Stable nuclide

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Graph of nuclides (isotopes) by type of decay. Orange and blue nuclides are unstable, with the black squares between these regions representing stable nuclides. The continuous line passing below most of the nuclides comprises the positions on the graph of the (mostly hypothetical) nuclides for which proton number would be the same as neutron number. The graph reflects the fact that elements with more than 20 protons either have more neutrons than protons or are unstable. Table isotopes en.svg
Graph of nuclides (isotopes) by type of decay. Orange and blue nuclides are unstable, with the black squares between these regions representing stable nuclides. The continuous line passing below most of the nuclides comprises the positions on the graph of the (mostly hypothetical) nuclides for which proton number would be the same as neutron number. The graph reflects the fact that elements with more than 20 protons either have more neutrons than protons or are unstable.

Stable nuclides are isotopes of a chemical element whose nucleons are in a configuration that does not permit them the surplus energy required to produce a radioactive emission. The nuclei of such isotopes are not radioactive and unlike radionuclides do not spontaneously undergo radioactive decay. [1] When these nuclides are referred to in relation to specific elements they are usually called that element's stable isotopes.

Contents

The 80 elements with one or more stable isotopes comprise a total of 251 nuclides that have not been shown to decay using current equipment. Of these 80 elements, 26 have only one stable isotope and are called monoisotopic. The other 56 have more than one stable isotope. Tin has ten stable isotopes, the largest number of any element.

Definition of stability, and naturally occurring nuclides

Most naturally occurring nuclides are stable (about 251; see list at the end of this article), and about 35 more (total of 286) are known to be radioactive with long enough 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. Primordial radioisotopes are easily detected with half-lives as short as 700 million years (e.g., 235U). This is the present limit of detection,[ citation needed ] as shorter-lived nuclides have not yet been detected undisputedly in nature except when recently produced, such as decay products or cosmic ray spallation.

Many naturally occurring radioisotopes (another 53 or so, for a total of about 339) exhibit still shorter half-lives than 700 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, 14C made from nitrogen).

Some isotopes that are classed as stable (i.e. no radioactivity has been observed for them) are predicted to have extremely long half-lives (sometimes 1018 years or more). [2] 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. For example, 209Bi and 180W were formerly classed as stable, but were found to be alpha-active in 2003. However, such nuclides do not change their status as primordial when they are found to be radioactive.

Most stable isotopes on 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.

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 two exceptions, technetium (element 43) and promethium (element 61), that do not have any stable nuclides. As of 2024, there are total of 251 known "stable" nuclides. In this definition, "stable" means a nuclide that has never been observed to decay against the natural background. Thus, these elements have half-lives too long to be measured by any means, direct or indirect.

Stable isotopes:

These last 26 are thus called monoisotopic elements . [3] The mean number of stable isotopes for elements which have at least one stable isotope is 251/80 = 3.1375.

Physical 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. Such nuclei thus instead undergo double beta decay (or are theorized to do so) with half-lives several orders of magnitude larger than the age of the universe. This makes for a larger number of stable even–even nuclides, which account for 150 of the 251 total. Stable even–even nuclides number as many as three isobars for some mass numbers, and up to seven isotopes for some atomic numbers.

Conversely, of the 251 known stable nuclides, only five have both an odd number of protons and odd number of neutrons: hydrogen-2 (deuterium), lithium-6, boron-10, nitrogen-14, and tantalum-180m. Also, only four naturally occurring, radioactive odd–odd nuclides have a half-life >109 years: potassium-40, vanadium-50, lanthanum-138, and lutetium-176. Odd–odd primordial nuclides are rare because most odd–odd nuclei beta-decay, because the decay products are even–even, and are therefore more strongly bound, due to nuclear pairing effects. [4]

Yet another effect of the instability of an odd number of either type of nucleon is that odd-numbered elements tend to have fewer stable isotopes. Of the 26 monoisotopic elements (those with only one stable isotope), all but one have an odd atomic number, and all but one has an even number of neutrons: the single exception to both rules is beryllium.

The end of the stable elements occurs after lead, largely because nuclei with 128 neutrons—two neutrons above the magic number 126—are extraordinarily unstable and almost immediately alpha-decay. [5] This contributes to the very short half-lives of astatine, radon, and francium. A similar phenomenon occurs to a much lesser extent with 84 neutrons—two neutrons above the magic number 82—where various isotopes of lanthanide elements alpha-decay.

Nuclear isomers, including a "stable" one

The 251 known stable nuclides include tantalum-180m, since even though its decay is automatically implied by its being "metastable", this has not been observed. All "stable" isotopes (stable by observation, not theory) are the ground states of nuclei, except for tantalum-180m, which is a nuclear isomer or excited state. The ground state, tantalum-180, is radioactive with half-life 8 hours; in contrast, the decay of the nuclear isomer is extremely strongly forbidden by spin-parity selection rules. It has been reported by direct observation that the half-life of 180mTa to gamma decay must be >1015 years. Other possible modes of 180mTa decay (beta decay, electron capture, and alpha decay) have also never been observed.

Binding energy per nucleon of common isotopes. Binding energy curve - common isotopes.svg
Binding energy per nucleon of common isotopes.

Still-unobserved decay

It is expected that improvement of experimental sensitivity will allow discovery of very mild radioactivity of some isotopes now considered stable. For example, in 2003 it was reported that bismuth-209 (the only primordial isotope of bismuth) is very mildly radioactive, with half-life (1.9 ± 0.2) × 1019 yr, [6] [7] confirming earlier theoretical predictions [8] from nuclear physics that bismuth-209 would very slowly alpha decay.

Isotopes that are theoretically believed to be unstable but have not been observed to decay are termed observationally stable. Currently there are 105 "stable" isotopes which are theoretically unstable, 40 of which have been observed in detail with no sign of decay, the lightest in any case being 36Ar. Many "stable" nuclides are "metastable" in that they would release energy if they were to decay, [9] and are expected to undergo very rare kinds of radioactive decay, including double beta decay.

146 nuclides from 62 elements with atomic numbers from 1 (hydrogen) through 66 (dysprosium) except 43 (technetium), 61 (promethium), 62 (samarium), and 63 (europium) are theoretically stable to any kind of nuclear decay — except for the theoretical possibility of proton decay, which has never been observed despite extensive searches for it; and spontaneous fission (SF), which is theoretically possible for the nuclides with atomic mass numbers ≥ 93. [10]

Besides SF, other theoretical decay routes for heavier elements include: [10]

These include all nuclides of mass 165 and greater. Argon-36 is the lightest known "stable" nuclide which is theoretically unstable. [10]

The positivity of energy release in these processes means they are allowed kinematically (they do not violate conservation of energy) and, thus, in principle, can occur. [10] 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. 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.

Type of nuclide by stability classNumber of nuclides in classRunning total of nuclides in all classes to this pointNotes
Theoretically stable according to known decay modes, including alpha decay, beta decay, isomeric transition, and double beta decay 146146All the first 66 elements, except 43, 61, 62, and 63. If spontaneous fission is possible for the nuclides with mass numbers ≥ 93, then all such nuclides are unstable, so that only the first 40 elements would be stable. If protons decay, then there are no stable nuclides.
Energetically unstable to one or more known decay modes, but no decay yet seen. Considered stable until radioactivity confirmed.105 [2] [11] 251Total is the observationally stable nuclides. All elements up to lead (except technetium and promethium) are included.
Radioactive primordial nuclides.35286Includes bismuth, thorium, and uranium
Radioactive nonprimordial, but occur naturally on Earth.~61 significant~347 significant Cosmogenic nuclides from cosmic rays; daughters of radioactive primordials such as francium, etc.

List of stable nuclides

The primordial radionuclides are included for comparison; they are italicized and offset from the list of stable nuclides proper.

  1. Hydrogen-1
  2. Hydrogen-2 (deuterium)
  3. Helium-3
  4. Helium-4
    no mass number 5
  5. Lithium-6
  6. Lithium-7
    no mass number 8
  7. Beryllium-9
  8. Boron-10
  9. Boron-11
  10. Carbon-12
  11. Carbon-13
  12. Nitrogen-14
  13. Nitrogen-15
  14. Oxygen-16
  15. Oxygen-17
  16. Oxygen-18
  17. Fluorine-19
  18. Neon-20
  19. Neon-21
  20. Neon-22
  21. Sodium-23
  22. Magnesium-24
  23. Magnesium-25
  24. Magnesium-26
  25. Aluminium-27
  26. Silicon-28
  27. Silicon-29
  28. Silicon-30
  29. Phosphorus-31
  30. Sulfur-32
  31. Sulfur-33
  32. Sulfur-34
  33. Sulfur-36
  34. Chlorine-35
  35. Chlorine-37
  36. Argon-36 (2E)
  37. Argon-38
  38. Argon-40
  39. Potassium-39
    Potassium-40 (B, E) – long-lived primordial radionuclide
  40. Potassium-41
  41. Calcium-40 (2E)*
  42. Calcium-42
  43. Calcium-43
  44. Calcium-44
  45. Calcium-46 (2B)*
    Calcium-48 (2B) – long-lived primordial radionuclide (B also predicted possible)
  46. Scandium-45
  47. Titanium-46
  48. Titanium-47
  49. Titanium-48
  50. Titanium-49
  51. Titanium-50
    Vanadium-50 (B, E) – long-lived primordial radionuclide
  52. Vanadium-51
  53. Chromium-50 (2E)*
  54. Chromium-52
  55. Chromium-53
  56. Chromium-54
  57. Manganese-55
  58. Iron-54 (2E)*
  59. Iron-56
  60. Iron-57
  61. Iron-58
  62. Cobalt-59
  63. Nickel-58 (2E)*
  64. Nickel-60
  65. Nickel-61
  66. Nickel-62
  67. Nickel-64
  68. Copper-63
  69. Copper-65
  70. Zinc-64 (2E)*
  71. Zinc-66
  72. Zinc-67
  73. Zinc-68
  74. Zinc-70 (2B)*
  75. Gallium-69
  76. Gallium-71
  77. Germanium-70
  78. Germanium-72
  79. Germanium-73
  80. Germanium-74
    Germanium-76 (2B) – long-lived primordial radionuclide
  81. Arsenic-75
  82. Selenium-74 (2E)
  83. Selenium-76
  84. Selenium-77
  85. Selenium-78
  86. Selenium-80 (2B)
    Selenium-82 (2B) – long-lived primordial radionuclide
  87. Bromine-79
  88. Bromine-81
    Krypton-78 (2E) – long-lived primordial radionuclide
  89. Krypton-80
  90. Krypton-82
  91. Krypton-83
  92. Krypton-84
  93. Krypton-86 (2B)
  94. Rubidium-85
    Rubidium-87 (B) – long-lived primordial radionuclide
  95. Strontium-84 (2E)*
  96. Strontium-86
  97. Strontium-87
  98. Strontium-88
  99. Yttrium-89
  100. Zirconium-90
  101. Zirconium-91
  102. Zirconium-92
  103. Zirconium-94 (2B)*
    Zirconium-96 (2B) – long-lived primordial radionuclide (B also predicted possible)
  104. Niobium-93
  105. Molybdenum-92 (2E)*
  106. Molybdenum-94
  107. Molybdenum-95
  108. Molybdenum-96
  109. Molybdenum-97
  110. Molybdenum-98 (2B)*
    Molybdenum-100 (2B) – long-lived primordial radionuclide
    Technetiumno stable isotopes
  111. Ruthenium-96 (2E)*
  112. Ruthenium-98
  113. Ruthenium-99
  114. Ruthenium-100
  115. Ruthenium-101
  116. Ruthenium-102
  117. Ruthenium-104 (2B)
  118. Rhodium-103
  119. Palladium-102 (2E)
  120. Palladium-104
  121. Palladium-105
  122. Palladium-106
  123. Palladium-108
  124. Palladium-110 (2B)*
  125. Silver-107
  126. Silver-109
  127. Cadmium-106 (2E)*
  128. Cadmium-108 (2E)*
  129. Cadmium-110
  130. Cadmium-111
  131. Cadmium-112
    Cadmium-113 (B) – long-lived primordial radionuclide
  132. Cadmium-114 (2B)*
    Cadmium-116 (2B) – long-lived primordial radionuclide
  133. Indium-113
    Indium-115 (B) – long-lived primordial radionuclide
  134. Tin-112 (2E)*
  135. Tin-114
  136. Tin-115
  137. Tin-116
  138. Tin-117
  139. Tin-118
  140. Tin-119
  141. Tin-120
  142. Tin-122 (2B)*
  143. Tin-124 (2B)*
  144. Antimony-121
  145. Antimony-123
  146. Tellurium-120 (2E)*
  147. Tellurium-122
  148. Tellurium-123 (E)*
  149. Tellurium-124
  150. Tellurium-125
  151. Tellurium-126
    Tellurium-128 (2B) – long-lived primordial radionuclide
    Tellurium-130 (2B) – long-lived primordial radionuclide
  152. Iodine-127
    Xenon-124 (2E) – long-lived primordial radionuclide
  153. Xenon-126 (2E)
  154. Xenon-128
  155. Xenon-129
  156. Xenon-130
  157. Xenon-131
  158. Xenon-132
  159. Xenon-134 (2B)*
    Xenon-136 (2B) – long-lived primordial radionuclide
  160. Caesium-133
    Barium-130 (2E) – long-lived primordial radionuclide
  161. Barium-132 (2E)*
  162. Barium-134
  163. Barium-135
  164. Barium-136
  165. Barium-137
  166. Barium-138
    Lanthanum-138 (B, E) – long-lived primordial radionuclide
  167. Lanthanum-139
  168. Cerium-136 (2E)*
  169. Cerium-138 (2E)*
  170. Cerium-140
  171. Cerium-142 (α, 2B)*
  172. Praseodymium-141
  173. Neodymium-142
  174. Neodymium-143 (α)
    Neodymium-144 (α) – long-lived primordial radionuclide
  175. Neodymium-145 (α)*
  176. Neodymium-146 (α, 2B)*
    no mass number 147§
  177. Neodymium-148 (α, 2B)*
    Neodymium-150 (2B) – long-lived primordial radionuclide
    Promethium - no stable isotopes
  178. Samarium-144 (2E)
    Samarium-146 (α) – probable long-lived primordial radionuclide
    Samarium-147 (α) – long-lived primordial radionuclide
    Samarium-148 (α) – long-lived primordial radionuclide
  179. Samarium-149 (α)*
  180. Samarium-150 (α)
    no mass number 151§
  181. Samarium-152 (α)
  182. Samarium-154 (2B)*
    Europium-151 (α) – long-lived primordial radionuclide
  183. Europium-153 (α)*
    Gadolinium-152 (α) – long-lived primordial radionuclide (2E also predicted possible)
  184. Gadolinium-154 (α)
  185. Gadolinium-155 (α)
  186. Gadolinium-156
  187. Gadolinium-157
  188. Gadolinium-158
  189. Gadolinium-160 (2B)*
  190. Terbium-159
  191. Dysprosium-156 (α, 2E)*
  192. Dysprosium-158 (α)
  193. Dysprosium-160 (α)
  194. Dysprosium-161 (α)
  195. Dysprosium-162 (α)
  196. Dysprosium-163
  197. Dysprosium-164
  198. Holmium-165 (α)
  199. Erbium-162 (α, 2E)*
  200. Erbium-164 (α, 2E)
  201. Erbium-166 (α)
  202. Erbium-167 (α)
  203. Erbium-168 (α)
  204. Erbium-170 (α, 2B)*
  205. Thulium-169 (α)
  206. Ytterbium-168 (α, 2E)*
  207. Ytterbium-170 (α)
  208. Ytterbium-171 (α)
  209. Ytterbium-172 (α)
  210. Ytterbium-173 (α)
  211. Ytterbium-174 (α)
  212. Ytterbium-176 (α, 2B)*
  213. Lutetium-175 (α)
    Lutetium-176 (B) – long-lived primordial radionuclide (α, E also predicted possible)
    Hafnium-174 (α) – long-lived primordial radionuclide (2E also predicted possible)
  214. Hafnium-176 (α)
  215. Hafnium-177 (α)
  216. Hafnium-178 (α)
  217. Hafnium-179 (α)
  218. Hafnium-180 (α)
  219. Tantalum-180m (α, B, E, IT)* ^
  220. Tantalum-181 (α)
    Tungsten-180 (α) – long-lived primordial radionuclide (2E also predicted possible)
  221. Tungsten-182 (α)*
  222. Tungsten-183 (α)*
  223. Tungsten-184 (α)*
  224. Tungsten-186 (α, 2B)*
  225. Rhenium-185 (α)
    Rhenium-187 (B) – long-lived primordial radionuclide (A also predicted possible)
    Osmium-184 (α) – long-lived primordial radionuclide (2E also predicted possible)
    Osmium-186 (α) – long-lived primordial radionuclide
  226. Osmium-187 (α)
  227. Osmium-188 (α)
  228. Osmium-189 (α)
  229. Osmium-190 (α)
  230. Osmium-192 (α, 2B)*
  231. Iridium-191 (α)
  232. Iridium-193 (α)
    Platinum-190 (α) – long-lived primordial radionuclide (2E also predicted possible)
  233. Platinum-192 (α)*
  234. Platinum-194 (α)
  235. Platinum-195 (α)*
  236. Platinum-196 (α)
  237. Platinum-198 (α, 2B)*
  238. Gold-197 (α)
  239. Mercury-196 (α, 2E)*
  240. Mercury-198 (α)
  241. Mercury-199 (α)
  242. Mercury-200 (α)
  243. Mercury-201 (α)
  244. Mercury-202 (α)
  245. Mercury-204 (2B)
  246. Thallium-203 (α)
  247. Thallium-205 (α)
  248. Lead-204 (α)*
  249. Lead-206 (α)*
  250. Lead-207 (α)*
  251. Lead-208 (α)*
    Bismuth ^^ and above –
    no stable isotopes
    no mass number 209 and above
    Bismuth-209 (α) – long-lived primordial radionuclide
    Thorium-232 (α, SF) – long-lived primordial radionuclide (2B also predicted possible)
    Uranium-235 (α, SF) – long-lived primordial radionuclide
    Uranium-238 (α, 2B, SF) – long-lived primordial radionuclide
    Plutonium-244 (α, SF) – probable long-lived primordial radionuclide (2B also predicted possible)

Abbreviations for predicted unobserved decay: [12] [2] [11]

α for alpha decay, B for beta decay, 2B for double beta decay, E for electron capture, 2E for double electron capture, IT for isomeric transition, SF for spontaneous fission, * for the nuclides whose half-lives have lower bound. Double beta decay has only been listed when beta decay is not also possible.

^ Tantalum-180m is a "metastable isotope", meaning it is an excited nuclear isomer of tantalum-180. See isotopes of tantalum. However, the half-life of this nuclear isomer is so long that it has never been observed to decay, and it thus is an "observationally stable" primordial nuclide, a rare isotope of tantalum. This is the only nuclear isomer with a half-life so long that it has never been observed to decay. It is thus included in this list.

^^ Bismuth-209 was long believed to be stable, due to its half-life of 2.01×1019 years, which is more than a billion times the age of the universe.

§ Europium-151 and samarium-147 are primordial nuclides with very long half-lives of 4.62×1018 years and 1.066×1011 years, respectively.

See also

Related Research Articles

A radionuclide (radioactive nuclide, radioisotope or radioactive isotope) is a nuclide that has excess numbers of either neutrons or protons, giving it excess nuclear energy, and making it unstable. This excess energy can be used in one of three ways: emitted from the nucleus as gamma radiation; transferred to one of its electrons to release it as a conversion electron; or used to create and emit a new particle (alpha particle or beta particle) from the nucleus. During those processes, the radionuclide is said to undergo radioactive decay. These emissions are considered ionizing radiation because they are energetic enough to liberate an electron from another atom. The radioactive decay can produce a stable nuclide or will sometimes produce a new unstable radionuclide which may undergo further decay. Radioactive decay is a random process at the level of single atoms: it is impossible to predict when one particular atom will decay. However, for a collection of atoms of a single nuclide the decay rate, and thus the half-life (t1/2) for that collection, can be calculated from their measured decay constants. The range of the half-lives of radioactive atoms has no known limits and spans a time range of over 55 orders of magnitude.

<span class="mw-page-title-main">Nuclide</span> Atomic species

Nuclides are a class of atoms characterized by their number of protons, Z, their number of neutrons, N, and their nuclear energy state.

<span class="mw-page-title-main">Neutron capture</span> Atomic nuclear process

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Natural tantalum (73Ta) consists of two stable isotopes: 181Ta (99.988%) and 180m
Ta
(0.012%).

Naturally occurring samarium (62Sm) is composed of five stable isotopes, 144Sm, 149Sm, 150Sm, 152Sm and 154Sm, and two extremely long-lived radioisotopes, 147Sm and 148Sm, with 152Sm being the most abundant. 146Sm is also fairly long-lived, but is not long-lived enough to have survived in significant quantities from the formation of the Solar System on Earth, although it remains useful in radiometric dating in the Solar System as an extinct radionuclide. It is the longest-lived nuclide that has not yet been confirmed to be primordial.

Naturally occurring xenon (54Xe) consists of seven stable isotopes and two very long-lived isotopes. Double electron capture has been observed in 124Xe and double beta decay in 136Xe, which are among the longest measured half-lives of all nuclides. The isotopes 126Xe and 134Xe are also predicted to undergo double beta decay, but this process has never been observed in these isotopes, so they are considered to be stable. Beyond these stable forms, 32 artificial unstable isotopes and various isomers have been studied, the longest-lived of which is 127Xe with a half-life of 36.345 days. All other isotopes have half-lives less than 12 days, most less than 20 hours. The shortest-lived isotope, 108Xe, has a half-life of 58 μs, and is the heaviest known nuclide with equal numbers of protons and neutrons. Of known isomers, the longest-lived is 131mXe with a half-life of 11.934 days. 129Xe is produced by beta decay of 129I ; 131mXe, 133Xe, 133mXe, and 135Xe are some of the fission products of both 235U and 239Pu, so are used as indicators of nuclear explosions.

<span class="mw-page-title-main">Isotopes of iodine</span>

There are 40 known isotopes of iodine (53I) from 108I to 147I; all undergo radioactive decay except 127I, which is stable. Iodine is thus a monoisotopic element.

<span class="mw-page-title-main">Fission products (by element)</span> Breakdown of nuclear fission results

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.

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<span class="mw-page-title-main">Neutron number</span> The number of neutrons in a nuclide

The neutron number is the number of neutrons in a nuclide.

<span class="mw-page-title-main">Isotope</span> Different atoms of the same element

Isotopes are distinct nuclear species of the same chemical element. They have the same atomic number and position in the periodic table, but different nucleon numbers due to different numbers of neutrons in their nuclei. While all isotopes of a given element have similar chemical properties, they have different atomic masses and physical properties.

<span class="mw-page-title-main">Primordial nuclide</span> Nuclides predating the Earths formation (found on Earth)

In geochemistry, geophysics and nuclear physics, primordial nuclides, also known as primordial isotopes, are nuclides found on Earth that have existed in their current form since before Earth was formed. Primordial nuclides were present in the interstellar medium from which the solar system was formed, and were formed in, or after, the Big Bang, by nucleosynthesis in stars and supernovae followed by mass ejection, by cosmic ray spallation, and potentially from other processes. They are the stable nuclides plus the long-lived fraction of radionuclides surviving in the primordial solar nebula through planet accretion until the present; 286 such nuclides are known.

<span class="mw-page-title-main">Isobar (nuclide)</span> Atoms of different elements with the same number of nucleons

Isobars are atoms (nuclides) of different chemical elements that have the same number of nucleons. Correspondingly, isobars differ in atomic number but have the same mass number. An example of a series of isobars is 40S, 40Cl, 40Ar, 40K, and 40Ca. While the nuclei of these nuclides all contain 40 nucleons, they contain varying numbers of protons and neutrons.

<span class="mw-page-title-main">Monoisotopic element</span> Element that has only a single stable isotope

A monoisotopic element is an element which has only a single stable isotope (nuclide). There are 26 such elements, as listed.

<span class="mw-page-title-main">Radiogenic nuclide</span>

A radiogenic nuclide is a nuclide that is produced by a process of radioactive decay. It may itself be radioactive or stable.

The Mattauch isobar rule, formulated by Josef Mattauch in 1934, states that if two adjacent elements on the periodic table have isotopes of the same mass number, one of the isotopes must be radioactive. Two nuclides that have the same mass number (isobars) can both be stable only if their atomic numbers differ by more than one. In fact, for currently observationally stable nuclides, the difference can only be 2 or 4, and in theory, two nuclides that have the same mass number cannot be both stable, but many such nuclides which are theoretically unstable to double beta decay have not been observed to decay, e.g. 134Xe. However, this rule cannot make predictions on the half-lives of these radioisotopes.

<span class="mw-page-title-main">Even and odd atomic nuclei</span> Nuclear physics classification method

In nuclear physics, properties of a nucleus depend on evenness or oddness of its atomic number Z, neutron number N and, consequently, of their sum, the mass number A. Most importantly, oddness of both Z and N tends to lower the nuclear binding energy, making odd nuclei generally less stable. This effect is not only experimentally observed, but is included in the semi-empirical mass formula and explained by some other nuclear models, such as the nuclear shell model. This difference of nuclear binding energy between neighbouring nuclei, especially of odd-A isobars, has important consequences for beta decay.

References

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Book references