Three dimensional imaging of the nucleon --- TMD (theory and phenomenology)

Abstract

This is intend to provide an overview of the theoretical and phenomenological parts of the TMD (Transverse Momentum Dependent parton distribution and fragmentation functions) studies. By comparing with the theoretical framework that we have for the inclusive deep inelastic lepton-nucleon scattering and the one-dimensional imaging of the nucleon, I try to outline what we need to do in order to construct a comprehensive theoretical framework for semi-inclusive reactions and the three dimensional imaging of the nucleon. After that, I try to give an overview of what we have already achieved and make an outlook for the future.

plenary talk at the 21st International Symposium on Spin Physics, Oct 20-24, 2014, Peking University, Beijing, China

References in corpus (11)

• Sivers Effect for Pion and Kaon Production in Semi-Inclusive Deep Inelastic Scattering
• Dilepton production from polarized hadron hadron collisions
• TMDlib and TMDplotter: library and plotting tools for transverse-momentum-dependent parton distributions
• QCD Evolution of the Transverse Momentum Dependent Correlations
• Nucleon tensor charge from Collins azimuthal asymmetry measurements
• A systematic phenomenological study of the $\cos 2\varphi$ asymmetry in unpolarized semi--inclusive DIS
• Extracting Boer-Mulders functions from $p+D$ Drell-Yan processes
• Twist-4 contributions to the azimuthal asymmetry in SIDIS
• Azimuthal and single spin asymmetry in deep-inelastic lepton-nucleon scattering
• Leading and higher twist contributions in semi-inclusive e+e- annihilation at high energies
• $\cos 2\varphi$ asymmetries in unpolarized semi-inclusive DIS

Cited by in corpus (4)

• Global polarization effect and spin-orbit coupling in strong interaction
• Tensor polarization dependent fragmentation functions and e+e-\to V πX at high energies
• Twist-4 contributions to semi-inclusive deeply inelastic scatterings with polarized beam and target
• Twist-4 contributions to semi-inclusive $e^{+}{e}^{-}$-annihilation process