519 research outputs found
Are hadrons simpler than they seem?
I briefly review a systematic approximation scheme of QCD in which the quark
model picture of hadrons emerges at lowest order. A linear A^0 potential arises
if Gauss' law is solved with a non-vanishing boundary condition at spatial
infinity. Similarly to the Dirac case one can describe relativistic states
including any number of particle pairs (sea quarks) using valence wave
functions, whose norms give {\em inclusive} probability densities. Provided
\alpha_s(Q^2) freezes in the infrared, perturbative corrections to the S-matrix
can be calculated in the usual way, but with states bound by the linear
\order{\alpha_s^0} potential instead of plane waves in the in and out states.Comment: 4 pages. Talk presented at the 3rd Workshop on the QCD Structure of
the Nucleon (QCD-N'12), 22-26 October 2012 in Bilbao, Spai
Measuring transverse size with virtual photons
Fourier transforming the virtual photon transverse momentum in \gamma*(q)+N
\to f processes allows new insight into hadron dynamics as a function of impact
parameter b. I discuss how previous analyses of charge density based on elastic
and transition form factors (f=N, N*) can be generalized to any multi-hadron
final state (f=\pi N, \pi\pi N, \bar D \Lambda_c,...). The b-distribution
determines the transverse positions of the quarks that the photon couples to,
and can be studied as a function of multiplicity, the relative transverse
momenta, quark masses and polarization. The method requires no factorization
nor leading twist approximation. Data with spacelike photon virtualities in the
range 0 1/Q_{max} in impact
parameter.Comment: Talk at the Third International Workshop on Transverse Polarization
Phenomena in Hard Scattering (Transversity 2011), in Veli Losinj, Croatia, 29
August - 2 September 2011. 7 page
Duality in Semi-Exclusive Processes
Bloom-Gilman duality relates parton distributions to nucleon form factors and
thus constrains the dynamics of exclusive processes. The quark electric charge
dependence implies that exclusive scattering is incoherent on the quarks even
at high momentum transfers. Data on semi-exclusive meson production exceeds the
duality prediction by more than an order of magnitude and violates quark
helicity conservation. This suggests that the subprocess is dominated by soft
`endpoint' contributions which obey dimensional scaling. The large transverse
size of the subprocess may explain the absence of color transparency in fixed
angle processes.Comment: Talk at the ``Workshop on Exclusive Processes at High Momentum
Transfer'' at Jefferson Laboratory, Newport News, USA (May 2002). 7 page
Summary Talk on Quark-Hadron Duality
I ascribe the origin of Bloom-Gilman duality in DIS to a separation of scales
between the hard subprocess and soft resonance formation. The success of
duality indicates that the subprocesses of exclusive form factors are the same
as in DIS. The observed dominance of the longitudinal structure function at
large x in \pi N \to \mu^+\mu^- X can explain why local duality works for DIS
with a pion target. The failure of duality in semi-exclusive processes
indicates that high momentum transfer t is not sufficient to make the
corresponding subprocesses compact.Comment: 8 pages, 5 figures. Summary talk at the First Workshop on
Quark-Hadron Duality and the Transition to pQCD, Frascati, 6-8 June 200
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