Graph of isotopes/nuclides by type of decay. Orange and blue nuclides are unstable, with the black squares between these regions representing stable nuclides. The unbroken line passing below many of the nuclides represents the theoretical position on the graph of nuclides for which proton number is the same as neutron number. The graph shows that elements with more than 20 protons must have more neutrons than protons, in order to be stable.

Stable isotopes are chemical isotopes that are may or may not be radioactive, but if radioactive, have half lives too long to be measured.

Only 90 nuclides from the first 40 elements are energetically stable to any kind of decay save proton decay, in theory (see list of nuclides). An additional 137 are theoretically unstable to known types of decay, but no evidence of decay has ever been observered, for a total of 227 nuclides for which there is no evidence whatsoever of radioactivity.

Finally, an additional 30 nuclides have had their predicted decay observed at the right energy, but the half life is too long to be directly measured, or even estimated from decay products found in nature. Without details of decay half life, such nuclides are often still classed as "stable."

Thus, by this definition, there are 257 known stable nuclides of the 80 elements which have one or more stable isotopes. A list of these is given at the end of this article. The 30 nuclides which have been observed to decay by the theoretical route, are marked with an asterisk.

Of the 80 elements with one or more stable isotopes, twenty-six have only a single stable isotope, and are thus termed monoisotopic, and the rest have more than one stable isotope. One element (tin) has ten stable isotopes, the largest number known for an element.

Properties of stable isotopes

Different isotopes of the same element (whether stable or unstable) have nearly the same chemical characteristics and therefore behave almost identically in biology (a notable exception is the isotopes of hydrogen-see heavy water). The mass differences, due to a difference in the number of neutrons, will result in partial separation of the light isotopes from the heavy isotopes during chemical reactions and during physical processes such as diffusion and vaporization. This process is called isotope fractionation. For example, the difference in mass between the two stable isotopes of hydrogen, ¹H (1 proton, no neutron, also known as protium) and ²H (1 proton, 1 neutron, also known as deuterium) is almost 100%. Therefore, a significant fractionation will occur.

Study of stable isotopes

Commonly analysed stable isotopes include oxygen, carbon, nitrogen, hydrogen and sulfur. These isotope systems have been under investigation for many years in order to study processes of isotope fractionation in natural systems because they are relatively simple to measure. Recent advances in mass spectrometry (i.e. multiple-collector inductively coupled plasma mass spectrometry) now enable the measurement of heavier stable isotopes, such as iron, copper, zinc, molybdenum, etc.

Stable isotopes have been used in botanical and plant biological investigations for many years, and more and more ecological and biological studies are finding stable isotopes (mostly carbon, nitrogen and oxygen) to be extremely useful. Other workers have used oxygen isotopes to reconstruct historical atmospheric temperatures, making them important tools for climate research.

Definition of stability, and natural isotopic presence

Most naturally occurring nuclides are stable (about 257; see list at the end of this article); and about 31 more (total of 288) are known radioactives with sufficiently long half-lives (also known) to occur "primordially." If the half-life of a nuclide is comparable to, or greater than, the Earth's age (4.5 billion years), a significant amount will have survived since the formation of the Solar System, and then is said to be primordial. It will then contribute in that way to the natural isotopic composition of a chemical element. Primordially present radioisotopes are easily detected with half-lives as short as 700 million years (e.g., ²³⁵U), although some primordial isotopes have been detected with half lives as short as 80 million years (e.g., ²⁴⁴Pu). However, this is the present limit of detection, as the nuclide with the next-shortest half life (niobium-92 with half life 34.7 million years) has not been yet been detected in nature.

Many naturally-occurring radioisotopes (another 51 or so, for a total of about 339) exhibit still shorter half-lives than 80 million years, but they are made freshly, as daughter products of decay processes of primordial nuclides (for example, radium from uranium) or from ongoing energetic reactions, such as cosmogenic nuclides produced by present bombardment of Earth by cosmic rays (for example, carbon-14 made from nitrogen).

Many isotopes that are classed as stable (i.e. no radioactivity has been observed for them; or else it has been observed but no half life can be determined) are predicted to have extremely long half-lives (sometimes as high as 10¹⁸ years or more). If the predicted half-life falls into an experimentally accessible range, such isotopes have a chance to move from the list of stable nuclides to the radioactive category, once their activity is observed. Good examples are bismuth-209 and tungsten-180 which were formerly classed as stable, but have been recently (2003) found to be alpha-active. However, such nuclides do not change their status as primordial.

Most stable isotopes in the earth are believed to have been formed in processes of nucleosynthesis, either in the 'Big Bang', or in generations of stars that preceded the formation of the solar system. However, some stable isotopes also show abundance variations in the earth as a result of decay from long-lived radioactive nuclides. These decay-products are termed radiogenic isotopes, in order to distinguish them from the much larger group of 'non-radiogenic' isotopes. They play an important role in radiometric dating and isotope geochemistry and also helpful for determining the food web dynamics in an aquatic ecosystem

Research areas

The so-called Island of Stability may reveal a number of long-lived or even stable atoms that are heavier (and with more protons) than lead.

Stable isotope fractionation

There are three types of isotope fractionation:

• equilibrium fractionation
• kinetic fractionation
• mass-independent fractionation

Isotopes per element

Of the known chemical elements, 80 elements have at least one stable nuclide. These comprise the first 82 elements from hydrogen to lead, with the exceptions of technetium (#43) and promethium (#61), which do not have any stable nuclides. As of January 2010, there were a total of 257 known "stable" nuclides. In this definition, "stable" means a nuclide which has either never been observed to decay, or if observed to decay (the case for 30 of the 257 nuclides), has a half life too long to be measured by any means, direct or indirect.

Only one element (tin) has 10 stable isotopes, and one (xenon) has nine stable isotopes. No elements have exactly eight stable isotopes, but five elements have seven stable isotopes, eight have six stable isotopes, ten have five stable isotopes, eight have four stable isotopes, five have three stable isotopes, 16 have two stable isotopes, and 26 have only a single stable isotope and are thus considered monoisotopic elements.^[1] The mean number of stable isotopes for elements which have at least one such isotope, is 257/80 = 3.2.

"Magic numbers" and odd and even proton and neutron count

Stability of isotopes is affected by the ratio of protons to neutrons, and also by presence of certain "magic numbers" of neutrons or protons which represent closed and filled quantum shells. These quantum shells correspond to a set of energy levels within the shell model of the nucleus; filled shells, such as the filled shell of 50 protons for tin, confers unusual stability on the nuclide. As in the case of tin, a magic number for Z, the atomic number, tends to increase the number of stable isotopes for the element.

Just as in the case of electrons, which have the lowest energy state when they occur in pairs in a given orbital, nucleons (both protons and neutrons) exhibit a lower energy state when their number is even, rather than odd. This stability tends to prevent beta decay (in two steps) of many even-even nuclides into another even-even nuclide of the same mass number but lower energy (and of course with two more protons and two fewer neutrons), because decay proceeding one step at a time would have to pass through an odd-odd nuclide of higher energy. This makes for a larger number of stable even-even nuclides, up to three for some mass numbers, and up to seven for some atomic (proton) numbers. Conversely, of the 257 known stable nuclides, only four have both an odd number of protons and odd number of neutrons: hydrogen-2 (deuterium), lithium-6, boron-10 and nitrogen-14. Also, only four naturally occurring, radioactive odd-odd nuclides have a half-life over a billion years: potassium-40, vanadium-50, lanthanum-138 and tantalum-180m. Odd-odd primordial nuclides are rare because most odd-odd nuclei are highly unstable with respect to beta decay, because the decay products are even-even, and are therefore more strongly bound, due to nuclear pairing effects.^[2]

Yet another effect of the instability of an odd number of either type of nucleons, is that odd-numbered elements tend to have fewer stable isotopes. Of the 26 monoisotopic elements that have only a single stable isotope, all but one have an odd atomic number - the single exception to both rules being beryllium. All of these elements also have an even number of neutrons, with the single exception again being beryllium.

Nuclear isomers, including a "stable" one

The count of 257 known stable nuclides includes Ta-180m, since even though its decay and instability is automatically implied by its notation of "metastable", still this has not yet been observed. All "stable" isotopes (stable by observation, not theory) are the ground states of nuclei, with the exception of tantalum-180m, which is the nuclear isomer or excited level (the ground state of this nucleus is radioactive with a very short half-life of 8 hours); but the decay of the excited nuclear isomer is extremely strongly forbidden by spin-parity selection rules. It has been reported experimentally by direct observation that the half-life of ^180mTa to gamma decay must be more than 10¹⁵ years. Other possible modes of ^180mTa decay (beta decay, electron capture and alpha decay) have also never been observed.

Primordial radioactive and naturally occurring non-primordial isotopes

Elements with more than 82 protons only have radioactive isotopes, although they can still occur naturally because their half-lives are more than about 2% of the time since the supernova nucleosynthesis of the elements from which our solar system was made. An extreme case of this is plutonium-244, which is still detectable from primordial reservoirs, even though it has a half-life of only 80 million years (1.8% of the solar system age). In about 50 known cases, elements with shorter half-lives than plutonium-244 are naturally observed on Earth, since as they are produced by cosmic rays (e.g., carbon-14), or else because (like radium and polonium) they occur in a decay chain of radioactive isotopes (primarily uranium and thorium), which have long-enough half-lifes to be abundant primordially.

Still-unobserved decay

Binding energy per nucleon of common isotopes.

It is expected that continuous improvement of experimental sensitivity will allow discovery of very mild radioactivity (instability) of some isotopes that are considered stable today. For example, it wasn't until 2003 that bismuth-209 (the only naturally-occurring isotope of bismuth) was shown to be very mildly radioactive.^[3] Many "stable" nuclides are possibly "meta-stable" in as much as they may be calculated to have an energy release^[4] upon several possible kinds of radioactive decays.

Only 90 nuclides from the first 40 elements are theoretically stable to any sort of decay save proton decay (which has not been observed). The rest, starting with niobium-93, are theoretically unstable to processes like spontaneous fission.

For processes other than spontaneous fission, other theoretical decay routes for heavier elements include:

• alpha decay - 70 heavy nuclides
• double beta decay (including double electron capture, electron-positron conversion and double positron decay) - 55 nuclides
• beta decay - Ta-180m
• electron capture - Te-123, Ta-180m
• isomeric transition - Ta-180m
• cluster decay and spontaneous fission - many heaviest nuclides

These include all nuclides of mass 165 and greater, and all but nine nuclides of mass 140 and greater.

The positivity of energy release in these processes means that they are allowed kinematically (they do not violate the conservation of energy) and, thus, in principle, can occur. They are not observed due to strong but not absolute suppression, by spin-parity selection rules (for beta decays and isomeric transitions) or by the thickness of the potential barrier (for alpha and cluster decays and spontaneous fission).

Summary table for numbers of each class of nuclides

This is a summary table from List of nuclides. Note that numbers are not exact, and may change slightly in the future, as nuclides are observed to be radioactive, or new half lives are determined to some precision. Note that only the 257 have any claim to stability, but that only 90 nuclides from the first 40 elements are theoretically stable to any process but proton decay.

List of observationally-stable isotopes

In the list below, the predicted (but often not observed) modes of radioactive decay are noted as: A for alpha decay, B for beta decay, BB for double beta decay, E for electron capture, EE for double electron capture, and IT for isomeric transition. Because of the curve of binding energy, many nuclides beyond Z = 41 (niobium) are theoretically unstable with regard to spontaneous fission (see list of nuclides for details).

Some sources may give lower limits on possible half-lives for such decays, estimated either from theory or (negative) observation. However, without a hard figure for decay half life (the case for 30 nuclides, marked with an asterisks * ), nuclides are still classed as being "observationally-stable," and remain in this list. These 30 include nuclides such as zirconium-96, given as "stable" in some lists, and as unstable with unknown half life, in other lists.

Abbreviations:
A for alpha decay, B for beta decay, BB for double beta decay, E for electron capture, EE for double electron capture, IT for isomeric transition. * = Observed decay, half life unknown.

See also

• Table of nuclides
• List of nuclides (905 nuclides in order of stability, all with half lives > one hour)
• Isotope geochemistry
• Radionuclide
• Mononuclidic element
• Primordial nuclide
• List of elements by stability of isotopes
• List of elements by nuclear stability

References

1. ^ Sonzogni, Alejandro. "Interactive Chart of Nuclides". National Nuclear Data Center: Brook haven National Laboratory. http://www.nndc.bnl.gov/chart/. Retrieved 2008-06-06. 
2. ^ Various (2002). Lide, David R.. ed. Handbook of Chemistry & Physics (88th ed.). CRC. ISBN 0849304865. OCLC 179976746. http://www.hbcpnetbase.com/. Retrieved 2008-05-23. 
3. ^ "WWW Table of Radioactive Isotopes". http://nucleardata.nuclear.lu.se/nucleardata/toi/listnuc.asp?sql=&HlifeMin=1e30&tMinStr=1e30+s&HlifeMax=1e40&tMaxStr=1e+40+s. 
4. ^ AME2003 Atomic Mass Evaluation from the National Nuclear Data Center

Book references

• Various (2002). Lide, David R.. ed. Handbook of Chemistry & Physics (88th ed.). CRC. ISBN 0849304865. OCLC 179976746. http://www.hbcpnetbase.com/. Retrieved 2008-05-23. 

External links

• The LIVEChart of Nuclides - IAEA in Java or HTML