Baryons as relativistic three-quark bound states
G Eichmann, H Sanchis-Alepuz, R Williams… - Progress in Particle and …, 2016 - Elsevier
We review the spectrum and electromagnetic properties of baryons described as relativistic
three-quark bound states within QCD. The composite nature of baryons results in a rich …
three-quark bound states within QCD. The composite nature of baryons results in a rich …
Chiral representation of the scattering amplitude and the pion-nucleon sigma term
JM Alarcón, JM Camalich, JA Oller - Physical Review D—Particles, Fields …, 2012 - APS
We present a novel analysis of the π N scattering amplitude in Lorentz covariant baryon
chiral perturbation theory renormalized in the extended-on-mass-shell scheme. This …
chiral perturbation theory renormalized in the extended-on-mass-shell scheme. This …
Cross-channel constraints on resonant antikaon-nucleon scattering
Chiral perturbation theory and its unitarized versions have played an important role in our
understanding of the low-energy strong interaction. Yet, so far, such studies typically deal …
understanding of the low-energy strong interaction. Yet, so far, such studies typically deal …
Recent development in SU(3) covariant baryon chiral perturbation theory
LS Geng - Frontiers of Physics, 2013 - Springer
Baryon chiral perturbation theory (BChPT), as an effective field theory of low-energy
quantum chromodynamics (QCD), has played and is still playing an important role in our …
quantum chromodynamics (QCD), has played and is still playing an important role in our …
[HTML][HTML] The strangeness content of the nucleon from effective field theory and phenomenology
We revisit the classical relation between the strangeness content of the nucleon, the pion–
nucleon sigma term and the SU (3) F breaking of the baryon masses in the context of …
nucleon sigma term and the SU (3) F breaking of the baryon masses in the context of …
Measurements of Σ+ and Σ− time-like electromagnetic form factors for center-of-mass energies from 2.3864 to 3.0200 GeV
M Ablikim, MN Achasov, P Adlarson, S Ahmed… - Physics Letters B, 2021 - Elsevier
The Born cross sections of the e+ e−→ Σ+ Σ¯− and e+ e−→ Σ− Σ¯+ processes are
determined for center-of-mass energy from 2.3864 to 3.0200 GeV with the BESIII detector …
determined for center-of-mass energy from 2.3864 to 3.0200 GeV with the BESIII detector …
Strange physics of dark baryons
Dark sector particles at the GeV scale carrying baryon number provide an attractive
framework for understanding the origin of dark matter and the matter-antimatter asymmetry …
framework for understanding the origin of dark matter and the matter-antimatter asymmetry …
Accurate relativistic chiral nucleon-nucleon interaction up to next-to-next-to-leading order
We construct a relativistic chiral nucleon-nucleon interaction up to the next-to-next-to-
leading order in covariant baryon chiral perturbation theory. We show that a good …
leading order in covariant baryon chiral perturbation theory. We show that a good …
Improved description of the πN-scattering phenomenology at low energies in covariant baryon chiral perturbation theory
JM Alarcón, JM Camalich, JA Oller - Annals of Physics, 2013 - Elsevier
We present a novel analysis of the π N scattering amplitude in covariant baryon chiral
perturbation theory up to O (p 3) within the extended-on-mass-shell renormalization scheme …
perturbation theory up to O (p 3) within the extended-on-mass-shell renormalization scheme …
Measurement of the e+ e−→ Σ0Σ¯ 0 cross sections at center-of-mass energies from 2.3864 to 3.0200 GeV
M Ablikim, MN Achasov, P Adlarson, S Ahmed… - Physics Letters B, 2022 - Elsevier
The Born cross sections of e+ e−→ Σ 0 Σ¯ 0 are measured at center-of-mass energies from
2.3864 to 3.0200 GeV using data samples with an integrated luminosity of 328.5 pb− 1 …
2.3864 to 3.0200 GeV using data samples with an integrated luminosity of 328.5 pb− 1 …