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Two-proton radioactivity of exotic nuclei beyond proton drip-line
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Yanzhao Wang(王艳召),Jianpo Cui(崔建坡),Yonghao Gao(高永浩),Jianzhong Gu(顾建中)
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Table 2. Same as table 1, but for the predicted 2p radioactivity half-lives by inputting the Q2p values extracted from the WS4 [63], FRDM [64], KTUY [74] and HFB29 [67] nuclear mass models.
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Nuclei | Q2p (MeV) | log${}_{10}{T}_{1/2}^{\mathrm{cal}.}$ (s) |
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| WS4 | FRDM | KTUY | HFB29 | WS4 | FRDM | KTUY | HFB29 |
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${}_{18}^{30}$Ar | — | 1.22 | — | — | — | −10.65 | — | — | ${}_{18}^{31}$Ar | 1.08 | — | — | 0.43 | −9.54 | — | — | 1.14 | ${}_{20}^{34}$Ca | — | 0.75 | 0.96 | — | — | −3.65 | −6.53 | — | ${}_{22}^{38}$Ti | — | 1.41 | 1.56 | — | — | −8.60 | −9.59 | — | ${}_{22}^{39}$Ti | 0.98 | — | — | — | −4.62 | — | — | — | ${}_{24}^{41}$Cr | — | 2.12 | 2.13 | — | — | −11.10 | −11.10 | — | ${}_{24}^{42}$Cr | 1.40 | 1.11 | — | — | −6.95 | −4.21 | — | — | ${}_{28}^{49}$Ni | 1.13 | 1.65 | — | 1.88 | −0.75 | −5.80 | — | −7.33 | ${}_{30}^{55}$Zn | — | 1.49 | — | — | — | −3.05 | — | — | ${}_{32}^{58}$Ge | 2.68 | 2.57 | 2.45 | 1.77 | −9.80 | −9.34 | −8.80 | −4.76 | ${}_{32}^{59}$Ge | 1.43 | 1.85 | — | — | −1.73 | −5.36 | — | — | ${}_{34}^{62}$Se | 3.64 | 2.93 | 3.27 | 3.04 | −12.00 | −9.75 | −10.90 | −10.20 | ${}_{34}^{63}$Se | 2.39 | 1.37 | 1.78 | 1.80 | −7.38 | 0.57 | −3.45 | −3.61 | ${}_{36}^{65}$Kr | — | — | 2.83 | 3.11 | — | — | −8.34 | −9.45 | ${}_{36}^{66}$Kr | — | 2.65 | — | — | — | −7.54 | — | — | ${}_{36}^{68}$Kr | 1.80 | — | — | — | −2.23 | — | — | — | ${}_{38}^{70}$Sr | — | 3.15 | 2.80 | 3.38 | — | −8.64 | −7.18 | −9.47 | ${}_{38}^{71}$Sr | 2.92 | 1.83 | — | 2.15 | −7.72 | −1.10 | — | −3.56 | ${}_{38}^{72}$Sr | 1.65 | — | — | — | 0.59 | — | — | — | ${}_{40}^{74}$Zr | — | 3.27 | 2.65 | 3.51 | — | −8.16 | −5.39 | −9.02 | ${}_{40}^{75}$Zr | 2.80 | 1.93 | — | 2.51 | −6.15 | −0.60 | — | −4.63 | ${}_{40}^{76}$Zr | 1.85 | — | — | — | 0.10 | — | — | — | ${}_{40}^{77}$Zr | — | — | — | 1.86 | — | — | — | −0.06 | ${}_{42}^{78}$Mo | — | — | 3.07 | 3.68 | — | — | −6.08 | −8.42 | ${}_{42}^{79}$Mo | 3.07 | — | 2.19 | — | −6.09 | — | −1.07 | — | ${}_{42}^{80}$Mo | 2.34 | 1.91 | — | — | −2.13 | 1.21 | — | — | ${}_{44}^{81}$Ru | — | — | — | 4.78 | — | — | — | −10.70 | ${}_{44}^{82}$Ru | — | — | — | 3.69 | — | — | — | −7.60 | ${}_{44}^{83}$Ru | 3.20 | 2.83 | — | 2.33 | −5.69 | −3.92 | — | −0.88 | ${}_{44}^{84}$Ru | 2.20 | — | — | 2.68 | 0.08 | — | — | −3.11 | ${}_{46}^{85}$Pd | — | — | — | 4.47 | — | — | — | −9.11 | ${}_{46}^{86}$Pd | 3.83 | — | 3.34 | 3.59 | −7.23 | — | −5.35 | −6.36 | ${}_{46}^{87}$Pd | 3.04 | — | — | 2.62 | −3.98 | — | — | −1.66 | ${}_{48}^{88}$Cd | — | — | — | 5.59 | — | — | — | −11.10 | ${}_{48}^{89}$Cd | — | — | — | 4.54 | — | — | — | −8.55 | ${}_{48}^{90}$Cd | 3.90 | — | 3.39 | 3.77 | −6.65 | — | −4.64 | −6.18 | ${}_{48}^{91}$Cd | 3.08 | — | — | 2.94 | −3.19 | — | — | −2.46 | ${}_{48}^{94}$Cd | — | — | 0.34 | — | — | — | 0.00 | — | ${}_{50}^{94}$Sn | — | — | 3.34 | — | — | — | −3.39 | — | ${}_{50}^{95}$Sn | — | — | 2.48 | — | — | — | 1.53 | — | ${}_{50}^{96}$Sn | 2.67 | — | — | — | 0.20 | — | — | — | ${}_{52}^{101}$Te | — | — | — | 5.45 | — | — | — | −9.54 | ${}_{54}^{107}$Xe | — | — | — | 3.08 | — | — | — | −0.24 | ${}_{56}^{111}$Ba | — | — | — | 3.46 | — | — | — | −2.28 | ${}_{58}^{114}$Ce | — | — | — | 4.94 | — | — | — | −7.12 | ${}_{58}^{116}$Ce | — | — | — | 3.22 | — | — | — | −0.01 |
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