482,292 research outputs found
JLab: Probing Hadronic Physics with Electrons and Photons
Precision measurements of the structure of nucleons and nuclei in the regime
of strong interaction QCD are now possible with the availability of high
current polarized electron beams, polarized targets, and recoil polarimeters,
in conjunction with modern spectrometers and detector instrumentation. The
physics at JLab will be highlighted using two recent measurements of general
interest. The ratio of the proton electric to magnetic form factors indicates
the importance of the role of angular momentum in the structure of the nucleon.
The existence of 5-quark configurations in the ground state wavefunctions of
hadrons is confirmed by a narrow peak attributed to an exotic baryon with
strangeness S=+1. These and other examples will be used to illustrate the
capabilities and focus of the experimental program at JLab.Comment: V Latinamerican Symposium on Nuclear Physics, Santos, Brazil (Sept
1-5, 2003) 4 pages, 4 figure
Circuit switches latching relay in response to signals of different polarity
A circuit using one power supply and two storage capacitors, which may be separately discharged in opposite directions through a relay in response to change in polarity of a signal, is described
Review of Recent Jlab Results
High quality polarized electron beams at Jefferson Lab make possible
precision measurements of hadronic properties in the regime of strongly
interacting QCD. We will describe a few programs at Jefferson Lab that are
making measurements that link the basic static properties of hadrons to their
quark sub-structure. For example, parity-violating electron proton elastic
scattering probes the spatial distribution of strange quarks in the nucleon.
The nucleon-Delta transition form factors give us information about the
deformation of nucleons and Deltas. Finally, new high statistics measurements
of photons scattering off proton and deuteron targets are used to set upper
limits on the production of exotic baryons with strangeness S=+1. These
examples will be used to illustrate the capabilities and focus of the
experimental program at JLab.Comment: Contribution to XI International Conference on Hadron Spectroscopy, 4
figure
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