Nuclide |
The even Z, even N nuclide studied
|
Transition Energy |
Energy of the first excited 2+ state in keV
|
Transition Rate Ratio |
B(↑) = (2J + 1)B(↓)/(2J0+1), where J0
and J are spins of the lower and upper levels, respectively.
|
B(E2; 0+ → 2+) |
Reduced electric quadrupole transition rate for the ground state to
2+ state transition in units of e2b2
|
W.U. |
Weisskopf units are based on single-particle estimate for the λ-th
multipole reduced electric transition probability and originally have been used for
transitions from higher to lower states:
Bw(Eλ)=(1/4π)(3/(λ+3))2(1.2)2λA2λ/3
e2fm2λ
|
|
Weisskopf (single-particle) B(E2) value for
0+→2+ transition is given by:
Bw(E2↑)=0.297xA4/3 e2fm4
|
τ |
Mean lifetime of the state in ps
τ = 40.81 x
1013E-5[B(E2↑)/e2b2]-1(1 +
α)-1
|
β |
Deformation parameter
β = (4π/3ZR02)[B(E2↑)/e2]1/2, where
R02 = (1.2 x 10-13 A1/3 cm)2 =
0.0144A2/3b
|
Q0 |
Intrinsic quadrupole moment in b Q0 =
[16πB(E2↑)/5e2]1/2
|
Reference |
Nuclear Science References Database Abstract
|
Global Best Fit |
Global Best Fit for B(E2)↑ by S. Raman, C.W. Nestor and P. Tikkanen
|
Modified Grodzins rule |
B(E2↑) =
(2.57±0.45)E-1Z2A-2/3
β = (466±41)E-1/2A-1
|
null |
No data available
|