Decuplet baryon masses in covariant baryon chiral perturbation theory

Xiu-Lei Ren, Li-Sheng Geng, and Jie Meng
Phys. Rev. D 89, 054034 – Published 26 March 2014

Abstract

We present an analysis of the lowest-lying decuplet baryon masses in the covariant baryon chiral perturbation theory with the extended-on-mass-shell scheme up to next-to-next-to-next-to-leading order. In order to determine the 14 low-energy constants, we perform a simultaneous fit of the nf=2+1 lattice QCD data from the PACS-CS, QCDSF-UKQCD, and HSC Collaborations, taking finite-volume corrections into account self-consistently. We show that up to next-to-next-to-next-to-leading order one can achieve a good description of the lattice QCD and experimental data. Surprisingly, we note that the current lattice decuplet baryon masses can be fitted rather well by the next-to-leading order baryon chiral perturbation theory, which, however, misses the experimental data a little bit. Furthermore, we predict the pion- and strangeness-sigma terms of the decuplet baryons by use of the Feynman-Hellmann theorem.

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  • Received 18 November 2013

DOI:https://doi.org/10.1103/PhysRevD.89.054034

© 2014 American Physical Society

Authors & Affiliations

Xiu-Lei Ren1, Li-Sheng Geng1,2,*, and Jie Meng1,3,4

  • 1School of Physics and Nuclear Energy Engineering and International Research Center for Nuclei and Particles in the Cosmos, Beihang University, Beijing 100191, China
  • 2Physik Department, Technische Universität München, D-85747 Garching, Germany
  • 3State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, China
  • 4Department of Physics, University of Stellenbosch, Stellenbosch 7602, South Africa

  • *lisheng.geng@buaa.edu.cn

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Vol. 89, Iss. 5 — 1 March 2014

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