucleon structure TMDs Transverse momentum

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 Motivations 3 D nucleon structure TMDs (Transverse momentum dependent distributions) Transverse single-spin asymmetries

Motivations 3 D nucleon structure TMDs (Transverse momentum dependent distributions) Transverse single-spin asymmetries in various processes GPDs (Generalized parton distributions) Open issues 1 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Spin effects in QCD and 3 D nucleon structure

Disclaimer/apologies - Models of TMDs and GPDs - Lattice calculations - Parton orbital angular

Disclaimer/apologies - Models of TMDs and GPDs - Lattice calculations - Parton orbital angular momentum - GPD phenomenology - TMDs/GPDs in nuclei - Double Parton Distribution Functions Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Not covered in this talk: 2

Motivations (general statements) QCD and confinement: still to be understood Spin: fundamental quantum degree

Motivations (general statements) QCD and confinement: still to be understood Spin: fundamental quantum degree of freedom A tool to study the inner structure of composite systems Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Nucleon: still a mysterious object despite 50 years of studies 3

4 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University

4 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Almost energy independent

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University &

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Collinear PDFs DIS Structure Function 5 1 -D picture of the nucleon inclusive DIS

Physics issues er va bl es 3 D s O Non perturbative effects in

Physics issues er va bl es 3 D s O Non perturbative effects in high-energy processes Origin of transverse/azimuthal spin asymmetries e ur t c rt u Role of local color gauge invariance of QCD Factorization, universality, resummation Q CD at r o w k Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Orbital motion of quarks/gluons Its correlation to proton spin Intrinsic transverse momentum of quarks/gluons Spatial distribution of quarks/gluons 6 bs (open)

7 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University

7 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University &

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 TMD factorization proven 8 TMDs: How can we access them?

9 And possibly in processes like Spin effects in QCD and 3 D nucleon

9 And possibly in processes like Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 And more

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University &

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Drell-Yan EIC SIDIS 10 Where can we access TMDs?

Theory: factorization and evolution 11 Collinear approach Evolution → DGLAP eqs. Spin effects in

Theory: factorization and evolution 11 Collinear approach Evolution → DGLAP eqs. Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Factorization A cornerstone in p. QCD TMD approach…more involved

TMD Factorization and evolution Collins approach (2011) Collinear PDF p. QCD Theor. equivalent but

TMD Factorization and evolution Collins approach (2011) Collinear PDF p. QCD Theor. equivalent but potentially different in phen. Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 DY processes 12 Non perturbative parts Role of NON perturbative input

TMDs and unpolarized cross sections SIDIS multiplicities 13 Spin effects in QCD and 3

TMDs and unpolarized cross sections SIDIS multiplicities 13 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Anselmino, Boglione, Gonzalez, Melis, Prokudin (2014) Signori, Bacchetta, Radici, Schnell (2013)

TMDs: flavour structure 14 Spin effects in QCD and 3 D nucleon structure U.

TMDs: flavour structure 14 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Gaussian widths Signori, Bacchetta, Radici, Schnell (2013) up < down < sea ? ? to be further explored

15 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University

15 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 TMD evolution at NNLL (SCET) UD, Echevarria, Melis, Scimemi (2014) (223 data points) Tevatron Low energy

UD, Echevarria, Melis, Scimemi (2014) Spin effects in QCD and 3 D nucleon structure

UD, Echevarria, Melis, Scimemi (2014) Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Pure p. QCD 16 TMDs at LHC Predictions from NNLL fit Ferrera (2014)

TMDs and spin Correlation between the spin of the proton and the parton transverse

TMDs and spin Correlation between the spin of the proton and the parton transverse momentum Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Sivers (1989) 17

Analogously, one can define TMDs in the fragmentation process. In particular, for its relevance

Analogously, one can define TMDs in the fragmentation process. In particular, for its relevance Correlation between the spin of the fragmenting quark and the hadron transverse momentum Crucial for the first ever extraction of the transversity distribution Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Collins (1992) 18

Sivers and Collins functions extensively studied theoretically, experimentally and phenomenologically 19 SIDIS Collins Sivers

Sivers and Collins functions extensively studied theoretically, experimentally and phenomenologically 19 SIDIS Collins Sivers First phase: analysis with DGLAP evolution Second phase (just started): TMD evolution Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 CLEAR evidence from data HERMES, COMPASS

Extracted Sivers functions TO-CA and PV groups Effect of TMD evolution Aybat, Collins, Qiu,

Extracted Sivers functions TO-CA and PV groups Effect of TMD evolution Aybat, Collins, Qiu, Rogers (2012) Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 sea region: unconstrained [→EIC] 20

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University &

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Non zero Sivers effect related to parton orbital angular momentum 21 Distortion in the transverse plane

Modified universality of the Sivers function Final state interactions in SIDIS Initial state interactions

Modified universality of the Sivers function Final state interactions in SIDIS Initial state interactions in DY Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Collins (2012) 22 A clear-cut test If falsified: - misunderstanding of final-state interacts. leading to T-odd effects - missing points in QCD factorization (TMD and collinear) [most severe scenario]

23 No TMD evolution Spin effects in QCD and 3 D nucleon structure U.

23 No TMD evolution Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 STAR Collaboration (2016) First hint at the sign change, but large exp. errors and … Kang et al (2016)

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University &

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Sign reversed 24 New analysis: (in progress) Anselmino, Boglione, UD, Murgia, Prokudin (2016)

Collins function & transversity Without TMD evolution Anselmino, Boglione, UD, Melis, Murgia, Prokudin (2015)

Collins function & transversity Without TMD evolution Anselmino, Boglione, UD, Melis, Murgia, Prokudin (2015) Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Combined analysis of SIDIS 25

Same analysis but with TMD evolution Kang, Prokudin, Sun, Yuan (2015) 26 Spin effects

Same analysis but with TMD evolution Kang, Prokudin, Sun, Yuan (2015) 26 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 No compelling TMD evolution yet Remember: SSAs are ratios….

27 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University

27 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Collins effect alone Sivers effect alone Non separable In a phenomenological TMD scheme

28 Collinear factorization: proven Qiu, Sterman (1991) Spin effects in QCD and 3 D

28 Collinear factorization: proven Qiu, Sterman (1991) Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Twist-three functions corresponding, and related, to the TMDs, like Boer, Mulders, Piljman (2003)

In the meantime …. 29 Spin effects in QCD and 3 D nucleon structure

In the meantime …. 29 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Predictions from TMD fact. at LO + Weizsäcker-Williams approximation HERMES data (2014) UD, Flore, Murgia (2016) [LO] Anselmino, Boglione, UD, Melis, Murgia, Prokudin (2010&2014)

30 Data from STAR Collaboration (2015) Spin effects in QCD and 3 D nucleon

30 Data from STAR Collaboration (2015) Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 500 Ge. V 200 Ge. V UD, Murgia, Pisano (2011, 2016) without TMD evolution Universality of the Collins function and mild (or no) TMD evolution

Open issues in TMD phenomenology Kang (2015) w/o TMD evolution Role of non perturbative

Open issues in TMD phenomenology Kang (2015) w/o TMD evolution Role of non perturbative input choices Transverse momentum dependence in SIDIS and its consistency with DY Gluon TMDs at low x and parton saturation, TMD factorization vs. Color Glass Condensate Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 TMD evolution and its relevance An example 31

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University &

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Non trivial decomposition [Leader, Lorcé (2014)] 32 Proton spin puzzle

GPDs: few hints Virtual Compton scattering Form Factor: Position information No sensitivity to quark

GPDs: few hints Virtual Compton scattering Form Factor: Position information No sensitivity to quark momentum Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Elastic scattering GPDs: Information on position and quark momentum fraction 33

34 DVCS Factorization Spin effects in QCD and 3 D nucleon structure U. D'Alesio

34 DVCS Factorization Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Collins et al. (1998) Compton Form Factor GPD

35 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University

35 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016

Physics issues in GPDs golden channel. Measured at HERMES, COMPASS, CLASS, H 1, ZEUS

Physics issues in GPDs golden channel. Measured at HERMES, COMPASS, CLASS, H 1, ZEUS - DVMP (virtual meson product): uncertainty on meson distr. amplit. - Extraction of GPDs: model-dependent - Parameterizations: different families, not always able to describe all data, qualitatively good (different observables, few parameters and assumptions) - Major role in the nucleon spin decomposition Ji (1997) Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 - DVCS: 36

37 Future → EIC Spin effects in QCD and 3 D nucleon structure U.

37 Future → EIC Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 JLAB

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University &

Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 38 Conclusions and open issues

Research activities in Italy 39 Spin effects in QCD and 3 D nucleon structure

Research activities in Italy 39 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Theory NINPHA National Initiative on Physics of Hadrons Experiments COMPASS JLAB Thank you

40 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University

40 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 BACK-UP SLIDES

Access to the gluon Sivers function 41 Spin effects in QCD and 3 D

Access to the gluon Sivers function 41 Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 PHENIX Collaboration data (2014) All other effects are washed out UD, Murgia, Pisano JHEP 09 (2015)

Seminal paper TMD framework Spin effects in QCD and 3 D nucleon structure U.

Seminal paper TMD framework Spin effects in QCD and 3 D nucleon structure U. D'Alesio (Cagliari University & INFN) 15/11/2016 INFN 2016 Tremendous progress 42 TMD factorization approaches