Neutron-proton mass difference from gauge/gravity duality
arXiv:1803.05202 · doi:10.1103/PhysRevD.98.046004
Abstract
Using gauge/gravity duality as a tool, we compute the strong sector, isospin breaking induced contribution to the neutron-proton mass difference in the Witten-Sakai-Sugimoto model of large QCD with two non-degenerate light flavors. The mass difference, for which we provide an analytic expression, turns out to be positive and proportional to the down-up quark mass splitting, consistently with expectations and previous estimates based on effective QCD models. Extrapolating the model parameters to fit QCD hadronic observables, we find that the strong sector contribution to the nucleon mass splitting overcomes the electromagnetic contribution and is about of the average nucleon mass in the model, a result which approaches recent lattice QCD estimates. Our formula is extended to resonances and baryons. We thus use it to compute the strong sector contribution to baryons mass differences. Finally, we also provide details of how isospin breaking affects the holographic instanton solution describing the baryons.
Latex, 23 pages; v2 clarifications, comments and references added, version published on PRD
References in corpus (8)
- Ab initio calculation of the neutron-proton mass difference
- Holographic Duals of Long Open Strings
- Quark mass and condensate in HQCD
- Holographic QCD with Dynamical Flavors
- Quark Mass Deformation of Holographic Massless QCD
- Baryons and the Chern-Simons term in holographic QCD with three flavors
- Theta dependence in Holographic QCD
- Neutron electric dipole moment from gauge/string duality
Cited by in corpus (9)
- Isospin asymmetry in holographic baryonic matter
- Heavy Holographic QCD
- The Holographic QCD Axion
- Non-derivative Axionic Couplings to Nucleons at large and small N
- Duality family of scalar field
- Symmetry energy in holographic QCD
- A simple mass-splitting mechanism in the Skyrme model
- Towards a holographic quark-hadron continuity
- Mass and Isospin Breaking Effects in the Skyrme Model and in Holographic QCD