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Hadron Physics
New theories are explored and discussed on establishing relations between the fundamental theory of strong interactions, known as QCD, and experiment. Powerful theoretical models, known as effective theories, based on symmetries of QCD, have been developed to address the non-perturbative regime of QCD in an approximate, yet quantitatively controllable way. The present workshop focussed on the most recent developments in this area. New results on meson and baryon physics are discussed as well and new directions towards the possible experimental confirmation of nuclear/quark matter and quark-gluon plasma are indicated.
Hadron Physics
New theories are explored and discussed on establishing relations between the fundamental theory of strong interactions, known as QCD, and experiment. Powerful theoretical models, known as effective theories, based on symmetries of QCD, have been developed to address the non-perturbative regime of QCD in an approximate, yet quantitatively controllable way. The present workshop focussed on the most recent developments in this area. New results on meson and baryon physics are discussed as well and new directions towards the possible experimental confirmation of nuclear/quark matter and quark-gluon plasma are indicated.
Hadron Physics: Effective Theories of Low Energy QCD
The study of hadrons unites a variety of theoretical approaches, ranging from low-energy QCD dynamics, chiral perturbation theory, and meson and baryon phenomenology, to the effects of hot and dense nuclear matter. Fruitful crosslinks between these topics had become clear in the recent past. These proceedings form a coherent overview of the actual state of low-energy hadron physics.
Strong Coupling Gauge Theories in LHC Era
The purpose of the Workshop is to have intensive discussions on both theoretical and phenomenological aspects of strong coupling gauge theories (SCGTs), with particular emphasis on the model buildings to be tested in the LHC experiments. Dynamical issues are discussed in lattice simulations and various analytical methods. This proceedings volume is a collection of the presentations made at the Workshop by many leading scientists in the field.
Strong Coupling Gauge Theories in LHC Era
The purpose of the Workshop is to have intensive discussions on both theoretical and phenomenological aspects of strong coupling gauge theories (SCGTs), with particular emphasis on the model buildings to be tested in the LHC experiments. Dynamical issues are discussed in lattice simulations and various analytical methods. This proceedings volume is a collection of the presentations made at the Workshop by many leading scientists in the field.
The London Stage
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The British Drama
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Strongly Interacting Matter in Magnetic Fields
The physics of strongly interacting matter in an external magnetic field is presently emerging as a topic of great cross-disciplinary interest for particle, nuclear, astro- and condensed matter physicists. It is known that strong magnetic fields are created in heavy ion collisions, an insight that has made it possible to study a variety of surprising and intriguing phenomena that emerge from the interplay of quantum anomalies, the topology of non-Abelian gauge fields, and the magnetic field. In particular, the non-trivial topological configurations of the gluon field induce a non-dissipative electric current in the presence of a magnetic field. These phenomena have led to an extended formula...
Chiral Quark Dynamics
These notes give an introduction to the description of hadrons, i.e., mesons and baryons, within a quark model based on a chirally invariant quantum field theory. Emphasis is put on a didactic approach intended for graduate students with some background on functional integral techniques. Starting from QCD a motivation of a specific form of the effective quark interaction is given. Functional integral bosonization leads to a theory describing successfully meson properties. It possesses solitonic solutions which are identified as baryons. Via functional integral techniques a Faddeev equation for baryons describing them as bound states of a diquark and a quark is derived. Finally, a unification of these two complementary pictures of baryons is proposed.
