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
${}_{18}^{30}$Ar—1.22———−10.65——
${}_{18}^{31}$Ar1.08——0.43−9.54——1.14
${}_{20}^{34}$Ca—0.750.96——−3.65−6.53—
${}_{22}^{38}$Ti—1.411.56——−8.60−9.59—
${}_{22}^{39}$Ti0.98———−4.62———
${}_{24}^{41}$Cr—2.122.13——−11.10−11.10—
${}_{24}^{42}$Cr1.401.11——−6.95−4.21——
${}_{28}^{49}$Ni1.131.65—1.88−0.75−5.80—−7.33
${}_{30}^{55}$Zn—1.49———−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
${}_{36}^{65}$Kr——2.833.11——−8.34−9.45
${}_{36}^{66}$Kr—2.65———−7.54——
${}_{36}^{68}$Kr1.80———−2.23———
${}_{38}^{70}$Sr—3.152.803.38—−8.64−7.18−9.47
${}_{38}^{71}$Sr2.921.83—2.15−7.72−1.10—−3.56
${}_{38}^{72}$Sr1.65———0.59———
${}_{40}^{74}$Zr—3.272.653.51—−8.16−5.39−9.02
${}_{40}^{75}$Zr2.801.93—2.51−6.15−0.60—−4.63
${}_{40}^{76}$Zr1.85———0.10———
${}_{40}^{77}$Zr———1.86———−0.06
${}_{42}^{78}$Mo——3.073.68——−6.08−8.42
${}_{42}^{79}$Mo3.07—2.19—−6.09—−1.07—
${}_{42}^{80}$Mo2.341.91——−2.131.21——
${}_{44}^{81}$Ru———4.78———−10.70
${}_{44}^{82}$Ru———3.69———−7.60
${}_{44}^{83}$Ru3.202.83—2.33−5.69−3.92—−0.88
${}_{44}^{84}$Ru2.20——2.680.08——−3.11
${}_{46}^{85}$Pd———4.47———−9.11
${}_{46}^{86}$Pd3.83—3.343.59−7.23—−5.35−6.36
${}_{46}^{87}$Pd3.04——2.62−3.98——−1.66
${}_{48}^{88}$Cd———5.59———−11.10
${}_{48}^{89}$Cd———4.54———−8.55
${}_{48}^{90}$Cd3.90—3.393.77−6.65—−4.64−6.18
${}_{48}^{91}$Cd3.08——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—
${}_{50}^{96}$Sn2.67———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