Proton radius puzzle in Hamiltonian dynamics
arXiv:1410.5798 · doi:10.1007/s00601-014-0919-y
Abstract
Relativistic lepton-proton bound-state eigenvalue equations for Hamiltonians derived from quantum field theory using second-order renormalization group procedure for effective particles, are reducible to two-body Schroedinger eigenvalue equations with the effective Coulomb potential that exhibits a tiny sensitivity to the characteristic momentum-scale of the bound system. The scale dependence is shown to be relevant to the theoretical interpretation of precisely measured lepton-proton bound-state energy levels in terms of a 4 percent difference between the proton radii in muon-proton and electron-proton bound states.
arXiv comment7 pages, latex, FBS style
References in corpus (13)
- CODATA Recommended Values of the Fundamental Physical Constants: 2010
- Complete Tenth-Order QED Contribution to the Muon g-2
- High-precision determination of the electric and magnetic form factors of the proton
- Muonic hydrogen and the proton radius puzzle
- Nonperturbative Light-Front QCD
- Dispersion analysis of the nucleon form factors including meson continua
- Proton structure effects in muonic hydrogen
- Higher-order effective Hamiltonian for light atomic systems
- Sixth-Order Vacuum-Polarization Contribution to the Lamb Shift of the Muonic Hydrogen
- Harmonic oscillator force between heavy quarks
- The Lamb Shift in a Light Front Hamiltonian Approach
- Boost-Invariant Running Couplings in Effective Hamiltonians
- Calculation of size for bound-state constituents