Abstract
The calculation of electromagnetic transition moments has been recognized as a powerful tool to help discriminate among models of hadronic structure. Here, SU(3)-flavor baryon octet-to-decuplet transition moments are examined within a quenched lattice QCD simulation. The pattern of flavor symmetry breaking for the transition moments is found to be more similar to that of decuplet than octet magnetic moments and suggests that the constituent quark model can better account for decuplet than octet structure. The lattice magnetic dipole transition moment for the Nλ → Δ channel is found to be in agreement with recent (model-dependent) experimental determinations. The lattice results indicate μpΔ/μp = 0.88(15) for pγ → Δ+. For the hyperon electromagnetic transitions, the significant nonvanishing signals for the E2/M1 ratio in Ξ - and ∑- electromagnetic transitions are of particular interest.
Original language | English |
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Pages (from-to) | 427-430 |
Number of pages | 4 |
Journal | Nuclear Physics B - Proceedings Supplements |
Volume | 30 |
Issue number | C |
DOIs | |
State | Published - Mar 1993 |
Bibliographical note
Funding Information:This work is supported in part by the U.S. Department of Energy under grant numbers DE-FG05-84ER40154 and DE-FG05-87ER-40322, by the National Science Foundation under grant number STI-9108764 and by the Natural Sciences and Engineering Research Council of Canada.
Funding
This work is supported in part by the U.S. Department of Energy under grant numbers DE-FG05-84ER40154 and DE-FG05-87ER-40322, by the National Science Foundation under grant number STI-9108764 and by the Natural Sciences and Engineering Research Council of Canada.
Funders | Funder number |
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National Science Foundation Arctic Social Science Program | STI-9108764 |
National Science Foundation Arctic Social Science Program | |
U.S. Department of Energy EPSCoR | DE-FG05-84ER40154, DE-FG05-87ER-40322 |
U.S. Department of Energy EPSCoR | |
Natural Sciences and Engineering Research Council of Canada |
ASJC Scopus subject areas
- Atomic and Molecular Physics, and Optics
- Nuclear and High Energy Physics