6533b82afe1ef96bd128c329

RESEARCH PRODUCT

Electromagnetic structure of few-nucleon ground states

Franz GrossFranz GrossMichele VivianiLaura Elisa MarcucciIngo SickAlfred StadlerAlfred StadlerRocco SchiavillaRocco SchiavillaM. PiarulliM. PiarulliM. T. PeñaJ. W. Van OrdenJ. W. Van Orden

subject

QuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryDegrees of freedom (physics and chemistry)FOS: Physical sciencescharge and magnetic radiiElectromagnetic properties01 natural sciences7. Clean energychiral effective field theoryNuclear Theory (nucl-th)Momentum0103 physical sciencesEffective field theoryCovariant transformationNuclear Experiment (nucl-ex)010306 general physicsform factorsNuclear ExperimentIsotopes of heliumPhysics010308 nuclear & particles physicselectric quadrupole and magnetic dipole momentslight nucleiGluoncharge and magnetic radii; chiral effective field theory; covariant spectator theory; electric quadrupole and magnetic dipole moments; form factors; light nuclei; Nuclear and High Energy Physicscovariant spectator theoryFew-nucleon ground statesNucleon

description

Experimental form factors of the hydrogen and helium isotopes, extracted from an up-to-date global analysis of cross sections and polarization observables measured in elastic electron scattering from these systems, are compared to predictions obtained in three different theoretical approaches: the first is based on realistic interactions and currents, including relativistic corrections (labeled as the conventional approach); the second relies on a chiral effective field theory description of the strong and electromagnetic interactions in nuclei (labeled $\chi$EFT); the third utilizes a fully relativistic treatment of nuclear dynamics as implemented in the covariant spectator theory (labeled CST). For momentum transfers below $Q \lesssim 5$ fm$^{-1}$ there is satisfactory agreement between experimental data and theoretical results in all three approaches. However, at $Q \gtrsim 5$ fm$^{-1}$, particularly in the case of the deuteron, a relativistic treatment of the dynamics, as is done in the CST, is necessary. The experimental data on the deuteron $A$ structure function extend to $Q \simeq 12$ fm$^{-1}$, and the close agreement between these data and the CST results suggests that, even in this extreme kinematical regime, there is no evidence for new effects coming from quark and gluon degrees of freedom at short distances.

https://doi.org/10.1088/0954-3899/43/2/023002