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The ODU theory group performs research across a broad range of topics in
hadronic and nuclear physics, from the keV energy scale in light
nuclei to the scattering of nucleons at multi-GeV energies. Their work
is of relevance to experiments across the globe, with particular
emphasis on experiments performed at the nearby Jefferson Lab, where
all group members are also staff scientists.
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Quantum ChromoDynamics at High Energy (Ian Balitsky)
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At high energies, the theory of QCD can be described
perturbatively in terms of explicit interactions between
quarks and gluons. Within this framework, recent and current topics of study
include calculations of Deeply Virtual Compton Scattering(DVCS) at
small x, scattering of color dipoles corresponding to fast
moving quark-antiquark pairs of finite size and construction
of an effective theory, valid at high energy, that recasts the
gluonic dynamics of QCD in terms of Wilson lines of the gauge
field.
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Hadron Spectroscopy and Lattice QCD (Jozef Dudek)
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Interests include the study of the spectrum and decays of hadronic resonances. This includes the extraction of resonance properties from experimental data by the building of models describing the hadronic reaction involved. The nature of these states is investigated using models at the quark level and, where possible, by a controlled approximation to
QCD named Lattice QCD. Lattice QCD considers the quark and gluon fields to live on a four-dimensional grid of spacetime
points, rendering the number of degrees-of-freedom finite and casting it into a form suitable for numerical computation.
Large-scale computing resources are utilised to compute observable quantities. Recent work includes the spectrum of the
charmonium mesons as well as their radiative and two-photon decays. Future work will apply these and other methods to light-quark systems.
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At intermediate energies, hadronic observables can often
be separated into pieces sensitive to short distances
and calculable in perturbative QCD and other pieces,
sensitive to longer distances, that are essentially
non-perturbative. An example of these non-perturbative
objects are the Generalised Parton Distributions(GPDs) that
describe the quark-gluon substructure of the
nucleon. These are an ongoing research interest that is
being modeled in a number of ways, including their estimation in the QCD Sum-Rule approach
which utilises the condensates of quarks and gluons that
fill the vacuum of QCD. Defining the connection between
GPDs and experimental observables in processes like DVCS
and wide-angle Compton scattering remains an active area
of research.
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Studies of Light Nuclei from keV to GeV Energies (Rocco Schiavilla)
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Nuclear structure can be studied precisely using the response to
probes electromagnetic and weak in nature. Studies of few-body systems are
aimed at producing a quantitative understanding of the structure and
dynamics of light nuclei with A<8 based on realistic interaction
models, and electroweak current operators constructed consistently
with these interactions. Exact Monte Carlo methods suitable for the
nuclear many-body problem are being developed and applied to investigate a wide variety of properties depending on the bound and continuum spectra of the nuclei, such as for example, very low-energy electroweak capture reactions, or the response to lepton and hadronic probes in the quasi-elastic
regime.
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Relativistic Dynamics in Hadrons and Nuclei (Wally Van Orden)
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At the energy and momentum transfers typical of
experiments at Jefferson Lab, it is necessary to include the effects
of special relativity in any calculation of electron scattering
reaction from nuclei. It has also been shown that for surprising
large energy and momentum transfers it is still appropriate to describe nuclei as consisting of nucleons interacting through the exchange of mesons. Models of
nuclei under these conditions can be constructed using techniques related to the relativistic Bethe-Salpeter equation for two- and many-nucleon systems. Similar techniques have also been applied to relativistic constituent quark models
of mesons and baryons.
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