Fission product yield
| Nuclide | t<templatestyles src="Fraction/styles.css" />1⁄2 | Yield | Q[a 1] | βγ |
|---|---|---|---|---|
| <templatestyles src="Nobold/styles.css"/>(Ma) | <templatestyles src="Nobold/styles.css"/>(%)[a 2] | <templatestyles src="Nobold/styles.css"/>(keV) | ||
| 99Tc | 0.211 | 6.1385 | 294 | β |
| 126Sn | 0.230 | 0.1084 | 4050[a 3] | βγ |
| 79Se | 0.327 | 0.0447 | 151 | β |
| 135Cs | 1.33Template:Fsp | 6.9110[a 4] | 269 | β |
| 93Zr | 1.61Template:Fsp | 5.4575 | 91 | βγ |
| 107Pd | 6.5Template:Fsp | 1.2499 | 33 | β |
| 129I | 16.14Template:Fsp | 0.8410 | 194 | βγ |
| <templatestyles src="Reflist/styles.css" /> | ||||
| t½ (year) |
Yield (<templatestyles src="Template:Tooltip/styles.css" />%Script error: No such module "Check for unknown parameters".) |
Q (keV) |
βγ | |
|---|---|---|---|---|
| 155Eu | Template:Fsp4.76 | <templatestyles src="Template:Tooltip/styles.css" />0.0803Script error: No such module "Check for unknown parameters".Template:Fsp | 252 | βγ |
| 85Kr | 10.76 | <templatestyles src="Template:Tooltip/styles.css" />0.2180Script error: No such module "Check for unknown parameters".Template:Fsp | 687 | βγ |
| 113mCd | 14.1Template:Fsp | <templatestyles src="Template:Tooltip/styles.css" />0.0008Script error: No such module "Check for unknown parameters".Template:Fsp | 316 | β |
| 90Sr | 28.9Template:Fsp | 4.505Template:Fsp | <templatestyles src="Template:Tooltip/styles.css" />2826Script error: No such module "Check for unknown parameters". | <templatestyles src="Template:Tooltip/styles.css" />βScript error: No such module "Check for unknown parameters". |
| 137Cs | 30.23 | 6.337Template:Fsp | <templatestyles src="Template:Tooltip/styles.css" />1176Script error: No such module "Check for unknown parameters". | β<templatestyles src="Template:Tooltip/styles.css" />γScript error: No such module "Check for unknown parameters". |
| 121mSn | 43.9Template:Fsp | 0.00005 | 390 | βγ |
| 151Sm | 94.6Template:Fsp | <templatestyles src="Template:Tooltip/styles.css" />0.5314Script error: No such module "Check for unknown parameters".Template:Fsp | 77 | β |
Nuclear fission splits a heavy nucleus such as uranium or plutonium into two lighter nuclei, which are called fission products. Yield refers to the fraction of a fission product produced per fission.
Yield can be broken down by:
- Individual isotope
- Chemical element spanning several isotopes of different mass number but same atomic number.
- Nuclei of a given mass number regardless of atomic number. Known as "chain yield" because it represents a decay chain of beta decay.
Isotope and element yields will change as the fission products undergo beta decay, while chain yields do not change after completion of neutron emission by a few neutron-rich initial fission products (delayed neutrons), with half-life measured in seconds.
A few isotopes can be produced directly by fission, but not by beta decay because the would-be precursor with atomic number one less is stable and does not decay (atomic number grows by 1 during beta decay). Chain yields do not account for these "shadowed" isotopes; however, they have very low yields (less than a millionth as much as common fission products) because they are far less neutron-rich than the original heavy nuclei.
Yield is usually stated as percentage per fission, so that the total yield percentages sum to 200%.Script error: No such module "Unsubst". Less often, it is stated as percentage of all fission product.Script error: No such module "Unsubst".
Definitions
There are several types of yields. For the most common fission reactions, the decay of the fission products preserve mass number. Thus the products form decay chains of constant mass. That makes the independent yield especially useful.[1]Template:Rp
The independent yield is a product of three factors, Y(A) the sum yield or mass yield, the fractional independent yield, and R(A,Z,I) the isomeric yield ratio:[1] Here possible product of fission can be represented by a triplet (A,Z,I), where A is the mass number, Z is the atomic number, and I is an integer for isomeric excited state, numbered from 0 for the ground state. For each decay chain (mass number A) the fractional independent yields and isomeric yield formulas sum to one: and the independent yields sum to the sum yield for each chain: The independent yield excludes delayed neutron emission. The cumulative yield,, c(A,Z,I), of a nuclide (A,Z,I) is the total number of atoms produced by one fission over all time. The chain yield, Ch(A), is the sum of all the cumulative yields for one mass chain for one fission. The independent, cumulative, and chain yields are given as percent per fission, that is as the yield of products per 100 fission reaction.[1]
Mass vs. yield curve
If a graph of the mass or mole yield of fission products against the atomic number of the fragments is drawn then it has two peaks, one in the area zirconium through to palladium and one at xenon through to neodymium. This is because the fission event causes the nucleus to split in an asymmetric manner,[2] as nuclei closer to magic numbers are more stable.[3]
Yield vs. Z - This is a typical distribution for the fission of uranium. Note that in the calculations used to make this graph the activation of fission products was ignored and the fission was assumed to occur in a single moment rather than a length of time. In this bar chart results are shown for different cooling times (time after fission).
Because of the stability of nuclei with even numbers of protons and/or neutrons the curve of yield against element is not a smooth curve. It tends to alternate.
In general, the higher the energy of the state that undergoes nuclear fission, the more likely a symmetric fission is, hence as the neutron energy increases and/or the energy of the fissile atom increases, the valley between the two peaks becomes more shallow; for instance, the curve of yield against mass for Pu-239 has a more shallow valley than that observed for U-235, when the neutrons are thermal neutrons. The curves for the fission of the later actinides tend to make even more shallow valleys. In extreme cases such as 259Fm, only one peak is seen.
Yield is usually expressed relative to number of fissioning nuclei, not the number of fission product nuclei, that is, yields should sum to 200%.
The table in the next section ("Ordered by yield") gives yields for notable radioactive (with half-lives greater than one year, plus iodine-131) fission products, and (the few most absorptive) neutron poison fission products, from thermal neutron fission of U-235 (typical of nuclear power reactors), computed from [1]Script error: No such module "Unsubst"..
The yields in the table sum to only 45.5522%, including 34.8401% which have half-lives greater than one year:
| t½ in years | Yield |
|---|---|
| 1 to 5 | 2.7252% |
| 10 to 100 | 12.5340% |
| 2 to 300,000 | 6.1251% |
| 1.5 to 16 million | 13.4494% |
The remainder and the unlisted 54.4478% decay with half-lives less than one year into nonradioactive nuclei.
This is before accounting for the effects of any subsequent neutron capture; e.g.:
- 135Xe capturing a neutron and becoming nearly stable 136Xe, rather than decaying to 135Cs which is radioactive with a half-life of 2.3 million years
- Nonradioactive 133Cs capturing a neutron and becoming 134Cs, which is radioactive with a half-life of 2 years
- Many of the fission products with mass 147 or greater such as 147Pm, 149Sm, 151Sm, and 155Eu have significant cross sections for neutron capture, so that one heavy fission product atom can undergo multiple successive neutron captures.
Besides fission products, the other types of radioactive products are
- plutonium containing 238Pu, 239Pu, 240Pu, 241Pu, and 242Pu,
- minor actinides including 237Np, 241Am, 243Am, curium isotopes, and perhaps californium
- reprocessed uranium containing 236U and other isotopes
- tritium
- activation products of neutron capture by the reactor or bomb structure or the environment
Fission products from U-235
| Yield | Element | Isotope | Halflife | Comment |
|---|---|---|---|---|
| 6.7896% | Caesium | Template:Hs 133Cs → 134Cs | Template:Ntsh 2.065 y | Neutron capture (29 barns) slowly converts stable 133Cs to 134Cs, which itself is low-yield because beta decay stops at 134Xe; can be further converted (140 barns) to 135Cs. |
| 6.3333% | Iodine, xenon | Template:Hs 135I → 135Xe | Template:Ntsh 6.57 h | Most important neutron poison; neutron capture converts 10–50% of 135Xe to 136Xe; remainder decays (9.14h) to 135Cs (2.3 My). |
| 6.2956% | Zirconium | Template:Hs 93Zr | Template:Ntsh 1.53 My | Long-lived fission product also produced by neutron activation in zircalloy cladding. |
| 6.1% | Molybdenum | Template:Hs 99Mo | Template:Ntsh 65.94 h | Its daughter nuclide 99mTc is important in medical diagnosing. |
| 6.0899% | Caesium | Template:Hs 137Cs | Template:Ntsh 30.17 y | Source of most of the decay heat from years to decades after irradiation, together with Template:Chem/link. |
| 6.0507% | Technetium | Template:Hs 99Tc | Template:Ntsh 211 ky | Candidate for disposal by nuclear transmutation. |
| 5.7518% | Strontium | Template:Hs 90Sr | Template:Ntsh 28.9 y | Source of much of the decay heat together with Template:Chem/link on the timespan of years to decades after irradiation. Formerly used in radioisotope thermoelectric generators. |
| 2.8336% | Iodine | Template:Hs 131I | Template:Ntsh 8.02 d | Reason for the use of potassium iodide tablets after nuclear accidents or nuclear bomb explosions. |
| 2.2713% | Promethium | Template:Hs 147Pm | Template:Ntsh 2.62 y | beta decays to very long lived Samarium-147 (half life>age of the universe); has seen some use in radioisotope thermoelectric generators |
| 1.0888% | Samarium | Template:Hs 149Sm | Template:Ntsh Observationally stable | 2nd most significant neutron poison. |
| 0.9%[4] | Iodine | Template:Hs 129I | Template:Ntsh 15.7 My | Long-lived fission product. Candidate for disposal by nuclear transmutation. |
| 0.4203% | Samarium | Template:Hs 151Sm | Template:Ntsh 90 y | Neutron poison; most will be converted to stable 152Sm. |
| 0.3912% | Ruthenium | Template:Hs 106Ru | Template:Ntsh 373.6 d | ruthenium tetroxide is volatile and chemically aggressive; daughter nuclide Template:Chem/link decays quickly to stable Template:Chem/link |
| 0.2717% | Krypton | Template:Hs 85Kr | Template:Ntsh 10.78 y | noble gas; has some uses in industry to detect fine cracks in materials via autoradiography |
| 0.1629% | Palladium | Template:Hs 107Pd | Template:Ntsh 6.5 My | Long-lived fission product; hampers extraction of stable isotopes of platinum group metals for use due to chemical similarity. |
| 0.0508% | Selenium | Template:Hs 79Se | Template:Ntsh 327 ky | |
| 0.0330% | Europium, gadolinium | Template:Hs 155Eu → 155Gd | Template:Ntsh 4.76 y | Both neutron poisons, most will be destroyed while fuel still in use. |
| 0.0297% | Antimony | Template:Hs 125Sb | Template:Ntsh 2.76 y | |
| 0.0236% | Tin | Template:Hs 126Sn | Template:Ntsh 230 ky | |
| 0.0065% | Gadolinium | Template:Hs 157Gd | Template:Ntsh stable | Neutron poison. |
| 0.0003% | Cadmium | Template:Hs 113mCd | Template:Ntsh 14.1 y | Neutron poison, most will be destroyed while fuel still in use. |
Cumulative fission yields
Cumulative fission yields give the amounts of nuclides produced either directly in the fission or by decay of other nuclides.
| Product | Thermal fission yield | Fast fission yield | 14-MeV fission yield |
|---|---|---|---|
| Template:Nuclide | 0.00171 ± 0.00018 | 0.00269 ± 0.00044 | 0.00264 ± 0.00045 |
| Template:Nuclide | 0.00084 ± 0.00015 | 0.00082 ± 0.00012 | 0.00081 ± 0.00012 |
| Template:Nuclide | 0.0108 ± 0.0004 | 0.0108 ± 0.0004 | 0.0174 ± 0.0036 |
| Template:Nuclide | 0.0108 ± 0.0004 | 0.0108 ± 0.0004 | 0.0174 ± 0.0036 |
| Template:Nuclide | 0.1702 ± 0.0049 | 0.17 ± 0.0049 | 0.1667 ± 0.0088 |
| Template:Nuclide | 1.304 ± 0.012 | 1.309 ± 0.043 | 1.64 ± 0.31 |
| Template:Nuclide | 0.000285 ± 0.000076 | 0.00044 ± 0.00016 | 0.038 ± 0.012 |
| Template:Nuclide | 0.286 ± 0.021 | 0.286 ± 0.026 | 0.47 ± 0.1 |
| Template:Nuclide | 1.303 ± 0.012 | 1.307 ± 0.043 | 1.65 ± 0.31 |
| Template:Nuclide | 5.73 ± 0.13 | 5.22 ± 0.18 | 4.41 ± 0.18 |
| Template:Nuclide | 6.502 ± 0.072 | 6.349 ± 0.083 | 5.07 ± 0.19 |
| Template:Nuclide | 0.00000042 ± 0.00000011 | 2.90±0.770 × 10−8 | 0.00004 ± 0.000015 |
| Template:Nuclide | 6.498 ± 0.072 | 6.345 ± 0.083 | 5.07 ± 0.19 |
| Template:Nuclide | 0.0702 ± 0.0067 | 0.0686 ± 0.0071 | 0.0548 ± 0.0072 |
| Template:Nuclide | 0 ± 0 | 0 ± 0 | 0 ± 0 |
| Template:Nuclide | 8.70 × 10−10 ± 3.20 × 10−10 | 0 ± 0 | 6.20 × 10−8 ± 2.50 × 10−8 |
| Template:Nuclide | 0.00042 ± 0.00015 | 0.000069 ± 0.000025 | 0.0033 ± 0.0015 |
| Template:Nuclide | 6.132 ± 0.092 | 5.8 ± 0.13 | 5.02 ± 0.13 |
| Template:Nuclide | 6.132 ± 0.092 | 5.8 ± 0.13 | 5.02 ± 0.13 |
| Template:Nuclide | 3.103 ± 0.084 | 3.248 ± 0.042 | 3.14 ± 0.11 |
| Template:Nuclide | 0.41 ± 0.011 | 0.469 ± 0.036 | 2.15 ± 0.59 |
| Template:Nuclide | 0.41 ± 0.011 | 0.469 ± 0.036 | 2.15 ± 0.59 |
| Template:Nuclide | 0.00106 ± 0.00011 | 0.0039 ± 0.00091 | 0.142 ± 0.023 |
| Template:Nuclide | 0.000000366 ± 0.000000098 | 0.0000004 ± 0.00000014 | 0.00193 ± 0.00068 |
| Template:Nuclide | 0.000089 ± 0.000021 | 0.000112 ± 0.000034 | 0.027 ± 0.01 |
| Template:Nuclide | 0.026 ± 0.0014 | 0.067 ± 0.011 | 1.42 ± 0.42 |
| Template:Nuclide | 4.276 ± 0.043 | 4.639 ± 0.065 | 3.85 ± 0.16 |
| Template:Nuclide | 0.706 ± 0.032 | 1.03 ± 0.26 | 1.59 ± 0.18 |
| Template:Nuclide | 2.878 ± 0.032 | 3.365 ± 0.054 | 4.11 ± 0.14 |
| Template:Nuclide | 6.59 ± 0.11 | 6.61 ± 0.13 | 5.42 ± 0.4 |
| Template:Nuclide | 6.39 ± 0.22 | 6.01 ± 0.18 | 4.8 ± 1.4 |
| Template:Nuclide | 0 ± 0 | 0 ± 0 | 0.00108 ± 0.00048 |
| Template:Nuclide | 0.000038 ± 0.0000098 | 0.000152 ± 0.000055 | 0.038 ± 0.014 |
| Template:Nuclide | 0.0313 ± 0.003 | 0.0365 ± 0.0031 | 0.047 ± 0.0049 |
| Template:Nuclide | 6.6 ± 0.11 | 6.61 ± 0.13 | 5.57 ± 0.41 |
| Template:Nuclide | 0.189 ± 0.015 | 0.19 ± 0.015 | 0.281 ± 0.049 |
| Template:Nuclide | 6.61 ± 0.22 | 6.32 ± 0.18 | 6.4 ± 1.8 |
| Template:Nuclide | 1.22 ± 0.12 | 1.23 ± 0.13 | 2.17 ± 0.66 |
| Template:Nuclide | 0.0000121 ± 0.0000032 | 0.0000279 ± 0.0000073 | 0.0132 ± 0.0035 |
| Template:Nuclide | 6.221 ± 0.069 | 5.889 ± 0.096 | 5.6 ± 1.3 |
| Template:Nuclide | 6.314 ± 0.095 | 5.959 ± 0.048 | 4.474 ± 0.081 |
| Template:Nuclide | 6.315 ± 0.095 | 5.96 ± 0.048 | 4.508 ± 0.081 |
| Template:Nuclide | 5.86 ± 0.15 | 5.795 ± 0.081 | 4.44 ± 0.2 |
| Template:Nuclide | 5.474 ± 0.055 | 5.094 ± 0.076 | 3.154 ± 0.038 |
| Template:Nuclide | 5.474 ± 0.055 | 5.094 ± 0.076 | 3.155 ± 0.038 |
| Template:Nuclide | 6.30 × 10−9 ± 1.70 × 10−9 | 1.70 × 10−9 ± 4.80 × 10−10 | 0.0000137 ± 0.0000049 |
| Template:Nuclide | 5.475 ± 0.055 | 5.094 ± 0.076 | 3.155 ± 0.038 |
| Template:Nuclide | 2.232 ± 0.04 | 2.148 ± 0.028 | 1.657 ± 0.045 |
| Template:Nuclide | 2.232 ± 0.04 | 2.148 ± 0.028 | 1.657 ± 0.045 |
| Template:Nuclide | 5.00 × 10−8 ± 1.70 × 10−8 | 7.40 × 10−9 ± 2.50 × 10−9 | 0.0000013 ± 0.00000042 |
| Template:Nuclide | 0.000000104 ± 0.000000039 | 1.78 × 10−8 ± 6.60 × 10−9 | 0.0000048 ± 0.0000018 |
| Template:Nuclide | 1.053 ± 0.021 | 1.064 ± 0.03 | 0.557 ± 0.09 |
| Template:Nuclide | 0.4204 ± 0.0071 | 0.431 ± 0.015 | 0.388 ± 0.061 |
| Template:Nuclide | 0.000000149 ± 0.000000041 | 2.43 × 10−8 ± 6.80 × 10−9 | 0.0000058 ± 0.0000018 |
| Template:Nuclide | 0.000061 ± 0.000022 | 0.0000201 ± 0.0000077 | 0.00045 ± 0.00018 |
| Template:Nuclide | 0.4204 ± 0.0071 | 0.431 ± 0.015 | 0.388 ± 0.061 |
| Template:Nuclide | 0.1477 ± 0.0071 | 0.1512 ± 0.0097 | 0.23 ± 0.015 |
| Template:Nuclide | 0.4204 ± 0.0071 | 0.431 ± 0.015 | 0.388 ± 0.061 |
| Template:Nuclide | 3.24 × 10−10 ± 8.50 × 10−11 | 0 ± 0 | 3.30 × 10−8 ± 1.10 × 10−8 |
| Template:Nuclide | 0.000000195 ± 0.000000064 | 4.00 × 10−8 ± 1.10 × 10−8 | 0.0000033 ± 0.0000011 |
| Template:Nuclide | 0.0308 ± 0.0013 | 0.044 ± 0.01 | 0.088 ± 0.014 |
| Product | Thermal fission yield | Fast fission yield | 14-MeV fission yield |
|---|---|---|---|
| Template:Nuclide | 0.00408 ± 0.00041 | 0.00346 ± 0.00057 | - |
| Template:Nuclide | 0.00135 ± 0.00019 | 0.00106 ± 0.00016 | - |
| Template:Nuclide | 0.0142 ± 0.0007 | 0.0142 ± 0.0007 | - |
| Template:Nuclide | 0.0142 ± 0.0007 | 0.0142 ± 0.0007 | - |
| Template:Nuclide | 0.2192 ± 0.009 | 0.219 ± 0.009 | - |
| Template:Nuclide | 0.574 ± 0.026 | 0.617 ± 0.049 | - |
| Template:Nuclide | 0.00175 ± 0.0006 | 0.00055 ± 0.0002 | - |
| Template:Nuclide | 0.136 ± 0.014 | 0.138 ± 0.017 | - |
| Template:Nuclide | 0.576 ± 0.026 | 0.617 ± 0.049 | - |
| Template:Nuclide | 2.013 ± 0.054 | 2.031 ± 0.057 | - |
| Template:Nuclide | 4.949 ± 0.099 | 4.682 ± 0.098 | - |
| Template:Nuclide | 0.0000168 ± 0.0000045 | 0.00000255 ± 0.00000069 | - |
| Template:Nuclide | 4.946 ± 0.099 | 4.68 ± 0.098 | - |
| Template:Nuclide | 0.0535 ± 0.0066 | 0.0506 ± 0.0062 | - |
| Template:Nuclide | 0 ± 0 | 0 ± 0 | - |
| Template:Nuclide | 3.60 × 10−8 ± 1.30 × 10−8 | 4.80 × 10−9 ± 1.70 × 10−9 | - |
| Template:Nuclide | 0.0051 ± 0.0018 | 0.0017 ± 0.00062 | - |
| Template:Nuclide | 6.185 ± 0.056 | 5.82 ± 0.13 | - |
| Template:Nuclide | 6.184 ± 0.056 | 5.82 ± 0.13 | - |
| Template:Nuclide | 6.948 ± 0.083 | 6.59 ± 0.16 | - |
| Template:Nuclide | 4.188 ± 0.092 | 4.13 ± 0.24 | - |
| Template:Nuclide | 4.188 ± 0.092 | 4.13 ± 0.24 | - |
| Template:Nuclide | 0.0052 ± 0.0011 | 0.0053 ± 0.0012 | - |
| Template:Nuclide | 0.000024 ± 0.0000063 | 0.0000153 ± 0.000005 | - |
| Template:Nuclide | 0.00228 ± 0.00049 | 0.00154 ± 0.00043 | - |
| Template:Nuclide | 0.117 ± 0.015 | 0.138 ± 0.022 | - |
| Template:Nuclide | 5.095 ± 0.094 | 4.92 ± 0.32 | - |
| Template:Nuclide | 1.407 ± 0.086 | 1.31 ± 0.13 | - |
| Template:Nuclide | 3.724 ± 0.078 | 4.09 ± 0.12 | - |
| Template:Nuclide | 6.97 ± 0.13 | 6.99 ± 0.33 | - |
| Template:Nuclide | 6.33 ± 0.23 | 6.24 ± 0.22 | - |
| Template:Nuclide | 0.00000234 ± 0.00000085 | 0.0000025 ± 0.0000012 | - |
| Template:Nuclide | 0.00166 ± 0.00056 | 0.00231 ± 0.00085 | - |
| Template:Nuclide | 0.0405 ± 0.004 | 0.0444 ± 0.0044 | - |
| Template:Nuclide | 6.99 ± 0.13 | 7.03 ± 0.33 | - |
| Template:Nuclide | 0.216 ± 0.016 | 0.223 ± 0.021 | - |
| Template:Nuclide | 7.36 ± 0.24 | 7.5 ± 0.23 | - |
| Template:Nuclide | 1.78 ± 0.21 | 1.97 ± 0.25 | - |
| Template:Nuclide | 0.00067 ± 0.00018 | 0.00115 ± 0.0003 | - |
| Template:Nuclide | 6.588 ± 0.08 | 6.35 ± 0.12 | - |
| Template:Nuclide | 5.322 ± 0.059 | 5.303 ± 0.074 | - |
| Template:Nuclide | 5.333 ± 0.059 | 5.324 ± 0.075 | - |
| Template:Nuclide | 5.205 ± 0.073 | 5.01 ± 0.16 | - |
| Template:Nuclide | 3.755 ± 0.03 | 3.504 ± 0.053 | - |
| Template:Nuclide | 3.756 ± 0.03 | 3.505 ± 0.053 | - |
| Template:Nuclide | 0.00000145 ± 0.0000004 | 0.00000251 ± 0.00000072 | - |
| Template:Nuclide | 3.756 ± 0.03 | 3.505 ± 0.053 | - |
| Template:Nuclide | 2.044 ± 0.039 | 1.929 ± 0.046 | - |
| Template:Nuclide | 2.044 ± 0.039 | 1.929 ± 0.046 | - |
| Template:Nuclide | 0.0000056 ± 0.0000019 | 0.000012 ± 0.000004 | - |
| Template:Nuclide | 0.0000118 ± 0.0000044 | 0.000029 ± 0.000011 | - |
| Template:Nuclide | 1.263 ± 0.032 | 1.275 ± 0.056 | - |
| Template:Nuclide | 0.776 ± 0.018 | 0.796 ± 0.037 | - |
| Template:Nuclide | 0.0000168 ± 0.0000046 | 0.000039 ± 0.000011 | - |
| Template:Nuclide | 0.00227 ± 0.00078 | 0.0051 ± 0.0019 | - |
| Template:Nuclide | 0.776 ± 0.018 | 0.797 ± 0.037 | - |
| Template:Nuclide | 0.38 ± 0.03 | 0.4 ± 0.18 | - |
| Template:Nuclide | 0.776 ± 0.018 | 0.797 ± 0.037 | - |
| Template:Nuclide | 0.000000195 ± 0.00000005 | 0.00000048 ± 0.00000014 | - |
| Template:Nuclide | 0.000049 ± 0.000012 | 0.000127 ± 0.000043 | - |
| Template:Nuclide | 0.174 ± 0.03 | 0.171 ± 0.054 | - |
| JEFF-3.1 |
Joint Evaluated Fission and Fusion File, Incident-neutron data, http://www-nds.iaea.org/exfor/endf00.htm, 2 October 2006; see also A. Koning, R. Forrest, M. Kellett, R. Mills, H. Henriksson, Y. Rugama, The JEFF-3.1 Nuclear Data Library, JEFF Report 21, OECD/NEA, Paris, France, 2006, Template:ISBN. |
Ordered by mass number
Decays, even if lengthy, are given down to the stable nuclide.
Decays with half lives longer than a century are marked with a single asterisk (Template:Asterisk), while decays with a half life longer than a hundred million years are marked with two asterisks (Template:AsteriskTemplate:Asterisk).
Half lives, decay modes, and branching fractions
| Nuclide | Half-life | Decay mode | Branching fraction | Source | Notes |
|---|---|---|---|---|---|
| Template:Nuclide | 2.9 ± 0.06 m | β− | 1.0 | [7] | Template:Efn |
| Template:Nuclide | 10.752 ± 0.023 y | β− | 1.0 | [8] | |
| Template:Nuclide | 4.48 ± 0.008 h | IT | 0.214 ± 0.005 | [7] | |
| β− | 0.786 ± 0.005 | ||||
| Template:Nuclide | 28.8 ± 0.07 y | β− | 1.0 | [9] | |
| Template:Nuclide | 64.032 ± 0.006 d | β− | 1.0 | [9] | |
| Template:Nuclide | (7.3 ± 0.9) × 106 d | β− | 1.0 | [10] | |
| Template:Nuclide | 3.61 ± 0.03 d | β− | 0.025 ± 0.001 | [9] | Template:Efn |
| IT | 0.975 ± 0.001 | ||||
| Template:Nuclide | 34.985 ± 0.012 d | β− | 1.0 | [10] | |
| Template:Nuclide | (2.111 ± 0.012) × 105 y | β− | 1.0 | [7] | |
| Template:Nuclide | 39.247 ± 0.013 d | β− | 1.0 | [10] | |
| Template:Nuclide | 1.018 ± 0.005 y | β− | 1.0 | [10] | |
| Template:Nuclide | 30.1 ± 0.3 s | β− | 1.0 | [10] | |
| Template:Nuclide | 55 ± 5 y | β− | 0.224 ± 0.02 | [7] | |
| IT | 0.776 ± 0.02 | ||||
| Template:Nuclide | 2.7238 ± 0.0002 d | EC | 0.0241 ± 0.0012 | [7] | |
| β− | 0.9759 ± 0.0012 | ||||
| Template:Nuclide | 60.2 ± 0.03 d | β− | 1.0 | [7] | |
| Template:Nuclide | 2.7584 ± 0.0006 y | β− | 1.0 | [10] | |
| Template:Nuclide | (5.89 ± 0.23) × 109 d | β− | 1.0 | [10] | |
| Template:Nuclide | 8.0233 ± 0.0019 d | β− | 1.0 | [8] | |
| Template:Nuclide | 20.87 ± 0.08 h | β− | 1.0 | [9] | Template:Efn |
| Template:Nuclide | 6.57 ± 0.02 h | β− | 1.0 | [7] | |
| Template:Nuclide | 11.930 ± 0.016 d | IT | 1.0 | [8] | |
| Template:Nuclide | 5.243 ± 0.001 d | β− | 1.0 | [7] | |
| Template:Nuclide | 2.19 ± 0.01 d | IT | 1.0 | [7] | |
| Template:Nuclide | 9.14 ± 0.02 h | β− | 1.0 | [7] | |
| Template:Nuclide | 15.29 ± 0.05 m | β− | 0.003 ± 0.003 | [7] | Template:Efn |
| IT | 0.997 ± 0.003 | ||||
| Template:Nuclide | 2.063 ± 0.003 y | EC | 0.000003 ± 0.000001 | [10] | Template:Efn |
| β− | 0.999997 ± 0.000001 | ||||
| Template:Nuclide | 30.05 ± 0.08 y | β− | 1.0 | [10] | |
| Template:Nuclide | 12.753 ± 0.004 d | β− | 1.0 | [8] | |
| Template:Nuclide | 1.67850 ± 0.00017 d | β− | 1.0 | [8] | |
| Template:Nuclide | 32.508 ± 0.010 d | β− | 1.0 | [9] | |
| Template:Nuclide | 285.1 ± 0.6 d | β− | 1.0 | [10] | |
| Template:Nuclide | 17.28 ± 0.05 m | β− | 1.0 | [7] | |
| Template:Nuclide | 10.98 ± 0.01 d | β− | 1.0 | [7] | |
| Template:Nuclide | 2.6234 ± 0.0002 y | β− | 1.0 | [7] | |
| Template:Nuclide | 41.29 ± 0.11 d | IT | 0.042 ± 0.007 | [7] | |
| β− | 0.958 ± 0.007 | ||||
| Template:Nuclide | 5.368 ± 0.002 d | β− | 1.0 | [7] | |
| Template:Nuclide | 2.2117 ± 0.0021 d | β− | 1.0 | [7] | |
| Template:Nuclide | 1.1833 ± 0.0017 d | β− | 1.0 | [7] | |
| Template:Nuclide | 90 ± 6 y | β− | 1.0 | [7] | |
| Template:Nuclide | 1.938 ± 0.010 d | β− | 1.0 | [10] | |
| Template:Nuclide | (4.941 ± 0.007) × 103 d | β− | 0.279 ± 0.003 | [10] | Template:Efn |
| EC | 0.721 ± 0.003 | ||||
| Template:Nuclide | (3.1381 ± 0.0014) × 103 d | EC | 0.00018 ± 0.00013 | [10] | Template:Efn |
| β− | 0.99982 ± 0.00013 | ||||
| Template:Nuclide | 4.753 ± 0.016 y | β− | 1.0 | [10] |
Ordered by thermal neutron absorption cross section
References
- ↑ a b c Mills, R. W. (1995). Fission product yield evaluation (Doctoral dissertation, University of Birmingham).
- ↑ Script error: No such module "citation/CS1".
- ↑ Script error: No such module "Citation/CS1".
- ↑ Purkayastha, B. C., and G. R. Martin. "The yields of 129I in natural and in neutron-induced fission of uranium." Canadian Journal of Chemistry 34.3 (1956): 293-300.
- ↑ a b Script error: No such module "citation/CS1".
- ↑ Script error: No such module "citation/CS1".
- ↑ a b c d e f g h i j k l m n o p q r s Evaluated Nuclear Structure Data File, http://www-nds.iaea.org/ensdf/, 26 January 2006.
- ↑ a b c d e M.-M. Bé, V. Chisté, C. Dulieu, E. Browne, V. Chechev, N. Kuzmenko, R. Helmer, A. Nichols, E. Schönfeld, R. Dersch, Monographie BIPM-5, Table of Radionuclides, Vol. 2 - A = 151 to 242, 2004.
- ↑ a b c d e Laboratoire National Henri Becquerel, Recommended Data, http://www.nucleide.org/DDEP_WG/DDEPdata.htm Template:Webarchive, 16 January 2006.
- ↑ a b c d e f g h i j k l m n M.-M. Bé, V.P. Chechev, R. Dersch, O.A.M. Helene, R.G. Helmer, M. Herman, S. Hlavác, A. Marcinkowski, G.L. Molnár, A.L. Nichols, E. Schönfeld, V.R. Vanin, M.J. Woods, IAEA CRP "Update of X-ray and Gamma-ray Decay Data Standards for Detector Calibration and Other Applications", IAEA Scientific and Technical Information report STI/PUB/1287, May 2007, International Atomic Energy Agency, Vienna, Austria, Template:ISBN.
External links
- HANDBOOK OF NUCLEAR DATA FOR SAFEGUARDS: DATABASE EXTENSIONS, AUGUST 2008
- File:Ndslivechart.png The Live Chart of Nuclides - IAEA Color-map of yields, and detailed data by click on a nuclide.