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Before
the discovery of Quantum
Chromodynamics, the parton model
provided a correct description of
scaling violations in deep inelastic
leptoproduction. Today, we understand
the QCD basis for this model. Using
the light-cone operator product
expansion, one can organize
contributions to moments (integrals)
of structure functions in deep
inelastic scattering according to
their "twist", defined as
the difference between an operator's
canonical dimension and its spin. The
anomalous dimensions of leading twist
operators correspond to moments of the
splitting functions that appear in
DGLAP evolution of parton distribution
functions. Physically, the leading
twist/parton model contributions
correspond to those that arise from
the incoherent scattering of leptons
from point-like constituents of the
target.
At
sufficiently high-energy, the leading
twist contributions dominate. However,
as the Q2 of the scattering
process is lowered, power corrections
associated with higher twist
contributions may become important.
Physically, these contributions
correspond to effects that arise from
correlations between the quarks and
gluons inside the target during the
scattering process - correlations that
are absent from the leading twist
terms. If the higher twist
contributions can be observed and
correctly analyzed, they can provide a
new look into the substructure of
protons and neutrons, providing
interesting information about the
internal landscape of the nucleons
beyond the view we already have from
the parton model description.
Recently,
data collected by the CLAS
collaboration at Jefferson Laboratory
has uncovered what appear to be
signatures of higher twist effects in
structure function moments. The data
present puzzles that call for a
theoretical resolution. NPAC theorists
and their collaborators have
undertaken a study of these higher
twist effects, seeking to interpret
them rigorously within the context of
QCD. The long term goal is to be able
to extract from the data higher-twist
operator matrix elements that can be
compared with computations using
lattice QCD. We are also studying the
implications of higher twist
contributions for parity-violating
deep inelastic scattering, in view of
future experiments that are planned
for the Jefferson
Laboratory after the 12 GeV
upgrade. We hope to determine whether
these parity violation experiments can
provide a complementary window on the
higher twist structure of the proton.
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