Isotopes of indium
Encyclopedia
Indium
(In) consists of two primordial nuclide
s, with the most common (~ 95.7%) nuclide (115In) being measurably radioactive (although with a very long half-life). The stable isotope 113In is only 4.3% of naturally occurring indium. Among elements with a known stable isotope, only tellurium and rhenium
similarly occur with a stable isotope in lower abundance than the long-lived radioactive isotope. Other than 115In, the longest-lived radioisotope is 111In with a half-life of 2.8047 days. All other radioisotopes have half-lives less than a day. This element also has 47 isomers
, the longest-lived being 114m1In with a half-life of 49.51 days. All other meta-states have half-lives less than a day, most less than an hour, and many measured in milliseconds or less..
Indium-111 is used medically in nuclear imaging, as a radiotracer nuclide tag for gamma camera
localization of protein radiopharmaceuticals, such as In-111-labeled octreotide
, which binds to receptors on certain endocrine tumors (Octreoscan). Indium-111 is also used in indium white blood cell scan
s which use nuclear medical techniques to search for hidden infections.
Standard atomic mass: 114.818(3) u
Indium
Indium is a chemical element with the symbol In and atomic number 49. This rare, very soft, malleable and easily fusible post-transition metal is chemically similar to gallium and thallium, and shows the intermediate properties between these two...
(In) consists of two primordial nuclide
Primordial nuclide
In geochemistry and geonuclear physics, primordial nuclides or primordial isotopes are nuclides found on the earth that have existed in their current form since before Earth was formed. Only 288 such nuclides are known...
s, with the most common (~ 95.7%) nuclide (115In) being measurably radioactive (although with a very long half-life). The stable isotope 113In is only 4.3% of naturally occurring indium. Among elements with a known stable isotope, only tellurium and rhenium
Rhenium
Rhenium is a chemical element with the symbol Re and atomic number 75. It is a silvery-white, heavy, third-row transition metal in group 7 of the periodic table. With an average concentration of 1 part per billion , rhenium is one of the rarest elements in the Earth's crust. The free element has...
similarly occur with a stable isotope in lower abundance than the long-lived radioactive isotope. Other than 115In, the longest-lived radioisotope is 111In with a half-life of 2.8047 days. All other radioisotopes have half-lives less than a day. This element also has 47 isomers
Nuclear isomer
A nuclear isomer is a metastable state of an atomic nucleus caused by the excitation of one or more of its nucleons . "Metastable" refers to the fact that these excited states have half-lives more than 100 to 1000 times the half-lives of the other possible excited nuclear states...
, the longest-lived being 114m1In with a half-life of 49.51 days. All other meta-states have half-lives less than a day, most less than an hour, and many measured in milliseconds or less..
Indium-111 is used medically in nuclear imaging, as a radiotracer nuclide tag for gamma camera
Gamma camera
A gamma camera, also called a scintillation camera or Anger camera, is a device used to image gamma radiation emitting radioisotopes, a technique known as scintigraphy...
localization of protein radiopharmaceuticals, such as In-111-labeled octreotide
Octreotide
Octreotide is an octapeptide that mimics natural somatostatin pharmacologically, though it is a more potent inhibitor of growth hormone, glucagon, and insulin than the natural hormone...
, which binds to receptors on certain endocrine tumors (Octreoscan). Indium-111 is also used in indium white blood cell scan
Indium white blood cell scan
The indium white blood cell scan, also called "indium leukocyte imaging," "indium-111 scan," or simply "indium scan," is a nuclear medicine procedure in which white blood cells are removed from the patient, tagged with the radioisotope Indium-111, and then injected intravenously into the patient...
s which use nuclear medical techniques to search for hidden infections.
Standard atomic mass: 114.818(3) u
Table
nuclide symbol |
Z(p Proton The proton is a subatomic particle with the symbol or and a positive electric charge of 1 elementary charge. One or more protons are present in the nucleus of each atom, along with neutrons. The number of protons in each atom is its atomic number.... ) |
N(n Neutron The neutron is a subatomic hadron particle which has the symbol or , no net electric charge and a mass slightly larger than that of a proton. With the exception of hydrogen, nuclei of atoms consist of protons and neutrons, which are therefore collectively referred to as nucleons. The number of... ) |
isotopic mass (u) |
half-lifeBold for isotopes with half-lives longer than the age of the universe (nearly stable) | decay mode(s)Abbreviations: EC: Electron capture Electron capture Electron capture is a process in which a proton-rich nuclide absorbs an inner atomic electron and simultaneously emits a neutrino... IT: Isomeric transition Isomeric transition An isomeric transition is a radioactive decay process that involves emission of a gamma ray from an atom where the nucleus is in an excited metastable state, referred to in its excited state, as a nuclear isomer.... |
daughter isotope(s)Bold for stable isotopes, bold italics for nearly-stable isotopes (half-life longer than the age of the universe) |
nuclear spin |
representative isotopic composition (mole fraction) |
range of natural variation (mole fraction) |
---|---|---|---|---|---|---|---|---|---|
excitation energy | |||||||||
97In | 49 | 48 | 96.94954(64)# | 5# ms | 9/2+# | ||||
98In | 49 | 49 | 97.94214(21)# | 45(23) ms [32(+32-11) ms] |
β+ Beta decay In nuclear physics, beta decay is a type of radioactive decay in which a beta particle is emitted from an atom. There are two types of beta decay: beta minus and beta plus. In the case of beta decay that produces an electron emission, it is referred to as beta minus , while in the case of a... |
98Cd | 0+# | ||
98mIn | 0(500)# keV | 1.7(8) s [1.2(+12-4) s] |
|||||||
99In | 49 | 50 | 98.93422(43)# | 3.1(8) s [3.0(+8-7) s] |
β+ | 99Cd | 9/2+# | ||
99mIn | 400(150)# keV | 1# s | 1/2-# | ||||||
100In | 49 | 51 | 99.93111(27) | 5.9(2) s | β+ (96.1%) | 100Cd | (6,7)+ | ||
β+, p Proton emission Proton emission is a type of radioactive decay in which a proton is ejected from a nucleus. Proton emission can occur from high-lying excited states in a nucleus following a beta decay, in which case the process is known as beta-delayed proton emission, or can occur from the ground state of very... (3.9%) |
99Ag | ||||||||
101In | 49 | 52 | 100.92634(32)# | 15.1(3) s | β+ | 100Cd | 9/2+# | ||
β+, p | 100Ag | ||||||||
101mIn | 550(100)# keV | 10# s | 1/2-# | ||||||
102In | 49 | 53 | 101.92409(12) | 23.3(1) s | β+ (99.99%) | 102Cd | (6+) | ||
β+, p (.00929%) | 101Ag | ||||||||
103In | 49 | 54 | 102.919914(27) | 60(1) s | β+ | 103Cd | 9/2+# | ||
103mIn | 631.7(1) keV | 34(2) s | (1/2-)# | ||||||
104In | 49 | 55 | 103.91830(9) | 1.80(3) min | β+ | 104Cd | 5,6(+) | ||
104mIn | 93.48(10) keV | 15.7(5) s | IT (80%) | 104In | (3+) | ||||
β+ (20%) | 104Cd | ||||||||
105In | 49 | 56 | 104.914674(19) | 5.07(7) min | β+ | 105Cd | 9/2+ | ||
105mIn | 674.1(3) keV | 48(6) s | IT | 105In | (1/2)- | ||||
106In | 49 | 57 | 105.913465(13) | 6.2(1) min | β+ | 106Cd | 7+ | ||
106mIn | 28.6(3) keV | 5.2(1) min | β+ | 106Cd | (3+) | ||||
107In | 49 | 58 | 106.910295(12) | 32.4(3) min | β+ | 107Cd | 9/2+ | ||
107mIn | 678.5(3) keV | 50.4(6) s | IT | 107In | 1/2- | ||||
108In | 49 | 59 | 107.909698(10) | 58.0(12) min | β+ | 108Cd | 7+ | ||
108mIn | 29.75(5) keV | 39.6(7) min | β+ | 108Cd | 2+ | ||||
109In | 49 | 60 | 108.907151(6) | 4.2(1) h | β+ | 109Cd | 9/2+ | ||
109m1In | 650.1(3) keV | 1.34(7) min | IT | 109In | 1/2- | ||||
109m2In | 2101.8(2) keV | 209(6) ms | (19/2+) | ||||||
110In | 49 | 61 | 109.907165(13) | 4.9(1) h | β+ | 110Cd | 7+ | ||
110mIn | 62.1(5) keV | 69.1(5) min | β+ | 110Cd | 2+ | ||||
111InUsed in medical applications Nuclear medicine In nuclear medicine procedures, elemental radionuclides are combined with other elements to form chemical compounds, or else combined with existing pharmaceutical compounds, to form radiopharmaceuticals. These radiopharmaceuticals, once administered to the patient, can localize to specific organs... |
49 | 62 | 110.905103(5) | 2.8047(5) d | EC Electron capture Electron capture is a process in which a proton-rich nuclide absorbs an inner atomic electron and simultaneously emits a neutrino... |
111Cd | 9/2+ | ||
111mIn | 536.95(6) keV | 7.7(2) min | IT Isomeric transition An isomeric transition is a radioactive decay process that involves emission of a gamma ray from an atom where the nucleus is in an excited metastable state, referred to in its excited state, as a nuclear isomer.... |
111In | 1/2- | ||||
112In | 49 | 63 | 111.905532(6) | 14.97(10) min | β+ (56%) | 112Cd | 1+ | ||
β- (44%) | 112Sn | ||||||||
112m1In | 156.59(5) keV | 20.56(6) min | β+ | 112Cd | 4+ | ||||
112m2In | 350.76(9) keV | 690(50) ns | 7+ | ||||||
112m3In | 613.69(14) keV | 2.81(3) µs | 8- | ||||||
113In | 49 | 64 | 112.904058(3) | Observationally StableTheoretically capable of spontaneous fission Spontaneous fission Spontaneous fission is a form of radioactive decay characteristic of very heavy isotopes. Because the nuclear binding energy reaches a maximum at a nuclear mass greater than about 60 atomic mass units , spontaneous breakdown into smaller nuclei and single particles becomes possible at heavier masses... |
9/2+ | 0.0429(5) | |||
113mIn | 391.699(3) keV | 1.6579(4) h | IT | 113In | 1/2- | ||||
114In | 49 | 65 | 113.904914(3) | 71.9(1) s | β+ (99.5%) | 114Cd | 1+ | ||
β- (0.5%) | 114Sn | ||||||||
114m1In | 190.29(3) keV | 49.51(1) d | IT (96.75%) | 114In | 5+ | ||||
β+ (3.25%) | 114Cd | ||||||||
114m2In | 501.94(3) keV | 43.1(6) ms | IT (96.75%) | 114In | (8-) | ||||
β+ (3.25%) | 114Cd | ||||||||
114m3In | 641.72(3) keV | 4.3(4) µs | (7+) | ||||||
115InFission product Fission product Nuclear fission products are the atomic fragments left after a large atomic nucleus fissions. Typically, a large nucleus like that of uranium fissions by splitting into two smaller nuclei, along with a few neutrons and a large release of energy in the form of heat , gamma rays and neutrinos. The... Primordial Primordial nuclide In geochemistry and geonuclear physics, primordial nuclides or primordial isotopes are nuclides found on the earth that have existed in their current form since before Earth was formed. Only 288 such nuclides are known... radionuclide Radionuclide A radionuclide is an atom with an unstable nucleus, which is a nucleus characterized by excess energy available to be imparted either to a newly created radiation particle within the nucleus or to an atomic electron. The radionuclide, in this process, undergoes radioactive decay, and emits gamma... |
49 | 66 | 114.903878(5) | 4.41(25)×1014 a | β- | 115Sn | 9/2+ | 0.9571(5) | |
115mIn | 336.244(17) keV | 4.486(4) h | IT (95%) | 115In | 1/2- | ||||
β- (5%) | 115Sn | ||||||||
116In | 49 | 67 | 115.905260(5) | 14.10(3) s | β- | 116Sn | 1+ | ||
EC | 116Cd | ||||||||
116m1In | 127.267(6) keV | 54.29(17) min | 5+ | ||||||
116m2In | 289.660(6) keV | 2.18(4) s | 8- | ||||||
117In | 49 | 68 | 116.904514(6) | 43.2(3) min | β- | 117Sn | 9/2+ | ||
117mIn | 315.302(12) keV | 116.2(3) min | β- (52.91%) | 117Sn | 1/2- | ||||
IT (47.09%) | 117In | ||||||||
118In | 49 | 69 | 117.906354(9) | 5.0(5) s | β- | 118Sn | 1+ | ||
118m1In | 100(50)# keV | 4.364(7) min | β- | 118Sn | 5+ | ||||
118m2In | 240(50)# keV | 8.5(3) s | 8- | ||||||
119In | 49 | 70 | 118.905845(8) | 2.4(1) min | β- | 119Sn | 9/2+ | ||
119m1In | 311.37(3) keV | 18.0(3) min | β- (94.4%) | 119Sn | 1/2- | ||||
IT (5.6%) | 119In | ||||||||
119m2In | 654.27(7) keV | 130(15) ns | 1/2+,3/2+ | ||||||
120In | 49 | 71 | 119.90796(4) | 3.08(8) s | β- | 120Sn | 1+ | ||
120m1In | 50(60)# keV | 46.2(8) s | 5+ | ||||||
120m2In | 300(200)# keV | 47.3(5) s | β- | 120Sn | 8(-) | ||||
121In | 49 | 72 | 120.907846(29) | 23.1(6) s | β- | 121Sn | 9/2+ | ||
121mIn | 312.98(8) keV | 3.88(10) min | β- (98.8%) | 121Sn | 1/2- | ||||
IT (1.2%) | 121In | ||||||||
122In | 49 | 73 | 121.91028(5) | 1.5(3) s | β- | 122Sn | 1+ | ||
122m1In | 40(60)# keV | 10.3(6) s | 5+ | ||||||
122m2In | 290(140) keV | 10.8(4) s | β- | 122Sn | 8- | ||||
123In | 49 | 74 | 122.910438(26) | 6.17(5) s | β- | 123mSn | (9/2)+ | ||
123mIn | 327.21(4) keV | 47.4(4) s | β- | 123mSn | (1/2)- | ||||
124In | 49 | 75 | 123.91318(5) | 3.11(10) s | β- | 124Sn | 3+ | ||
124mIn | -20(70) keV | 3.7(2) s | β- | 124Sn | (8)(-#) | ||||
IT | 124In | ||||||||
125In | 49 | 76 | 124.91360(3) | 2.36(4) s | β- | 125mSn | 9/2+ | ||
125mIn | 360.12(9) keV | 12.2(2) s | β- | 125Sn | 1/2(-) | ||||
126In | 49 | 77 | 125.91646(4) | 1.53(1) s | β- | 126Sn | 3(+#) | ||
126mIn | 100(60) keV | 1.64(5) s | β- | 126Sn | 8(-#) | ||||
127In | 49 | 78 | 126.91735(4) | 1.09(1) s | β- (99.97%) | 127mSn | 9/2(+) | ||
β-, n Neutron emission Neutron emission is a type of radioactive decay of atoms containing excess neutrons, in which a neutron is simply ejected from the nucleus. Two examples of isotopes which emit neutrons are helium-5 and beryllium-13... (.03%) |
126Sn | ||||||||
127mIn | 460(70) keV | 3.67(4) s | β- (99.31%) | 127mSn | (1/2-) | ||||
β-, n (.69%) | 126Sn | ||||||||
128In | 49 | 79 | 127.92017(5) | 0.84(6) s | β- (99.96%) | 128Sn | (3)+ | ||
β-, n (.038%) | 127Sn | ||||||||
128m1In | 247.87(10) keV | 10(7) ms | (1)- | ||||||
128m2In | 320(60) keV | 720(100) ms | β- | 128Sn | (8-) | ||||
129In | 49 | 80 | 128.92170(5) | 611(4) ms | β- (99.75%) | 129Sn | 9/2+# | ||
β-, n (.25%) | 128Sn | ||||||||
129m1In | 380(70) keV | 1.23(3) s | β- (97.2%) | 129Sn | (1/2-)# | ||||
β-, n (2.5%) | 128Sn | ||||||||
IT (.3%) | 129In | ||||||||
129m2In | 1688.0(5) keV | 8.5(5) µs | 17/2- | ||||||
130In | 49 | 81 | 129.92497(4) | 0.29(2) s | β- (98.35%) | 130Sn | 1(-) | ||
β-, n (1.65%) | 129Sn | ||||||||
130m1In | 50(50) keV | 538(5) ms | 10-# | ||||||
130m2In | 400(60) keV | 0.54(1) s | (5+) | ||||||
131In | 49 | 82 | 130.92685(3) | 0.28(3) s | β- (97.8%) | 131Sn | (9/2+) | ||
β-, n (2.19%) | 130Sn | ||||||||
131m1In | 363(37) keV | 0.35(5) s | (1/2-) | ||||||
131m2In | 4.10(7) MeV | 320(60) ms | (19/2+ to 23/2+) | ||||||
132In | 49 | 83 | 131.93299(7) | 206(4) ms | β- (94.8%) | 132Sn | (7-) | ||
β-, n (5.2%) | 131Sn | ||||||||
133In | 49 | 84 | 132.93781(32)# | 165(3) ms | β-, n (85%) | 132Sn | (9/2+) | ||
β- (15%) | 133Sn | ||||||||
133mIn | 330(40)# keV | 180# ms | IT | 133In | (1/2-) | ||||
134In | 49 | 85 | 133.94415(43)# | 140(4) ms | β- (79%) | 134Sn | |||
β-, n (17%) | 133Sn | ||||||||
β-, 2n (4%) | 132Sn | ||||||||
135In | 49 | 86 | 134.94933(54)# | 92(10) ms | 9/2+# |