This page discusses each of the main elements in the mixture of fission products produced by nuclear fission of the common nuclear fuels uranium and plutonium. The isotopes are listed by element, in order by atomic number.
Neutron capture by the nuclear fuel in nuclear reactors and atomic bombs also produces actinides and transuranium elements (not listed here). These are found mixed with fission products in spent nuclear fuel and nuclear fallout.
Neutron capture by materials of the nuclear reactor (shielding, cladding, etc.) or the environment (seawater, soil, etc.) produces activation products (not listed here). These are found in used nuclear reactors and nuclear fallout. A small but non-negligible proportion of fission events produces not two, but three fission products (not counting neutrons or subatomic particles). This ternary fission usually produces a very light nucleus such as helium (about 80% of ternary fissions produce an alpha particle) or hydrogen (most of the rest produce tritium or to a lesser extent deuterium and protium) as the third product. This is the main source of tritium from light water reactors. Another source of tritium is Helium-6 which immediately decays to (stable) Lithium-6. Lithium-6 produces tritium when hit by neutrons and is one of the main sources of commercially or militarily produced tritium. If the first or only step of nuclear reprocessing is an aqueous solution (as is the case in PUREX) this poses a problem as tritium contamination cannot be removed from water other than by costly isotope separation. Furthermore, a tiny fraction of the free neutrons involved in the operation of a nuclear reactor decay to a proton and a beta particle before they can interact with anything else. Given that protons from this source are indistinguishable from protons from ternary fission or radiolysis of coolant water, their overall proportion is hard to quantify.
Germanium-72, 73, 74, 76
If germanium-75 is produced, it quickly decays to arsenic. Germanium-76 is essentially stable, only decaying via extremely slow double beta decay to .
Arsenic-75
While arsenic presents no radiological hazard, it is extremely chemically toxic. If it is desired to get rid of arsenic (no matter its origin), thermal neutron irradiation of the only stable isotope will yield short lived which quickly decays to stable . If arsenic is irradiated with sufficient fast neutrons to cause notable "knockout" (n,2n) or even (n,3n) reactions, Isotopes of germanium will be produced instead.
Selenium-77, 78, 79, 80, 82
Se-79, half-life of 327k years, is one of the long-lived fission products. Given the stability of its next lighter and heavier isotopes and the high cross section those isotopes exhibit for various neutron reactions, it is likely that the relatively low yield is due to Se-79 being destroyed in the reactor to an appreciable extent.
Bromine-81
The other stable isotope is "shadowed" by the long half-life of its more neutron rich isobar .
Krypton-83, 84, 85, 86
Krypton-85, with a half-life 10.76 years, is formed by the fission process with a fission yield of about 0.3%. Only 20% of the fission products of mass 85 become 85Kr itself; the rest passes through a short-lived nuclear isomer and then to stable 85Rb. If irradiated reactor fuel is reprocessed, this radioactive krypton may be released into the air. This krypton release can be detected and used as a means of detecting clandestine nuclear reprocessing. Strictly speaking, the stage which is detected is the dissolution of used nuclear fuel in nitric acid, as it is at this stage that the krypton and other fission gases like the more abundant xenon are released. Despite the industrial applications of krypton-85 and the relatively high prices of both krypton and xenon, they are not currently extracted from spent fuel to any appreciable extent even though krypton and xenon both become solid at the temperature of liquid nitrogen and could thus be captured in a cold trap if the flue gas of a voloxidation process were cooled by liquid nitrogen.
Increase of fission gases above a certain limit can lead to fuel pin swelling and even puncture, so that fission gas measurement after discharging the fuel from the reactor is most important to make burn-up calculations, to study the nature of fuel inside the reactor, behaviour with pin materials, for effective utilization of fuel and also reactor safety. In addition to that, they are a nuisance in a nuclear reactor due to being neutron poisons, albeit not to the same extent as isotopes of xenon, another noble gas produced by fission.
Rubidium-85, 87
Rubidium-87 has such a long half-life as to be essentially stable (longer than the age of the Earth). Rubidium-86 quickly decays to stable strontium-86 if produced either directly via (n,2n) reactions in rubidium-87, or via neutron capture in rubidium-85.
Strontium-88, 89, 90
The strontium radioisotopes are very important, as strontium is a calcium mimic which is incorporated in bone growth and therefore has a great ability to harm humans. On the other hand, this also allows 89Sr to be used in the open source radiotherapy of bone tumors. This tends to be used in palliative care to reduce the pain due to secondary tumors in the bones.
Strontium-90 is a strong beta emitter with a half-life of 28.8 years. Its fission product yield decreases as the mass of the fissile nuclide increases - fission of produces more than fission of with fission of in the middle. A map of 90Sr contamination around Chernobyl has been published by the IAEA.Distribution of Surface Ground Contamination by Strontium-90 Released in the Chernobyl Accident and Deposited in the Byelorussian SSR, the Russian SSR, and the Ukrainian SSR (December 1989), IAEA, 1991 Due to its very small neutron absorption cross section, strontium-90 is poorly suited for thermal neutron induced nuclear transmutation as a way of disposing of it.
Strontium-90 has been used in radioisotope thermoelectric generators (RTGs) in the past because of its relatively high power density (0.95 Wthermal/g for the metal, 0.46 Wthermal/g for the commonly used inert perovskite form strontium titanate) and because it is easily extracted from spent fuel (both native strontium metal and strontium oxide react with water by forming soluble strontium hydroxide). However, the increased availability of renewable energy for off-grid applications formerly served by RTGs as well as concern about orphan sources has led to a nigh-total abandonment of in RTGs. The few (largely space based) applications for RTGs that still exist are largely supplied by despite its higher cost, as it has a higher power density, longer half-life and is easier shielded since it is an alpha emitter while strontium-90 is a beta emitter.
Yttrium-89 to 91
The only stable yttrium isotope, 89Y, will be found with yield somewhat less than 1% in a fission product mixture which has been allowed to age for months or years, as the next-longest lived yttrium isotopes have half-lives of only 107 days (88Y) or 59 days (91Y). However, a small amount of yttrium-90 will be found in secular equilibrium with its parent strontium-90 unless the two elements are separated from each other.
90Sr decays into 90Y which is a beta emitter with a half-life of 2.67 days. 90Y is sometimes used for medical purposes and can be obtained either by the neutron activation of stable 89Y or by using a device similar to a technetium cow.
As the half-lives of the unstable yttrium isotopes are low ( being the longest at 106 days), yttrium extracted from strontium-free moderately aged spent fuel has negligible radioactivity. However, the strong gamma emitter will be present as long as its parent nuclide is. Should a nonradioactive sample of yttrium be desired, care must be taken to remove all traces of strontium and sufficient time to let the short lived Y-90 (64 hours half-life) decay must be allowed before the product can be used.
Zirconium-90 to 96
A significant amount of zirconium is formed by the fission process; some of this consists of short-lived radionuclides (95Zr and 97Zr which decay to molybdenum), while almost 10% of the fission products mixture after years of decay consists of five stable or nearly stable isotopes of zirconium plus 93Zr with a halflife of 1.53 million years which is one of the 7 major long-lived fission products. Zirconium is commonly used in cladding of fuel rods due to its low neutron cross section. However, a small share of this zirconium does capture neutrons and contributes to the overall inventory of radioactive zirconium isotopes. Zircalloy cladding is not commonly reused and neither is fission product zirconium, which could be used in cladding as its relatively weak radioactivity would be of no major concern inside a nuclear reactor. Despite its high yield and long live, Zr-93 is generally not deemed to be of major concern as it is not chemically mobile and emits little radiation.
In PUREX plants the zirconium (regardless of source or isotope) sometimes forms a third phase which can be a disturbance in the plant. The third phase is the term in solvent extraction given to a third layer (such as foam and/or emulsion) which forms from the two layers in the solvent extraction process. The zirconium forms the third phase by forming small particles which stabilise the emulsion which is the third phase.
Zirconium-90 mostly forms by successive beta decays out of strontium-90. A nonradioactive zirconium sample can be extracted from spent fuel by extracting strontium-90 and allowing enough of it to decay (e.g. in an RTG). The zirconium can then be separated from the remaining strontium leaving a very isotopically pure Zr-90 sample.
Niobium-95
Niobium-95, with a half-life of 35 days, is initially present as a fission product. The only stable isotope of niobium has mass number 93, and fission products of mass 93 first decay to long-lived zirconium-93 (half-life 1.53 Ma). Niobium-95 will decay to molybdenum-95 which is stable.
Molybdenum-95, 97, 98, 99, 100
The fission product mixture contains significant amounts of molybdenum. Molybdenum-99 is of enormous interest to nuclear medicine as the parent nuclide to , but its short half-life means it will usually decay long before the spent fuel is reprocessed. can be produced both by fission followed by immediate reprocessing (usually only done in small-scale research reactors) or in particle accelerators. As molybdenum-100 only decays extremely slowly via double beta decay (half-life longer than the age of the universe), the molybdenum content of spent fuel will be essentially stable after a few days have passed to allow the molybdenum-99 to decay.
Technetium-99
99Tc, half-life 211 ka, is produced at a yield of about 6% per fission; see also the main fission products page. It is also produced (via the short-lived nuclear isomer technetium-99m) as a decay product of molybdenum-99. Technetium is particularly mobile in the environment as it forms negatively charged pertechnetate-ions (, resembling the permanganate anion), and it presents the biggest radiological hazard among the long-lived fission products. Despite being a metal, technetium usually does not form positively charged ions, but technetium halides like technetium hexafluoride exist. TcF6 is a nuisance in uranium enrichment as its boiling point () is very close to that of uranium hexafluoride (). The issue is known to enrichment facilities because spontaneous fission also yields small amounts of technetium (which will be in secular equilibrium with its parent nuclides in natural uranium) but if fluoride volatility is employed for reprocessing, a significant share of the "uranium" separated by fractional distillation will be contaminated with technetium requiring a further purification step.