Table I
Relative concentrations of the stable isotopes in the hafnium samples, in percent.
Hf sample |
---|
Isotope | Natural | 180 | 179 | 178 | 177 | 176 | 174 |
---|
180 | 35.44 | 93.27 | 44.20 | 3.96 | 3.68 | 1.01 | 12.86 |
179 | 13.78 | 2.54 | 53.32 | 5.95 | 4.53 | 2.35 | 7.14 |
178 | 27.08 | 2.97 | 1.81 | 84.79 | 31.73 | 10.71 | 21.72 |
177 | 18.39 | 0.87 | 0.68 | 4.38 | 59.08 | 26.46 | 28.87 |
176 | 5.15 | 0.36 | ⋯ | 0.92 | 0.99 | 59.45 | 19.28 |
174 | 0.18 | ⋯ | ⋯ | ⋯ | ⋯ | ⋯ | 10.14 |
Table II
Relative shifts between the even isotopes of hafnium.
Hafnium isotopes | Relative shift | No. of good determinations |
---|
180–178 | 100 | ⋯ |
178–176 | 82.6±3.5 | 20 |
176–174 | 87.6±3.7 | 21 |
Table III
Isotope shifts in the lines resulting from transitions from the odd states shown at the left to the even states shown above are given in mK. The wavelengths in A are shown directly above the shifts.
5d26s2 |
---|
5d26s6p | a3F2 | a3F3 | a3F4 | a1D2 | a3P1 | a3P0 |
---|
z5G30 | 5181 | 5902 | | | | |
| 28.9±1.2 | 30.3±1.1 | | | | |
z5G40 | | 5373 | 6098 | | | |
| | 35.5±0.3 | 36.8±0.4 | | | |
z5G50 | | | 5452 | | | |
| | | 40.9±1.8 | | | |
z5F20 | 4452 | 4975 | | | | |
| 37.8±0.1 | 38.4±1.1 | | | | |
z5F40 | | 4457 | | | | |
| | 43.8±1.4 | | | | |
z5F50 | | | 4620 | | | |
| | | 42.9±0.7 | | | |
z5D30 | | | 4598.9 | 4837 | | |
| | | 34.8±2.4 | 37.0±3.4 | | |
z3F30 | | | 4330 | | | |
| | | 42.5±2.6 | | | |
z3D20 | | | | 4417 | | |
| | | | 43.5±2.1 | | |
z3S10 | | | | 4461 | 4655 | 4438 |
| | | | 44.3±0.5 | 46.2±1.7 | 42.6±2.2 |
Table IV
Shifts in the levels of the odd configuration 5d26s6p relative to the 5d26s2 level.
State | Shift (mK) |
---|
z5G30 | 29.6±1.2 |
z5G40 | 36.2±0.4 |
z5G50 | 40.9±1.8 |
z5F20 | 38.1±0.6 |
z5F40 | 43.8±1.4 |
z5F50 | 42.9±0.7 |
z5D30 | 35.9±2.9 |
z3F30 | 42.5±2.6 |
z3D20 | 43.5±2.1 |
z3S10 | 44.4±1.5 |
Table V
Isotope shifts between the odd hafnium isotopes and their next heavier neighbors, in four lines, as determined from the positions of the hyperfine-structure components.
λ | 180–179 (mK) | 178–177 (mK) |
|
| 180–178 (mK) |
---|
4457 | 23.0±3.7 | 25.5±3 | 52.5±10.5 | 58.2±9.0 | 43.8±1.4 |
4620 | 33±4 | 35±1.5 | 77.0±10.7 | 81.6±5.0 | 42.9±0.7 |
4655 | 26±5 | 34±5 | 56.3±13.4 | 73.6±14.0 | 46.2±1.7 |
5452 | 22.5±3 | 30.8±1.3 | 56.0±9.6 | 76.6±6.0 | 40.2±1.3 |
Average | | | 60.5±8.3 | 72.5±7.2 | |
Table VI
Approximate shifts in the levels in HfI, in mK, as predicted from those in the levels in HfII.
State | Predicted displacement | Average |
---|
5d26s2 | (72) (1.6 )=115 | |
| (140) (0.77)=108 | 112 |
5d36s | (72) (0.77)=55 | 55 |
5d26s6p | (72) (0.92)=66 | |
| (86) (0.77)=66 | 66 |
5d6s26p | (140) (0.92)=129 | |
| (86) (1.6 )=138 | 134 |
Table VII
Differences between the squares of the intrinsic quadrupole moments in the various pairs of hafnium isotopes.
Isotopes | Δ(Q02) (Square barn) |
---|
180–178 | 0 to −8 |
178–176 | −2 to −9 |
176–174 | −1 to −9 |
178–177 | +9 to −6 |
180–179 | +6 to −8 |
179–177 | +4 to −8 |