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Proton radioactivity within the generalized liquid drop model with various versions of proximity potentials
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Yu-Qi Xin,Jun-Gang Deng,Hong-Fei Zhang
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Table 2. The logarithmic values of the proton radioactive half-lives derived when the proximity potential Prox.77-13 is applied to the GLDM, together with the corresponding results when the original version of the proximity potential is used. Elements with upper prefixes 'm'and 'n'represent the order of the excited isomeric states. '()'denotes the spin and/or parity is indeterminate. '#'means these values are estimated from the tendency of neighboring nuclides having the same Z and N parities. The experimental half-lives, spin/parity, and the proton radioactivity energies of the spherical proton emitters are taken from the NUBASE2016 [49]. All proton radioactivity half-lives and energies are in units of 's'and 'MeV’.
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Proton | Daughter | ${j}_{p}^{\pi }$ | ${j}_{d}^{\pi }$ | Qp | ${l}_{\min }$ | ${\mathrm{log}}_{10}{T}_{1/2}^{\exp }$ | ${\mathrm{log}}_{10}{T}_{1/2}^{77-13}$ | ${\mathrm{log}}_{10}{T}_{1/2}^{\mathrm{Ori}}$ | 145Tm | 144Er | (11/2−) | 0+ | 1.741 | 5 | −5.498 94 | −6.024 20 | −6.088 03 | 146Tm | 145Er | (1+) | 1/2+# | 0.891 | 0 | −0.809 67 | −0.744 90 | −0.833 77 | 146mTm | 145Er | (5−) | 1/2+# | l.201 | 5 | −1.124 94 | −1.365 37 | −1.429 20 | 147Tm | 146Er | 11/2− | 0+ | 1.059 | 5 | 0.572 87 | 0.406 40 | 0.341 77 | 147mTm | 146Er | 3/2+ | 0+ | 1.120 | 2 | −3.443 70 | −3.322 00 | −3.405 65 | 150mLu | 149Yb | (1+, 2+) | (1/2+) | 1.291 | 2 | −4.397 94 | −4.683 97 | −4.762 38 | 151mLu | 150Yb | (3/2+) | 0+ | 1.291 | 2 | −4.782 52 | −4.693 05 | −4.772 86 | 155Ta | 154Hf | (11/2−) | 0+ | 1.451 | 5 | −2.494 85 | −2.930 10 | −2.989 59 | 156Ta | 155Hf | (2−) | 7/2−# | 1.021 | 2 | −0.826 81 | −0.726 51 | −0.802 13 | 156mTa | 155Hf | (9+) | 7/2−# | 1.111 | 5 | 0.923 76 | 0.830 10 | 0.770 23 | 157Ta | 156Hf | 1/2+ | 0+ | 0.941 | 0 | −0.528 71 | −0.211 58 | −0.294 78 | 160Re | 159W | (4−) | 7/2−# | 1.271 | 0 | −3.163 68 | −4.121 50 | −4.199 74 | 161Re | 160W | 1/2+ | 0+ | 1.201 | 0 | −3.356 55 | −3.310 40 | −3.389 68 | 161mRe | 160W | 11/2− | 0+ | 1.321 | 5 | −0.679 85 | −1.174 20 | −1.232 43 | 165mIr | 164Os | (11/2−) | 0+ | 1.721 | 5 | −3.429 46 | −4.294 27 | −4.350 21 | 166Ir | 165Os | (2−) | (7/2−) | 1.161 | 2 | −0.841 64 | −1.484 46 | −1.554 32 | 166mIr | 165Os | (9+) | (7/2−) | 1.331 | 5 | −0.090 44 | −0.792 18 | −0.848 35 | 167Ir | 166Os | 1/2+ | 0+ | 1.071 | 0 | −1.127 84 | −0.965 68 | −1.042 01 | 167mIr | 166Os | 11/2− | 0+ | 1.246 | 5 | 0.778 15 | 0.175 67 | 0.118 72 | 170Au | 169Pt | (2−) | (7/2−) | 1.471 | 2 | −3.488 12 | −4.386 11 | −4.452 73 | 170mAu | 169Pt | (9+) | (7/2−) | 1.751 | 5 | −2.974 69 | −4.109 69 | −4.163 58 | 171Au | 170Pt | (1/2+) | 0+ | 1.448 | 0 | −4.651 70 | −4.879 26 | −4.952 22 | 171mAu | 170Pt | 11/2− | 0+ | 1.702 | 5 | −2.586 70 | −3.740 66 | −3.795 34 | 176Tl | 175Hg | (3−, 4−, 5−) | (7/2−) | 1.261 | 0 | −2.207 61 | −2.306 56 | −2.375 19 | 177Tl | 176Hg | (1/2+) | 0+ | 1.155 | 0 | −1.178 49 | −0.929 37 | −0.998 74 | 177mTl | 176Hg | (11/2−) | 0+ | 1.962 | 5 | −3.459 67 | −5.190 03 | −5.246 75 | 185mBi | 184Pb | 1/2+ | 0+ | 1.607 | 0 | −4.191 79 | −5.352 62 | −5.423 39 |
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