Light-front densities for transversely polarized hadrons Lorcé Cédric Mainz University Germany *4th Workshop on ERHMT, JLAb, Newport News, Virginia USA.

Slides:



Advertisements
Similar presentations
Cédric Lorcé IPN Orsay - LPT Orsay Observability of the different proton spin decompositions June , University of Glasgow, UK CLAS12 3rd European.
Advertisements

Rory Miskimen University of Massachusetts, Amherst
Cédric Lorcé IFPA Liège ECT* Colloquium: Introduction to quark and gluon angular momentum August 25, 2014, ECT*, Trento, Italy Spin and Orbital Angular.
Onset of Scaling in Exclusive Processes Marco Mirazita Istituto Nazionale di Fisica Nucleare Laboratori Nazionali di Frascati First Workshop on Quark-Hadron.
Cédric Lorcé SLAC & IFPA Liège How to define and access quark and gluon contributions to the proton spin December 2, 2014, IIT Bombay, Bombay, India INTERNATIONAL.
Jefferson Lab/Hampton U
DESY PRC May 10, Beyond the One Photon Approximation in Lepton Scattering: A Definitive Experiment at DESY for J. Arrington (Argonne) D. Hasell,
Marc Vanderhaeghen Johannes Gutenberg Universität, Mainz Olympus Coll. Meeting, DESY, February 23-24, 2010 TexPoint fonts used in EMF. Read the TexPoint.
Nuclear de-excitation Outline of approach… Source of radiation Propagation of radiation field Detection of radiation ?? nucleus.
Cédric Lorcé SLAC & IFPA Liège Transversity and orbital angular momentum January 23, 2015, JLab, Newport News, USA.
LEPTON PAIR PRODUCTION AS A PROBE OF TWO PHOTON EFFECTS IN EXCLUSIVE PHOTON-HADRON SCATTERING Pervez Hoodbhoy Quaid-e-Azam University Islamabad.
1 Updates on Transversity Experiments and Interpretations Jen-Chieh Peng Transversity Collaboration Meeting, JLab, March 4, 2005 University of Illinois.
Xiangdong Ji University of Maryland/SJTU Physics of gluon polarization Jlab, May 9, 2013.
Xiangdong Ji University of Maryland/SJTU
Electromagnetic form factors in the relativized Hypercentral CQM M. De Sanctis, M.M.Giannini, E. Santopinto, A. Vassallo Introduction The hypercentral.
Cédric Lorcé IPN Orsay - LPT Orsay Orbital Angular Momentum in QCD June , Dipartimento di Fisica, Universita’ di Pavia, Italy.
1 Transverse weighting for quark correlators QCD workshop, JLAB, May 2012 Maarten Buffing & Piet Mulders
Generalized Transverse- Momentum Distributions Cédric Lorcé Mainz University Germany Barbara Pasquini Pavia University Italy In collaboration with:
Spin Azimuthal Asymmetries in Semi-Inclusive DIS at JLAB  Nucleon spin & transverse momentum of partons  Transverse-momentum dependent distributions.
Spin-Flavor Decomposition J. P. Chen, Jefferson Lab PVSA Workshop, April 26-27, 2007, Brookhaven National Lab  Polarized Inclusive DIS,  u/u and  d/d.
Trilinear Gauge Couplings at TESLA Photon Collider Ivanka Božović - Jelisavčić & Klaus Mönig DESY/Zeuthen.
Cédric Lorcé IFPA Liège Multidimensional pictures of the nucleon (3/3) June 30-July 4, 2014, LPT, Paris-Sud University, Orsay, France Second International.
Electromagnetic N →  (1232) Transition Shin Nan Yang Department of Physic, National Taiwan University  Motivations  Model for  * N →  N DMT (Dubna-Mainz-Taipei)
Ralf W. Gothe 1  Basic Tools: Experiment and Theory  Goals: Unveil the dynamics of the strong interaction  Connections: Not everything is difficult.
Higher order forward spin polarizabilities Barbara Pasquini Pavia U. and INFN Pavia Paolo Pedroni Dieter Drechsel Paolo Pedroni Dieter Drechsel INFN Pavia.
Wigner Distributions and light-front quark models Barbara Pasquini Pavia U. & INFN, Pavia in collaboration with Cédric Lorcé Feng Yuan Xiaonu Xiong IPN.
Generalized TMDs of the Proton Barbara Pasquini Pavia U. & INFN, Pavia in collaboration with Cédric Lorcé Mainz U. & INFN, Pavia.
Methods of excitation: nuclear reactions
Deeply Virtual Meson Production and Transversity GPDs Valery Kubarovsky Jefferson Lab 1 Exclusive Meson Production and Short-Range Hadron Structure January.
EIC, Nucleon Spin Structure, Lattice QCD Xiangdong Ji University of Maryland.
Thomas Jefferson National Accelerator Facility PAC-25, January 17, 2004, 1 Baldin Sum Rule Hall C: E Q 2 -evolution of GDH integral Hall A: E94-010,
Baryon Resonance Analysis from MAID D. Drechsel, S. Kamalov, L. Tiator.
GPD and underlying spin structure of the nucleon M. Wakamatsu and H. Tsujimoto (Osaka Univ.) 1. Introduction - Still unsolved fundamental puzzle in hadron.
Symmetries of the Cranked Mean Field S. Frauendorf Department of Physics University of Notre Dame USA IKH, Forschungszentrum Rossendorf, Dresden Germany.
Cédric Lorcé IPN Orsay - LPT Orsay Introduction to the GTMDs and the Wigner distributions June , Palace Hotel, Como, Italy.
Wigner distributions and quark orbital angular momentum Cédric Lorcé and May , JLab, Newport News, VA, USA.
OAM in transverse densities and resonances Cédric Lorcé and 09 Feb 2012, INT, Seattle, USA INT Workshop INT-12-49W Orbital Angular Momentum in QCD February.
Nuclear and Radiation Physics, BAU, 1 st Semester, (Saed Dababneh). 1 Electromagnetic moments Electromagnetic interaction  information about.
Single spin asymmetries in pp scattering Piet Mulders Trento July 2-6, 2006 _.
Tensor and Flavor-singlet Axial Charges and Their Scale Dependencies Hanxin He China Institute of Atomic Energy.
GPD and underlying spin structure of the Nucleon M. Wakamatsu and H. Tsujimoto (Osaka Univ.) 1. Introduction Still unsolved fundamental puzzle in hadron.
Transverse-Momentum Distributions and spherical symmetry Cédric Lorcé Mainz University Germany in collaboration with Barbara Pasquini Pavia University.
Marc Vanderhaeghen 1 Introduction LEPP16 Marc Vanderhaeghen LEPP16 Workshop Kupferberg, Mainz, April 4-7, 2016 New Vistas in Low-Energy Precision Physics.
Generalized Parton Distributions: A general unifying tool for exploring the internal structure of hadrons INPC, 06/06/2013.
Proton spin structure in phase-space May 17, FSU Alumni Center, Tallahassee, Florida, USA Cédric Lorcé CPhT Baryons May 2016 Florida State University.
A sideways look into the proton Transverse momentum and transverse spin in QCD Alessandro Bacchetta.
PV Electron Scattering
Quantum imaging of the proton via Wigner distributions
Sep 21st 2015, INFN Frascati National Laboratories, Frascati, Italy
June 28, Temple University, Philadelphia, USA
June , Dipartimento di Fisica, Universita’ di Pavia, Italy
May , JLab, Newport News, VA, USA
Theory : phenomenology support 12 GeV
for STAR Collaboration
Structure and Dynamics of the Nucleon Spin on the Light-Cone
Quark’s angular momentum densities in position space
New Results for Transverse Spin Effects at COMPASS
August 29, Riken Tokyo Office, Tokyo, Japan
Hadron Form Factors Rolf Ent Jefferson Lab
March 16, meeting Y. Koike (BNL/Niigata Univ.)
§3.4.1–3 Multipole expansion
Transverse distributions of polarized quarks
Christopher Crawford PHY
Large-X PDFs in the Drell-Yan Process
Quark and Gluon Sivers Functions
Quark Parton Model (QPM)
Transverse distributions of polarized quarks
Single spin asymmetries in semi-inclusive DIS
Institute of Modern Physics Chinese Academy of Sciences
Presentation transcript:

Light-front densities for transversely polarized hadrons Lorcé Cédric Mainz University Germany *4th Workshop on ERHMT, JLAb, Newport News, Virginia USA (May 18-21, 2010) *

Outline Picture in the transverse plane Form Factors Generalized Polarizabilities GTMDs & Co.

Standard Picture Breit frame BUT Lorentz contraction Creation/annihilation of pairs NO probability/charge density interpretation [Ernst, Sachs, Wali (1960)] [Sachs (1962)]

Correct Picture Extreme Lorentz contraction 2D picture No creation/annihilation of massive pairs Light-front frame [Burkardt (2001,2003)]

Transverse Charge Densities p n Long. pol.Transv. pol. Electric dipole! [Miller (2007)][Carlson & Vdh (2008)]

B int Transverse Charge Densities MonopoleAnomalous! Interpretation: Transversity basis S d Induced EDM Dipole u d X

dipole Similarly for higher spins quadrupolemonopoleoctupole 2j+1 circular multipoles! =+++ Transverse Charge Densities [Lorcé (2009)] [Alexandrou et al. (2008,2009)] Distortions of transverse charge densities due to anomalous values of EM moments Claim:

Higher Spins 2j+1 circular multipoles! [Lorcé (2009)] ChargenormalizationUniversal g=2 factor Dirac EW SM Supergravity

Generalized Polarizabilities VCS in low limit described by 6 GPs Linear response to external quasi-static dipole electric field

Generalized Polarizabilities [Gorchtein, Lorcé, Pasquini, Vdh (2010)] dipole quadrupole monopole Only 3 linear combinations available! EEE

GTMDs (Generalized Transverse Momentum dependent parton Distributions) Complete parametrization [Meißner, Metz, Schlegel (2009)] Probabilistic interpretation in impact-parameter space with dd

,  GCDs (Generalized transverse Charge Densities) [Lorcé, Pasquini (in preparation)] k T b Unpolarized u quark in unpolarized proton k T  fixed

GCDs (Generalized transverse Charge Densities) [Lorcé, Pasquini (in preparation)] k T Unpolarized u quark in unpolarized proton k T fixed =+

GCDs (Generalized transverse Charge Densities) [Lorcé, Pasquini (in preparation)],k T  fixed k T k T k T k T Unpolarized u quark in unpolarized proton

GCDs (Generalized transverse Charge Densities) [Lorcé, Pasquini (in preparation)] Unpolarized u and d quarks in unpolarized proton  u  d More u than d in central region!

FFs  Correct picture on the light front  Distortions of densities due to anomalous moments  « Natural » EM moments form a pseudo-Pascal triangle GPs  VCS amplitude in the light front  3 out of 6 mapped out GTMDs & Co.  Full information  Anisotropic distribution of  u/d quarks dominance in central region of proton/neutron Summary k T