Coexistence and fluctuations phenomena with Davidson-like potentials in quadrupole–octupole deformed nuclei

M M Hammad,W H Mansour,E M El-Maghraby,H A Motaweh,Ayman A Aly

Table 4. The same as in table 1, but for 220Rn [48] and 220Th [48].

220Rn 220Th ${L}^{+}$ ${{\epsilon }}_{i}^{\exp }$ ${{\epsilon }}_{i}^{Q}$ ${{\epsilon }}_{i}^{W}$ ${{\epsilon }}_{i}^{{\rm{\Lambda }}}$ ${{\epsilon }}_{i}^{\exp }$ ${{\epsilon }}_{i}^{Q}$ ${{\epsilon }}_{i}^{W}$ ${{\epsilon }}_{i}^{{\rm{\Lambda }}}$ Yrast ${0}^{+}$ 0 0 0 0 0 0 0 0 ${2}^{+}$ 1 1 1 1 1 1 1 1 ${4}^{+}$ 2.214 52 2.413 83 2.201 39 2.416 71 2.652 01 2.390 34 2.204 27 2.372 51 ${6}^{+}$ (3.626 14) (3.926 53) (3.553 91) (3.931 76) 4.069 81 3.870 33 3.559 24 3.826 03 ${8}^{+}$ (5.163 07) (5.471 61) (5.029 76) (5.479 37) 5.578 36 5.378 80 5.037 17 5.305 25 ${10}^{+}$ (6.768 05) (7.030 76) (6.611 25) (7.041 51) 7.025 13 6.899 77 6.620 47 6.796 08 ${12}^{+}$ (8.439 42) (8.597 60) (8.285 93) (8.611 64) 8.523 21 8.427 56 8.296 74 8.293 19 ${14}^{+}$ (10.1772) (10.1690) (10.0445) (10.1867) 10.0698 9.959 36 10.0567 9.794 08 ${16}^{+}$ (11.9793) (11.7433) (11.8796) (11.7653) 11.7850 11.4937 11.8931 11.2975 ${18}^{+}$ (13.7979) (13.3196) (13.7854) (13.3468) 13.4977 13.0297 13.8001 12.8031 ${20}^{+}$ (15.6178) (14.8973) (15.7571) (14.9314) 15.0771 14.5670 15.7729 14.3106 Yrast ${1}^{-}$ 2.669 71 0.397 09 0.470 03 0.397 02 ${3}^{-}$ 2.751 04 1.686 46 1.579 42 1.687 77 ${5}^{-}$ (3.534 85) (3.163 84) (2.860 83) (3.167 98) 3.468 76 3.124 75 2.864 98 3.094 33 ${7}^{-}$ (4.681 33) (4.696 66) (4.277 69) (4.703 08) 4.638 74 4.622 44 4.284 09 4.563 66 ${9}^{-}$ (6.066 80) (6.249 93) (5.808 17) (6.259 15) 5.999 65 6.138 18 5.816 51 6.049 64 ${11}^{-}$ (7.609 96) (7.813 46) (7.437 58) (7.825 82) 7.535 43 7.663 04 7.447 62 7.544 05 ${13}^{-}$ (9.241 08) (9.382 87) (9.155 21) (9.398 68) 8.918 67 9.193 08 9.166 75 9.043 25 ${15}^{-}$ (10.9473) (10.9559) (10.9529) (10.9756) 10.4880 10.7263 10.9658 10.5455 ${17}^{-}$ (12.7328) (12.5312) (12.8240) (12.5557) 12.1019 12.2615 12.8381 12.0501 ${19}^{-}$ (14.5635) (14.1083) (14.7633) (14.1387) 13.8000 13.7983 14.7785 13.5566 ${21}^{-}$ (16.4378) (15.6865) (16.7663) (15.7250) $2{B}_{2}/{\hslash }^{2}$ 1.000 00 15.0000 1.000 00 1.100 00 14.0000 1.200 00 Δ 0.630 22 0.556 52 0.627 32 0.444 85 0.620 04 0.498 08