The propagation of colored quarks through strongly interacting systems, and their subsequent evolution into color-singlet hadrons, are phenomena that showcase unique facets of Quantum Chromodynamics (QCD). Medium-stimulated gluon bremsstrahlung, a fundamental QCD process, induces broadening of the transverse momentum of the parton, and creates partonic energy loss manifesting itself in experimental observables that are accessible in high energy interactions in hot and cold systems. The formation of hadrons, which is the dynamical enforcement of the QCD confinement principle, is very poorly understood on the basis of fundamental theory, although detailed models such as the Lund string model or cluster hadronization models can generally be tu...
The topical workshop Strong QCD from Hadron Structure Experiments took place at Jefferson Lab from N...
We present an extension to the colour reconnection model in the Monte Carlo event generator Herwig t...
The J-PARC is a hadron-accelerator facility to provide secondary beams of kaons, pions, neutrinos, m...
Over the last few decades, several experiments have used atomic nuclei as unique laboratories to pro...
The CLAS experiment E02-104, part of the EG2 run at Jefferson Lab, was performed to study the hadron...
The basic questions are always been asked by the mankind that, ``What are the constituents of matter...
The production of heavy quarkonium as QQbar bound-states in hadron-hadron collisions is considered w...
We discuss the empirical evidence for a universal Color Glass Condensate and outline prospects for f...
We present a new model for the description of heavy-flavor hadronization in high-energy nuclear (and...
These lectures stress the theoretical elements that underlie a wide range of phenomenological studie...
Quantum Chromo-Dynamics (QCD) is now well established as the theory for strong interaction of quarks...
Mapping the transition of the strong interaction from the hadronic degrees of freedom to the partoni...
Quantum Chromodynamics (QCD) is the correct theory of strong interactions. The main direction of inv...
Recent results on studies of the structure of nucleons and nuclei in the regime of strong interactio...
We outline theoretical ideas on the soft and hard dynamics of strong high-energy interactions and di...
The topical workshop Strong QCD from Hadron Structure Experiments took place at Jefferson Lab from N...
We present an extension to the colour reconnection model in the Monte Carlo event generator Herwig t...
The J-PARC is a hadron-accelerator facility to provide secondary beams of kaons, pions, neutrinos, m...
Over the last few decades, several experiments have used atomic nuclei as unique laboratories to pro...
The CLAS experiment E02-104, part of the EG2 run at Jefferson Lab, was performed to study the hadron...
The basic questions are always been asked by the mankind that, ``What are the constituents of matter...
The production of heavy quarkonium as QQbar bound-states in hadron-hadron collisions is considered w...
We discuss the empirical evidence for a universal Color Glass Condensate and outline prospects for f...
We present a new model for the description of heavy-flavor hadronization in high-energy nuclear (and...
These lectures stress the theoretical elements that underlie a wide range of phenomenological studie...
Quantum Chromo-Dynamics (QCD) is now well established as the theory for strong interaction of quarks...
Mapping the transition of the strong interaction from the hadronic degrees of freedom to the partoni...
Quantum Chromodynamics (QCD) is the correct theory of strong interactions. The main direction of inv...
Recent results on studies of the structure of nucleons and nuclei in the regime of strong interactio...
We outline theoretical ideas on the soft and hard dynamics of strong high-energy interactions and di...
The topical workshop Strong QCD from Hadron Structure Experiments took place at Jefferson Lab from N...
We present an extension to the colour reconnection model in the Monte Carlo event generator Herwig t...
The J-PARC is a hadron-accelerator facility to provide secondary beams of kaons, pions, neutrinos, m...