TY - JOUR
T1 - Consistency between SU(3) and SU(2) covariant baryon chiral perturbation theory for the nucleon mass
AU - Ren, Xiu Lei
AU - Alvarez-Ruso, L.
AU - Geng, Li Sheng
AU - Ledwig, Tim
AU - Meng, Jie
AU - Vicente Vacas, M. J.
N1 - Publisher Copyright:
© 2017 The Author(s)
PY - 2017/3/10
Y1 - 2017/3/10
N2 - Treating the strange quark mass as a heavy scale compared to the light quark mass, we perform a matching of the nucleon mass in the SU(3) sector to the two-flavor case in covariant baryon chiral perturbation theory. The validity of the 19 low-energy constants appearing in the octet baryon masses up to next-to-next-to-next-to-leading order [1] is supported by comparing the effective parameters (the combinations of the 19 couplings) with the corresponding low-energy constants in the SU(2) sector [2]. In addition, it is shown that the dependence of the effective parameters and the pion-nucleon sigma term on the strange quark mass is relatively weak around its physical value, thus providing support to the assumption made in Ref. [2] that the SU(2) baryon chiral perturbation theory can be applied to study nf=2+1 lattice QCD simulations as long as the strange quark mass is close to its physical value.
AB - Treating the strange quark mass as a heavy scale compared to the light quark mass, we perform a matching of the nucleon mass in the SU(3) sector to the two-flavor case in covariant baryon chiral perturbation theory. The validity of the 19 low-energy constants appearing in the octet baryon masses up to next-to-next-to-next-to-leading order [1] is supported by comparing the effective parameters (the combinations of the 19 couplings) with the corresponding low-energy constants in the SU(2) sector [2]. In addition, it is shown that the dependence of the effective parameters and the pion-nucleon sigma term on the strange quark mass is relatively weak around its physical value, thus providing support to the assumption made in Ref. [2] that the SU(2) baryon chiral perturbation theory can be applied to study nf=2+1 lattice QCD simulations as long as the strange quark mass is close to its physical value.
KW - Baryon chiral perturbation theory
KW - Lattice QCD
KW - Nucleon mass and sigma term
UR - https://www.scopus.com/pages/publications/85010282281
U2 - 10.1016/j.physletb.2017.01.024
DO - 10.1016/j.physletb.2017.01.024
M3 - 文章
AN - SCOPUS:85010282281
SN - 0370-2693
VL - 766
SP - 325
EP - 333
JO - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
JF - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
ER -