Two-proton radioactivity of exotic nuclei beyond proton drip-line
Yanzhao Wang(王艳召),Jianpo Cui(崔建坡),Yonghao Gao(高永浩),Jianzhong Gu(顾建中)
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.
NucleiQ2p (MeV)log${}_{10}{T}_{1/2}^{\mathrm{cal}.}$ (s)
WS4FRDMKTUYHFB29WS4FRDMKTUYHFB29
${}_{18}^{30}$Ar1.22−10.65
${}_{18}^{31}$Ar1.080.43−9.541.14
${}_{20}^{34}$Ca0.750.96−3.65−6.53
${}_{22}^{38}$Ti1.411.56−8.60−9.59
${}_{22}^{39}$Ti0.98−4.62
${}_{24}^{41}$Cr2.122.13−11.10−11.10
${}_{24}^{42}$Cr1.401.11−6.95−4.21
${}_{28}^{49}$Ni1.131.651.88−0.75−5.80−7.33
${}_{30}^{55}$Zn1.49−3.05
${}_{32}^{58}$Ge2.682.572.451.77−9.80−9.34−8.80−4.76
${}_{32}^{59}$Ge1.431.85−1.73−5.36
${}_{34}^{62}$Se3.642.933.273.04−12.00−9.75−10.90−10.20
${}_{34}^{63}$Se2.391.371.781.80−7.380.57−3.45−3.61
${}_{36}^{65}$Kr2.833.11−8.34−9.45
${}_{36}^{66}$Kr2.65−7.54
${}_{36}^{68}$Kr1.80−2.23
${}_{38}^{70}$Sr3.152.803.38−8.64−7.18−9.47
${}_{38}^{71}$Sr2.921.832.15−7.72−1.10−3.56
${}_{38}^{72}$Sr1.650.59
${}_{40}^{74}$Zr3.272.653.51−8.16−5.39−9.02
${}_{40}^{75}$Zr2.801.932.51−6.15−0.60−4.63
${}_{40}^{76}$Zr1.850.10
${}_{40}^{77}$Zr1.86−0.06
${}_{42}^{78}$Mo3.073.68−6.08−8.42
${}_{42}^{79}$Mo3.072.19−6.09−1.07
${}_{42}^{80}$Mo2.341.91−2.131.21
${}_{44}^{81}$Ru4.78−10.70
${}_{44}^{82}$Ru3.69−7.60
${}_{44}^{83}$Ru3.202.832.33−5.69−3.92−0.88
${}_{44}^{84}$Ru2.202.680.08−3.11
${}_{46}^{85}$Pd4.47−9.11
${}_{46}^{86}$Pd3.833.343.59−7.23−5.35−6.36
${}_{46}^{87}$Pd3.042.62−3.98−1.66
${}_{48}^{88}$Cd5.59−11.10
${}_{48}^{89}$Cd4.54−8.55
${}_{48}^{90}$Cd3.903.393.77−6.65−4.64−6.18
${}_{48}^{91}$Cd3.082.94−3.19−2.46
${}_{48}^{94}$Cd0.340.00
${}_{50}^{94}$Sn3.34−3.39
${}_{50}^{95}$Sn2.481.53
${}_{50}^{96}$Sn2.670.20
${}_{52}^{101}$Te5.45−9.54
${}_{54}^{107}$Xe3.08−0.24
${}_{56}^{111}$Ba3.46−2.28
${}_{58}^{114}$Ce4.94−7.12
${}_{58}^{116}$Ce3.22−0.01