Abstract
We report a calculation of the baryon magnetic moments using covariant chiral perturbation theory within the extended-on-mass-shell renormalization scheme including intermediate octet and decuplet contributions. By fitting the two available low-energy constants, we improve the Coleman-Glashow description of the data when we include the leading SU(3) breaking effects coming from the lowest-order loops. We compare with previous attempts at the same order using heavy-baryon and covariant infrared chiral perturbation theory, and discuss the source of the differences.
| Original language | English |
|---|---|
| Journal | Proceedings of Science |
| State | Published - 2009 |
| Externally published | Yes |
| Event | International Workshop on Effective Field Theories: From the Pion to the Upsilon, EFT 2009 - Valencia, Spain Duration: 2 Feb 2009 → 6 Feb 2009 |
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