The results of the N*→N transition magnetic moments in units of the nuclear magneton μN and of the radiative decay widths in units of keV. The mass MΘ+ = (1524 ± 5) MeV is used as an input.
| μNN* | |$\mu _{NN^*}^{(0)}$| | |$\mu _{NN^*}^{({\mathrm {op}})}$| | |$\mu _{NN^*}^{({\mathrm {wf}})}$| | |$\mu _{NN^*}^{({\mathrm {total}})}$| | ΓNN* (keV) |
| μpp* | 0 | 0.272 ± 0.051 | −0.125 ± 0.013 | 0.146 ± 0.053 | 17.7 ± 3.2 |
| μnn* | −0.252 ± 0.077 | −0.159 ± 0.042 | 0.107 ± 0.003 | −0.304 ± 0.089 | 77.1 ± 11.3 |
| μNN* | |$\mu _{NN^*}^{(0)}$| | |$\mu _{NN^*}^{({\mathrm {op}})}$| | |$\mu _{NN^*}^{({\mathrm {wf}})}$| | |$\mu _{NN^*}^{({\mathrm {total}})}$| | ΓNN* (keV) |
| μpp* | 0 | 0.272 ± 0.051 | −0.125 ± 0.013 | 0.146 ± 0.053 | 17.7 ± 3.2 |
| μnn* | −0.252 ± 0.077 | −0.159 ± 0.042 | 0.107 ± 0.003 | −0.304 ± 0.089 | 77.1 ± 11.3 |
The results of the N*→N transition magnetic moments in units of the nuclear magneton μN and of the radiative decay widths in units of keV. The mass MΘ+ = (1524 ± 5) MeV is used as an input.
| μNN* | |$\mu _{NN^*}^{(0)}$| | |$\mu _{NN^*}^{({\mathrm {op}})}$| | |$\mu _{NN^*}^{({\mathrm {wf}})}$| | |$\mu _{NN^*}^{({\mathrm {total}})}$| | ΓNN* (keV) |
| μpp* | 0 | 0.272 ± 0.051 | −0.125 ± 0.013 | 0.146 ± 0.053 | 17.7 ± 3.2 |
| μnn* | −0.252 ± 0.077 | −0.159 ± 0.042 | 0.107 ± 0.003 | −0.304 ± 0.089 | 77.1 ± 11.3 |
| μNN* | |$\mu _{NN^*}^{(0)}$| | |$\mu _{NN^*}^{({\mathrm {op}})}$| | |$\mu _{NN^*}^{({\mathrm {wf}})}$| | |$\mu _{NN^*}^{({\mathrm {total}})}$| | ΓNN* (keV) |
| μpp* | 0 | 0.272 ± 0.051 | −0.125 ± 0.013 | 0.146 ± 0.053 | 17.7 ± 3.2 |
| μnn* | −0.252 ± 0.077 | −0.159 ± 0.042 | 0.107 ± 0.003 | −0.304 ± 0.089 | 77.1 ± 11.3 |
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