Weak capture of protons by protons
| dc.creator | Schiavilla, R. | |
| dc.creator | Stoks, V. G. J. | |
| dc.creator | Gloeckle, W. | |
| dc.creator | Kamada, H. | |
| dc.creator | Nogga, A. | |
| dc.creator | Carlson, J. | |
| dc.creator | Machleidt, R. | |
| dc.creator | Pandharipande, V. R. | |
| dc.creator | Wiringa, R. B. | |
| dc.creator | Kievsky, A. | |
| dc.creator | Rosati, S. | |
| dc.creator | Viviani, M. | |
| dc.date | 1998-08-06 | |
| dc.date.accessioned | 2026-07-07T11:36:41Z | |
| dc.date.available | 2026-07-07T11:36:41Z | |
| dc.description | The cross section for the proton weak capture reaction $^1H(p,e^+ν_e)^2H$ is calculated with wave functions obtained from a number of modern, realistic high-precision interactions. To minimize the uncertainty in the axial two-body current operator, its matrix element has been adjusted to reproduce the measured Gamow-Teller matrix element of tritium $β$ decay in model calculations using trinucleon wave functions from these interactions. A thorough analysis of the ambiguities that this procedure introduces in evaluating the two-body current contribution to the pp capture is given. Its inherent model dependence is in fact found to be very weak. The overlap integral $Λ^2(E=0)$ for the pp capture is predicted to be in the range 7.05--7.06, including the axial two-body current contribution, for all interactions considered. | |
| dc.description | 17 pages RevTeX (twocolumn), 5 postscript figures | |
| dc.identifier | https://arxiv.org/abs/nucl-th/9808010 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/9808010 | |
| dc.identifier | Phys.Rev.C58:1263,1998 | |
| dc.identifier | doi:10.1103/PhysRevC.58.1263 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/199001 | |
| dc.subject | Nuclear Theory | |
| dc.title | Weak capture of protons by protons | |
| dc.type | text |