






The energy spectrum of 153Gd radionuclide_18 In these data, the energy values were rounded to two decimal places
| Energy (keV) | Prevalence (%) |
|---|---|
| 5.18 | 0.374 |
| 5.82 | 0.976 |
| 5.82 | 0.1341 |
| 5.85 | 8.86 |
| 6.44 | 0.559 |
| 6.46 | 5.64 |
| 6.57 | 0.9214 |
| 6.62 | 0.0845 |
| 6.84 | 1.8512 |
| 7.48 | 0.947 |
| 7.77 | 0.173 |
| 7.79 | 0.244 |
| 14.06 | 0.0183 |
| 21.20 | 0.0224 |
| 40.47 | 0.00953 |
| 40.90 | 35.29 |
| 41.54 | 63.516 |
| 46.90 | 6.2516 |
| 47.04 | 12.13 |
| 47.37 | 0.1848 |
| 48.25 | 4.001 |
| 48.39 | 1.597 |
| 54.19 | 40.01622 |
| 69.67 | 2.41923 |
| 75.42 | 0.078323 |
| 83.37 | 0.1964 |
| 89.49 | 0.0694 |
| 96.88 | 0.0022 |
| 97.43 | 29 |
| 103.18 | 21.1123 |
| 118.11 | 0.000121 |
| 166.56 | 0.00033 |
| 172.30 | 0.00022 |
| 172.85 | 0.036017 |
Radial dose function values for the non-shield and shield modes_ The shield mode is related to the Pt and Al window sides
| g(r) | |||
|---|---|---|---|
| r(cm) | Without shield | With shield | |
| Pt shield side | Al window side | ||
| 0.5 | 0.90 | 0.52 | 0.93 |
| 1 | 1.00 | 1.00 | 1.00 |
| 1.5 | 1.06 | 1.39 | 1.04 |
| 2 | 1.11 | 1.73 1.04 | |
| 2.5 | 1.13 | 2.03 | 1.07 |
| 3 | 1.18 | 2.22 | 1.07 |
| 3.5 | 1.14 | 2.44 | 1.07 |
| 4 | 1.19 | 2.72 | 1.05 |
| 5 | 1.17 | 2.65 | 1.02 |
| 8 | 1.01 | 3.01 | 0.91 |
| 10 | 0.89 | 2.63 | 0.80 |
| 12 | 0.77 | 2.44 | 0.71 |
Anisotropy function values for the 153Gd source at different distances for the shielded mode at the Pt and Al windows sides
| r(cm) | ||||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| θ(degree) | Pt shield side | Al window side | ||||||||||||
| 0.5 | 1 | 2 | 3 | 5 | 10 | 12 | 0.5 | 1 | 2 | 3 | 5 | 10 | 12 | |
| 0 | 0.42 | 0.39 | 0.30 | - | - | - | - | 1.80 | 1.78 | 1.56 | - | - | - | - |
| 10 | 0.51 | 0.52 | 0.42 | 0.35 | 0.31 | 0.29 | 0.76 | 1.54 | 1.57 | 1.38 | 1.32 | 1.22 | 0.35 | - |
| 20 | 0.62 | 0.61 | 0.58 | 0.51 | 0.50 | 0.55 | 0.81 | 1.41 | 1.36 | 1.23 | 1.21 | 1.12 | 0.88 | 0.38 |
| 30 | 0.72 | 0.71 | 0.72 | 0.66 | 0.66 | 0.70 | 0.85 | 1.24 | 1.31 | 1.18 | 1.17 | 1.10 | 0.87 | 0.56 |
| 40 | 0.81 | 0.81 | 0.79 | 0.77 | 0.78 | 0.81 | 0.90 | 1.15 | 1.23 | 1.14 | 1.07 | 1.07 | 1.05 | 0.77 |
| 50 | 0.88 | 0.88 | 0.87 | 0.86 | 0.87 | 0.90 | 0.93 | 1.09 | 1.14 | 1.07 | 1.08 | 0.98 | 0.86 | 0.84 |
| 60 | 0.93 | 0.91 | 0.95 | 0.92 | 0.94 | 0.97 | 0.96 | 1.05 | 1.07 | 0.98 | 1.06 | 1.05 | 0.91 | 0.94 |
| 70 | 0.98 | 0.96 | 0.99 | 0.97 | 0.98 | 1.01 | 0.98 | 1.02 | 1.07 | 0.91 | 1.04 | 0.99 | 1.03 | 1.00 |
| 80 | 0.99 | 0.99 | 1.00 | 1.00 | 1.00 | 1.06 | 0.99 | 1.02 | 1.01 | 0.98 | 0.99 | 0.96 | 1.00 | 1.00 |
| 90 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 |
| 100 | 0.98 | 0.99 | 1.00 | 0.98 | 1.00 | 1.02 | 1.00 | 0.96 | 1.01 | 1.01 | 1.04 | 0.99 | 1.03 | 1.00 |
| 110 | 0.96 | 0.97 | 0.98 | 0.97 | 0.99 | 0.97 | 0.98 | 0.96 | 1.07 | 0.96 | 1.01 | 1.04 | 0.99 | 0.95 |
| 120 | 0.93 | 0.93 | 0.95 | 0.92 | 0.94 | 0.96 | 0.97 | 1.08 | 1.09 | 1.02 | 1.07 | 1.01 | 1.08 | 0.82 |
| 130 | 0.88 | 0.89 | 0.90 | 0.88 | 0.88 | 0.93 | 0.93 | 1.13 | 1.24 | 1.03 | 1.07 | 1.09 | 0.95 | 0.84 |
| 140 | 0.82 | 0.83 | 0.81 | 0.77 | 0.78 | 0.84 | 0.89 | 1.18 | 1.21 | 1.14 | 1.12 | 1.07 | 1.04 | 0.74 |
| 150 | 0.73 | 0.70 | 0.69 | 0.67 | 0.66 | 0.71 | 0.86 | 1.27 | 1.29 | 1.16 | 1.15 | 1.13 | 0.87 | 0.63 |
| 160 | 0.63 | 0.62 | 0.56 | 0.52 | 0.50 | 0.54 | 0.81 | 1.45 | 1.53 | 1.23 | 1.33 | 1.21 | 0.89 | 0.37 |
| 170 | 0.53 | 0.49 | 0.43 | 0.36 | 0.33 | 0.30 | 0.75 | 1.59 | 1.57 | 1.47 | 1.51 | 1.38 | 1.06 | - |
| 180 | 0.43 | 0.41 | - | - | - | - | - | 1.83 | 1.89 | - | - | - | - | - |
Anisotropy function values for the 153Gd source at different distances for the non-shielded mode
| θ(degrees) | r(cm) | |||||
|---|---|---|---|---|---|---|
| 0.5 | 1 | 2 | 3 | 5 | 10 | |
| 0 | 0.71 | 0.59 | 0.48 | 0.41 | 0.29 | - |
| 10 | 0.75 | 0.63 | 0.58 | 0.51 | 0.44 | 0.75 |
| 20 | 0.82 | 0.76 | 0.69 | 0.64 | 0.63 | 0.81 |
| 30 | 0.86 | 0.83 | 0.77 | 0.75 | 0.76 | 0.86 |
| 40 | 0.90 | 0.85 | 0.85 | 0.84 | 0.87 | 0.91 |
| 50 | 0.95 | 0.91 | 0.90 | 0.90 | 0.93 | 0.94 |
| 60 | 0.95 | 0.98 | 0.94 | 0.94 | 0.96 | 0.96 |
| 70 | 1.00 | 0.96 | 0.97 | 0.98 | 0.98 | 0.97 |
| 80 | 0.99 | 0.99 | 0.97 | 0.98 | 1.01 | 1.00 |
| 90 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 | 1.00 |
| 100 | 0.97 | 0.97 | 0.99 | 1.00 | 1.01 | 1.00 |
| 110 | 1.01 | 0.95 | 0.97 | 0.97 | 0.96 | 0.97 |
| 120 | 0.97 | 0.95 | 0.92 | 0.94 | 0.96 | 0.97 |
| 130 | 0.95 | 0.93 | 0.89 | 0.90 | 0.93 | 0.94 |
| 140 | 0.92 | 0.87 | 0.85 | 0.84 | 0.87 | 0.90 |
| 150 | 0.88 | 0.80 | 0.78 | 0.76 | 0.79 | 0.87 |
| 160 | 0.83 | 0.74 | 0.68 | 0.65 | 0.63 | 0.81 |
| 170 | 0.76 | 0.65 | 0.56 | 0.50 | 0.45 | 0.75 |
| 180 | 0.69 | - | - | - | - | - |
Mass attenuation coefficient (rμ/ρ) of Pt, Al and Ti in the 40 keV-100 keV energy range21
| Energy (keV) | Pt | Al | Ti |
|---|---|---|---|
| 40 | 12.45 | 0.57 | 2.21 |
| 50 | 6.95 | 0.37 | 1.21 |
| 60 | 4.34 | 0.28 | 0.77 |
| 80 | 8.73 | 0.20 | 0.41 |
| 100 | 4.99 | 0.17 | 0.27 |