1 / 16

Nucleon tomography through exclusive and semi-inclusive processes

International Workshop on Hadron Structure and Spectroscopy Lisbon, 16-18 April 2012. Nucleon tomography through exclusive and semi-inclusive processes. Cédric Lorcé. and. 17 Apr 2012, LIP, Lisbon, Portugal. Outline. Exclusive vs. Semi-inclusive DVCS vs. SIDIS GPDs vs. TMDs

gali
Download Presentation

Nucleon tomography through exclusive and semi-inclusive processes

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. International Workshop on Hadron Structure and Spectroscopy Lisbon, 16-18 April 2012 Nucleon tomography through exclusive and semi-inclusive processes Cédric Lorcé and 17 Apr 2012, LIP, Lisbon, Portugal

  2. Outline • Exclusive vs. Semi-inclusive • DVCS vs. SIDIS • GPDs vs. TMDs • Partonic interpretation • 3D imaging • Twist-2 and Twist-3 • Hadron structure • Angular momentum decompositions • Quark spin and OAM • Interesting relations

  3. DVCS vs. SIDIS Incoherent scattering DVCS SIDIS FFs GPDs TMDs Factorization Compton form factor Cross section hard soft • process dependent • perturbative • « universal » • non-perturbative

  4. GPDs vs. TMDs GPDs TMDs Dirac matrix Correlator Correlator Off-forward! Forward! Wilson line ISI FSI e.g. DY e.g. SIDIS

  5. Partonic interpretation Twist-2 ~ LO in U L T GPDs TMDs 3D imaging 3D imaging IPDs Impact parameter Transverse center of momentum [Soper (1977)] [Burkardt (2000,2003)] [Diehl, Hägler (2005)] Interpretation in gauge

  6. Complete picture GTMDs and Wigner distributions GTMDs 5D imaging TMDs TMFFs GPDs Wigner distribution TMSDs PDFs FFs Charges [C.L., Pasquini, Vanderhaeghen (2011)] [C.L., Pasquini (2011)]

  7. Twist-2 structure Monopole Dipole GPDs TMDs Quadrupole Quark polarization Quark polarization Nucleon polarization Nucleon polarization -odd Naive T-odd

  8. Twist-3 structure Parametrization [Meißner, Metz, Schlegel (2009)] GPDs TMDs Quark polarization Quark polarization Nucleon polarization Nucleon polarization -odd Naive T-odd

  9. Angular momentum decompositions Ji Jaffe-Manohar [Ji (1997)] [Jaffe, Manohar (1990)] Kinematic Canonical Pros: Pros: • Gauge-invariant decomposition • Accessible in DIS and DVCS • Satisfies canonical relations • Complete decomposition Cons: Cons: • Does not satisfy canonical relations • Incomplete decomposition • Gauge-variant decomposition • Missing observables for the OAM Improvements: Improvements: • Complete decomposition • Gauge-invariant extension [Wakamatsu (2009,2010)] [Chen et al. (2008)] • OAM accessible via Wigner distributions [C.L., Pasquini (2011)] [C.L., Pasquini, Xiong, Yuan(2011)] [Hatta (2011)]

  10. Quark spin and OAM GPDs TMDs Quark spin Quark spin Pretzelosity Ji sum rule [Ji (1997)] Twist-3 [Burkardt (2007)] [Efremov, Schweitzer, Teryaev, Zavada (2008,2010)] [She, Zhu, Ma (2009)] [Avakian, Efremov, Schweitzer, Yuan (2010)] [C.L., Pasquini (2011)] PPSS sum rule • Model-dependent • Not intrinsic OAM Pure twist-3! [Penttinen, Polyakov, Shuvaev, Strikman (2000)] TMDs Genuine sum rule GTMDs

  11. Interesting relations *=SU(6) Model relations Linear relations Quadratic relation Flavor-dependent * * * * * Flavor-independent * * * * * * * Bag LFcQSM LFCQM S Diquark AV Diquark Cov. Parton Quark Target [Jaffe, Ji (1991), Signal (1997), Barone & al. (2002), Avakian & al. (2008-2010)] [C.L., Pasquini, Vanderhaeghen (2011)] [Pasquini & al. (2005-2008)] [Ma & al. (1996-2009), Jakob & al. (1997), Bacchetta & al. (2008)] [Ma & al. (1996-2009), Jakob & al. (1997)][Bacchetta & al. (2008)] [Efremov & al. (2009)] [Meißner & al. (2007)]

  12. Geometrical explanation [C.L., Pasquini (2011)] Preliminaries Conditions: • Quasi-free quarks • Spherical symmetry Wigner rotation (reduces to Melosh rotation in case of FREE quarks) Canonical spin Light-front helicity

  13. Geometrical explanation Axial symmetry about z

  14. Geometrical explanation Axial symmetry about z

  15. Summary • Exclusive vs. Semi-inclusive • DVCS vs. SIDIS • Factorizationapproach • GPDs vs. TMDs • Quark-quark correlator • Partonicinterpretation • 3D imaging • Probabilisticinterpretation • Twist-2 and Twist-3 • Helicity structure • Hadron structure • Angularmomentumdecompositions • Short overview • Quark spin and OAM • Relation with observables • Interesting relations • Sphericalsymmetry in quark models

  16. Quark polarization Quark polarization Nucleon polarization Nucleon polarization LC helicity and canonical spin [C.L., Pasquini (2011)] LC helicity Canonical spin

More Related