Neutron structure effects in the deuteron and one neutron halos

dc.creatorNowakowski, M.
dc.creatorKelkar, N. G.
dc.creatorMart, T.
dc.date2005-11-28
dc.date2006-08-29
dc.date.accessioned2026-07-07T10:46:48Z
dc.date.available2026-07-07T10:46:48Z
dc.descriptionAlthough the neutron (n) does not carry a total electric charge, its charge and magnetization distributions represented in momentum space by the electromagnetic form factors, $F_1^{(n)} (q^2)$ and $F_2^{(n)} (q^2)$, lead to an electromagnetic potential of the neutron. Using this fact, we calculate the electromagnetic corrections to the binding energy, $B_d$, of the deuteron and a one neutron halo nucleus (11Be), by evaluating the neutron-proton and the neutron-charged core (10Be) potential, respectively. The correction to $B_d$ (~9 keV) is comparable to that arising due to the inclusion of the $Δ$-isobar component in the deuteron wave function. In the case of the more loosely bound halo nucleus, 11Be, the correction is close to about 2 keV.
dc.descriptionLaTex, 22 pages, 3 figures
dc.identifierhttps://arxiv.org/abs/nucl-th/0511078
dc.identifierhttp://arxiv.org/abs/nucl-th/0511078
dc.identifierPhys.Rev.C74:024323,2006
dc.identifierdoi:10.1103/PhysRevC.74.024323
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/183360
dc.subjectNuclear Theory
dc.titleNeutron structure effects in the deuteron and one neutron halos
dc.typetext

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