Relativistic Charge Form Factor of the Deuteron
| dc.creator | Afanasev, Andrei V. | |
| dc.creator | Afanasev, V. D. | |
| dc.creator | Trubnikov, S. V. | |
| dc.date | 1997-12-30 | |
| dc.date.accessioned | 2026-07-07T05:42:14Z | |
| dc.date.available | 2026-07-07T05:42:14Z | |
| dc.description | Relativistic integral representation in terms of experimental neutron-proton scattering phase shifts alone is used to compute the charge form factor of the deuteron $G_{Cd}(Q^2)$. The results of numerical calculations of $|G_{Cd}(Q^2)|$ are presented in the interval of the four-momentum transfers squared $0 \leq Q^2 \leq 35 fm^{-2}$. Zero and the prominent secondary maximum in $ |G_{Cd}(Q^2)|$ are the direct consequences of the change of sign in the experimental $^3S_1$- phase shifts. Till the point $Q^2 \simeq 20 fm^{-2}$ the total relativistic correction to $|G_{Cd}(Q^2)|$ is positive and reaches the maximal value of 25% at $Q^2 \simeq 14 fm^{-2}$. | |
| dc.description | 9 pages, LaTeX, 2 postscript figures, uses wor-sci.sty, epsf.sty | |
| dc.identifier | https://arxiv.org/abs/nucl-th/9712082 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/9712082 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/82857 | |
| dc.subject | Nuclear Theory | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Relativistic Charge Form Factor of the Deuteron | |
| dc.type | text |