This article needs additional citations for verification .(May 2018) |
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Standard atomic weight Ar°(I) | ||||||||||||||||||||||||||||||||||||||||||||||
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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.
Its longest-lived radioactive isotope, 129I, has a half-life of 16.14 million years, which is far too short for it to exist as a primordial nuclide. Cosmogenic sources of 129I produce very tiny quantities of it that are too small to affect atomic weight measurements; iodine is thus also a mononuclidic element—one that is found in nature only as a single nuclide. Most 129I derived radioactivity on Earth is man-made, an unwanted long-lived byproduct of early nuclear tests and nuclear fission accidents.
All other iodine radioisotopes have half-lives less than 60 days, and four of these are used as tracers and therapeutic agents in medicine. These are 123I, 124I, 125I, and 131I. All industrial production of radioactive iodine isotopes involves these four useful radionuclides.
The isotope 135I has a half-life less than seven hours, which is too short to be used in biology. Unavoidable in situ production of this isotope is important in nuclear reactor control, as it decays to 135Xe, the most powerful known neutron absorber, and the nuclide responsible for the so-called iodine pit phenomenon.
In addition to commercial production, 131I (half-life 8 days) is one of the common radioactive fission products of nuclear fission, and is thus produced inadvertently in very large amounts inside nuclear reactors. Due to its volatility, short half-life, and high abundance in fission products, 131I (along with the short-lived iodine isotope 132I, which is produced from the decay of 132Te with a half-life of 3 days) is responsible for the largest part of radioactive contamination during the first week after accidental environmental contamination from the radioactive waste from a nuclear power plant. Thus highly dosed iodine supplements (usually potassium iodide) are given to the populace after nuclear accidents or explosions (and in some cases prior to any such incident as a civil defense mechanism) to reduce the uptake of radioactive iodine compounds by the thyroid before the highly radioactive isotopes have had time to decay.
Nuclide [n 1] | Z | N | Isotopic mass (Da) [4] [n 2] [n 3] | Half-life [5] [n 4] | Decay mode [5] [n 5] | Daughter isotope [n 6] [n 7] | Spin and parity [5] [n 8] [n 4] | Isotopic abundance | |||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Excitation energy [n 4] | |||||||||||||||||||
108I | 53 | 55 | 107.94335(11)# | 26.4(8) ms | α (99.50%) | 104Sb | 1+# | ||||||||||||
p (0.50%) | 107Te | ||||||||||||||||||
β+? | 108Te | ||||||||||||||||||
β+, p? | 107Sb | ||||||||||||||||||
109I | 53 | 56 | 108.9380860(72) | 92.8(8) μs | p (99.986%) | 108Te | (1/2+,3/2+) | ||||||||||||
α (0.014%) | 105Sb | ||||||||||||||||||
110I | 53 | 57 | 109.935085(66) | 664(24) ms | β+ (71%) | 110Te | (1+) | ||||||||||||
α (17%) | 106Sb | ||||||||||||||||||
β+, p (11%) | 109Sb | ||||||||||||||||||
β+, α (1.1%) | 106Sn | ||||||||||||||||||
111I | 53 | 58 | 110.9302692(51) | 2.5(2) s | β+ (99.91%) | 111Te | 5/2+# | ||||||||||||
α (0.088%) | 107Sb | ||||||||||||||||||
β+, p? | 111Te | ||||||||||||||||||
112I | 53 | 59 | 111.928005(11) | 3.34(8) s | β+ (99.01%) | 112Te | 1+# | ||||||||||||
β+, p (0.88%) | 111Sb | ||||||||||||||||||
β+, α (0.104%) | 108Sn | ||||||||||||||||||
α (0.0012%) | 108Sb | ||||||||||||||||||
113I | 53 | 60 | 112.9236501(86) | 6.6(2) s | β+ | 113Te | 5/2+# | ||||||||||||
α (3.310×10−5#%) | 109Sb | ||||||||||||||||||
β+, α? | 109Sn | ||||||||||||||||||
114I | 53 | 61 | 113.922019(22) | 2.01(15) s | β+ | 114Te | 1+ | ||||||||||||
β+, p? | 113Sb | ||||||||||||||||||
α (7.7×10−9#%) | 110Sb | ||||||||||||||||||
114mI | 265.9(5) keV | 6.2(5) s | β+? | 114Te | (7−) | ||||||||||||||
IT? | 114I | ||||||||||||||||||
115I | 53 | 62 | 114.918048(31) | 1.3(2) min | β+ | 115Te | 5/2+# | ||||||||||||
116I | 53 | 63 | 115.916886(81) | 2.91(15) s | β+ | 116Te | 1+ | ||||||||||||
116mI | 430.4(5) keV | 3.27(16) μs | IT | 116I | (7−) | ||||||||||||||
117I | 53 | 64 | 116.913646(27) | 2.22(4) min | β+ (77%) | 117Te | (5/2)+ | ||||||||||||
EC (23%) | 117Te | ||||||||||||||||||
118I | 53 | 65 | 117.913074(21) | 13.7(5) min | β+ | 118Te | (2−) | ||||||||||||
118mI | 188.8(7) keV | 8.5(5) min | β+ | 118Te | (7−) | ||||||||||||||
IT? | 118I | ||||||||||||||||||
119I | 53 | 66 | 118.910061(23) | 19.1(4) min | β+ (51%) | 119Te | 5/2+ | ||||||||||||
EC (49%) | 119Te | ||||||||||||||||||
120I | 53 | 67 | 119.910094(16) | 81.67(18) min | β+ | 120Te | 2− | ||||||||||||
120m1I | 72.61(9) keV | 242(5) ns | IT | 120I | 3+ | ||||||||||||||
120m2I | 320(150) keV | 53(4) min | β+ | 120Te | (7−) | ||||||||||||||
121I | 53 | 68 | 120.9074115(51) | 2.12(1) h | β+ | 121Te | 5/2+ | ||||||||||||
121mI | 2376.9(4) keV | 9.0(14) μs | IT | 121I | 21/2+# | ||||||||||||||
122I | 53 | 69 | 121.9075901(56) | 3.63(6) min | β+ (78%) | 122Te | 1+ | ||||||||||||
EC (22%) | 122Te | ||||||||||||||||||
122m1I | 314.9(4) keV | 193.3(9) ns | IT | 122I | 7− | ||||||||||||||
122m2I | 379.4(5) keV | 79.1(12) μs | IT | 122I | 7− | ||||||||||||||
122m3I | 394.1(5) keV | 78.2(4) μs | IT | 122I | (8+) | ||||||||||||||
122m4I | 444.1(5) keV | 146.5(12) ns | IT | 122I | 8− | ||||||||||||||
123I [n 9] | 53 | 70 | 122.9055898(40) | 13.2232(15) h | EC | 123Te | 5/2+ | ||||||||||||
124I [n 9] | 53 | 71 | 123.9062103(25) | 4.1760(3) d | β+ | 124Te | 2− | ||||||||||||
125I [n 9] | 53 | 72 | 124.9046306(15) | 59.392(8) d | EC | 125Te | 5/2+ | ||||||||||||
126I | 53 | 73 | 125.9056242(41) | 12.93(5) d | β+ (52.7%) | 126Te | 2− | ||||||||||||
β− (47.3%) | 126Xe | ||||||||||||||||||
126mI | 111.00(23) keV | 128 ns | IT | 126I | 3+ | ||||||||||||||
127I [n 10] | 53 | 74 | 126.9044726(39) | Stable | 5/2+ | 1.0000 | |||||||||||||
128I | 53 | 75 | 127.9058094(39) | 24.99(2) min | β− (93.1%) | 128Xe | 1+ | ||||||||||||
β+ (6.9%) | 128Te | ||||||||||||||||||
128m1I | 137.851(3) keV | 845(20) ns | IT | 128I | 4− | ||||||||||||||
128m2I | 167.368(4) keV | 175(15) ns | IT | 128I | (6)− | ||||||||||||||
129I [n 10] [n 11] | 53 | 76 | 128.9049836(34) | 1.614(12)×107 y | β− | 129Xe | 7/2+ | Trace [n 12] | |||||||||||
130I | 53 | 77 | 129.9066702(34) | 12.36(1) h | β− | 130Xe | 5+ | ||||||||||||
130m1I | 39.9525(13) keV | 8.84(6) min | IT (84%) | 130I | 2+ | ||||||||||||||
β− (16%) | 130Xe | ||||||||||||||||||
130m2I | 69.5865(7) keV | 133(7) ns | IT | 130I | 6− | ||||||||||||||
130m3I | 82.3960(19) keV | 315(15) ns | IT | 130I | (8−) | ||||||||||||||
130m4I | 85.1099(10) keV | 254(4) ns | IT | 130I | 6− | ||||||||||||||
131I [n 10] [n 9] | 53 | 78 | 130.90612638(65) | 8.0249(6) d | β− | 131Xe | 7/2+ | ||||||||||||
131mI | 1918.4(4) keV | 24(1) μs | IT | 131I | 19/2− | ||||||||||||||
132I | 53 | 79 | 131.9079935(44) | 2.295(13) h | β− | 132Xe | 4+ | ||||||||||||
132mI | 110(11) keV | 1.387(15) h | IT (86%) | 132I | (8−) | ||||||||||||||
β− (14%) | 132Xe | ||||||||||||||||||
133I | 53 | 80 | 132.9078284(63) | 20.83(8) h | β− | 133Xe | 7/2+ | ||||||||||||
133m1I | 1634.148(10) keV | 9(2) s | IT | 133I | (19/2−) | ||||||||||||||
133m2I | 1729.137(10) keV | ~170 ns | IT | 133I | (15/2−) | ||||||||||||||
133m3I | 2493.7(4) keV | 469(15) ns | IT | 133I | (23/2+) | ||||||||||||||
134I | 53 | 81 | 133.9097757(52) | 52.5(2) min | β− | 134Xe | (4)+ | ||||||||||||
134mI | 316.49(22) keV | 3.52(4) min | IT (97.7%) | 134I | (8)− | ||||||||||||||
β− (2.3%) | 134Xe | ||||||||||||||||||
135I [n 13] | 53 | 82 | 134.9100594(22) | 6.58(3) h | β− | 135Xe | 7/2+ | ||||||||||||
136I | 53 | 83 | 135.914605(15) | 83.4(4) s | β− | 136Xe | (1−) | ||||||||||||
136mI | 206(15) keV | 46.6(11) s | β− | 136Xe | (6−) | ||||||||||||||
137I | 53 | 84 | 136.9180282(90) | 24.13(12) s | β− (92.49%) | 137Xe | 7/2+# | ||||||||||||
β−, n (7.51%) | 136Xe | ||||||||||||||||||
138I | 53 | 85 | 137.9227264(64) | 6.26(3) s | β− (94.67%) | 138Xe | (1−) | ||||||||||||
β−, n (5.33%) | 137Xe | ||||||||||||||||||
138mI | 67.9(3) keV | 1.26(16) μs | IT | 138I | (3−) | ||||||||||||||
139I | 53 | 86 | 138.9264934(43) | 2.280(11) s | β− (90.26%) | 139Xe | 7/2+# | ||||||||||||
β−, n (9.74%) | 138Xe | ||||||||||||||||||
140I | 53 | 87 | 139.931716(13) | 588(10) ms | β− (92.40%) | 140Xe | (2−) | ||||||||||||
β−, n (7.60%) | 139Xe | ||||||||||||||||||
β−, 2n? | 138Xe | ||||||||||||||||||
141I | 53 | 88 | 140.935666(17) | 420(7) ms | β− (78.8%) | 141Xe | 7/2+# | ||||||||||||
β−, n (21.2%) | 140Xe | ||||||||||||||||||
142I | 53 | 89 | 141.9411666(53) | 235(11) ms | β− | 142Xe | 2−# | ||||||||||||
β−, n? | 141Xe | ||||||||||||||||||
β−, 2n? | 140Xe | ||||||||||||||||||
143I | 53 | 90 | 142.94548(22)# | 182(8) ms | β− | 143Xe | 7/2+# | ||||||||||||
β−, n? | 141Xe | ||||||||||||||||||
β−, 2n? | 140Xe | ||||||||||||||||||
144I | 53 | 91 | 143.95134(43)# | 94(8) ms | β− | 144Xe | 1−# | ||||||||||||
β−, n? | 143Xe | ||||||||||||||||||
β−, 2n? | 142Xe | ||||||||||||||||||
145I | 53 | 92 | 144.95585(54)# | 89.7(93) ms | β− | 145Xe | 7/2+# | ||||||||||||
β−, n? | 144Xe | ||||||||||||||||||
β−, 2n? | 143Xe | ||||||||||||||||||
146I | 53 | 93 | 145.96185(32)# | 94(26) ms | β− | 146Xe | |||||||||||||
β−, n? | 145Xe | ||||||||||||||||||
β−, 2n? | 144Xe | ||||||||||||||||||
147I | 53 | 94 | 146.96651(32)# | 60# ms [>550 ns] | β−? | 147Xe | 3/2-# | ||||||||||||
β−, n? | 146Xe | ||||||||||||||||||
β−, 2n? | 145Xe | ||||||||||||||||||
This table header & footer: |
EC: | Electron capture |
IT: | Isomeric transition |
n: | Neutron emission |
p: | Proton emission |
This section needs additional citations for verification .(May 2018) |
Radioisotopes of iodine are called radioactive iodine or radioiodine. Dozens exist, but about a half dozen are the most notable in applied sciences such as the life sciences and nuclear power, as detailed below. Mentions of radioiodine in health care contexts refer more often to iodine-131 than to other isotopes.
Of the many isotopes of iodine, only two are typically used in a medical setting: iodine-123 and iodine-131. Since 131I has both a beta and gamma decay mode, it can be used for radiotherapy or for imaging. 123I, which has no beta activity, is more suited for routine nuclear medicine imaging of the thyroid and other medical processes and less damaging internally to the patient. There are some situations in which iodine-124 and iodine-125 are also used in medicine. [6]
Due to preferential uptake of iodine by the thyroid, radioiodine is extensively used in imaging of and, in the case of 131I, destroying dysfunctional thyroid tissues. Other types of tissue selectively take up certain iodine-131-containing tissue-targeting and killing radiopharmaceutical agents (such as MIBG). Iodine-125 is the only other iodine radioisotope used in radiation therapy, but only as an implanted capsule in brachytherapy, where the isotope never has a chance to be released for chemical interaction with the body's tissues.
The gamma-emitting isotopes iodine-123 (half-life 13 hours), and (less commonly) the longer-lived and less energetic iodine-125 (half-life 59 days) are used as nuclear imaging tracers to evaluate the anatomic and physiologic function of the thyroid. Abnormal results may be caused by disorders such as Graves' disease or Hashimoto's thyroiditis. Both isotopes decay by electron capture (EC) to the corresponding tellurium nuclides, but in neither case are these the metastable nuclides 123mTe and 125mTe (which are of higher energy, and are not produced from radioiodine). Instead, the excited tellurium nuclides decay immediately (half-life too short to detect). Following EC, the excited 123Te from 123I emits a high-speed 127 keV internal conversion electron (not a beta ray) about 13% of the time, but this does little cellular damage due to the nuclide's short half-life and the relatively small fraction of such events. In the remainder of cases, a 159 keV gamma ray is emitted, which is well-suited for gamma imaging.
Excited 125Te resulting from electron capture of 125I also emits a much lower-energy internal conversion electron (35.5 keV), which does relatively little damage due to its low energy, even though its emission is more common. The relatively low-energy gamma from 125I/125Te decay is poorly suited for imaging, but can still be seen, and this longer-lived isotope is necessary in tests that require several days of imaging, for example, fibrinogen scan imaging to detect blood clots.
Both 123I and 125I emit copious low energy Auger electrons after their decay, but these do not cause serious damage (double-stranded DNA breaks) in cells, unless the nuclide is incorporated into a medication that accumulates in the nucleus, or into DNA (this is never the case is clinical medicine, but it has been seen in experimental animal models). [7]
Iodine-125 is also commonly used by radiation oncologists in low dose rate brachytherapy in the treatment of cancer at sites other than the thyroid, especially in prostate cancer. When 125I is used therapeutically, it is encapsulated in titanium seeds and implanted in the area of the tumor, where it remains. The low energy of the gamma spectrum in this case limits radiation damage to tissues far from the implanted capsule. Iodine-125, due to its suitable longer half-life and less penetrating gamma spectrum, is also often preferred for laboratory tests that rely on iodine as a tracer that is counted by a gamma counter, such as in radioimmunoassaying.
125I is used as the radiolabel in investigating which ligands go to which plant pattern recognition receptors (PRRs). [8]
Iodine-124 is a proton-rich isotope of iodine with a half-life of 4.18 days. Its modes of decay are: 74.4% electron capture, 25.6% positron emission. 124I decays to 124Te. Iodine-124 can be made by numerous nuclear reactions via a cyclotron. The most common starting material used is 124Te.
Iodine-124 as the iodide salt can be used to directly image the thyroid using positron emission tomography (PET). [9] Iodine-124 can also be used as a PET radiotracer with a usefully longer half-life compared with fluorine-18. [10] In this use, the nuclide is chemically bonded to a pharmaceutical to form a positron-emitting radiopharmaceutical, and injected into the body, where again it is imaged by PET scan.
Iodine-129 (129I; half-life 15.7 million years) is a product of cosmic ray spallation on various isotopes of xenon in the atmosphere, in cosmic ray muon interaction with tellurium-130, and also uranium and plutonium fission, both in subsurface rocks and nuclear reactors. Artificial nuclear processes, in particular nuclear fuel reprocessing and atmospheric nuclear weapons tests, have now swamped the natural signal for this isotope. Nevertheless, it now serves as a groundwater tracer as indicator of nuclear waste dispersion into the natural environment. In a similar fashion, 129I was used in rainwater studies to track fission products following the Chernobyl disaster.
In some ways, 129I is similar to 36Cl. It is a soluble halogen, exists mainly as a non-sorbing anion, and is produced by cosmogenic, thermonuclear, and in-situ reactions. In hydrologic studies, 129I concentrations are usually reported as the ratio of 129I to total I (which is virtually all 127I). As is the case with 36Cl/Cl, 129I/I ratios in nature are quite small, 10−14 to 10−10 (peak thermonuclear 129I/I during the 1960s and 1970s reached about 10−7). 129I differs from 36Cl in that its half-life is longer (15.7 vs. 0.301 million years), it is highly biophilic, and occurs in multiple ionic forms (commonly, I− and IO3−), which have different chemical behaviors. This makes it fairly easy for 129I to enter the biosphere as it becomes incorporated into vegetation, soil, milk, animal tissue, etc. Excesses of stable 129Xe in meteorites have been shown to result from decay of "primordial" iodine-129 produced newly by the supernovas that created the dust and gas from which the solar system formed. This isotope has long decayed and is thus referred to as "extinct". Historically, 129I was the first extinct radionuclide to be identified as present in the early Solar System. Its decay is the basis of the I-Xe iodine-xenon radiometric dating scheme, which covers the first 85 million years of Solar System evolution.
Iodine-131 (131
I
) is a beta-emitting isotope with a half-life of eight days, and comparatively energetic (190 keV average and 606 keV maximum energy) beta radiation, which penetrates 0.6 to 2.0 mm from the site of uptake. This beta radiation can be used for the destruction of thyroid nodules or hyperfunctioning thyroid tissue and for elimination of remaining thyroid tissue after surgery for the treatment of Graves' disease. The purpose of this therapy, which was first explored by Dr. Saul Hertz in 1941, [11] is to destroy thyroid tissue that could not be removed surgically. In this procedure, 131I is administered either intravenously or orally following a diagnostic scan. This procedure may also be used, with higher doses of radio-iodine, to treat patients with thyroid cancer.
The 131I is taken up into thyroid tissue and concentrated there. The beta particles emitted by the radioisotope destroys the associated thyroid tissue with little damage to surrounding tissues (more than 2.0 mm from the tissues absorbing the iodine). Due to similar destruction, 131I is the iodine radioisotope used in other water-soluble iodine-labeled radiopharmaceuticals (such as MIBG) used therapeutically to destroy tissues.
The high energy beta radiation (up to 606 keV) from 131I causes it to be the most carcinogenic of the iodine isotopes. It is thought to cause the majority of excess thyroid cancers seen after nuclear fission contamination (such as bomb fallout or severe nuclear reactor accidents like the Chernobyl disaster) However, these epidemiological effects are seen primarily in children, and treatment of adults and children with therapeutic 131I, and epidemiology of adults exposed to low-dose 131I has not demonstrated carcinogenicity. [12]
Iodine-135 is an isotope of iodine with a half-life of 6.6 hours. It is an important isotope from the viewpoint of nuclear reactor physics. It is produced in relatively large amounts as a fission product, and decays to xenon-135, which is a nuclear poison with the largest known thermal neutron cross section, which is a cause of multiple complications in the control of nuclear reactors. The process of buildup of xenon-135 from accumulated iodine-135 can temporarily preclude a shut-down reactor from restarting. This is known as xenon poisoning or "falling into an iodine pit".
Iodine fission-produced isotopes not discussed above (iodine-128, iodine-130, iodine-132, and iodine-133) have half-lives of several hours or minutes, rendering them almost useless in other applicable areas. Those mentioned are neutron-rich and undergo beta decay to isotopes of xenon. Iodine-128 (half-life 25 minutes) can decay to either tellurium-128 by electron capture or to xenon-128 by beta decay. It has a specific radioactivity of 2.177×106 TBq/g.
This section possibly contains original research .(May 2018) |
Colloquially, radioactive materials can be described as "hot," and non-radioactive materials can be described as "cold." There are instances in which cold iodide is administered to people in order to prevent the uptake of hot iodide by the thyroid gland. For example, blockade of thyroid iodine uptake with potassium iodide is used in nuclear medicine scintigraphy and therapy with some radioiodinated compounds that are not targeted to the thyroid, such as iobenguane (MIBG), which is used to image or treat neural tissue tumors, or iodinated fibrinogen, which is used in fibrinogen scans to investigate clotting. These compounds contain iodine, but not in the iodide form. However, since they may be ultimately metabolized or break down to radioactive iodide, it is common to administer non-radioactive potassium iodide to insure that metabolites of these radiopharmaceuticals is not sequestered by thyroid gland and inadvertently administer a radiological dose to that tissue.
Potassium iodide has been distributed to populations exposed to nuclear fission accidents such as the Chernobyl disaster. The iodide solution SSKI, a saturated solution of potassium (K) iodide in water, has been used to block absorption of the radioiodine (it has no effect on other radioisotopes from fission). Tablets containing potassium iodide are now also manufactured and stocked in central disaster sites by some governments for this purpose. In theory, many harmful late-cancer effects of nuclear fallout might be prevented in this way, since an excess of thyroid cancers, presumably due to radioiodine uptake, is the only proven radioisotope contamination effect after a fission accident, or from contamination by fallout from an atomic bomb (prompt radiation from the bomb also causes other cancers, such as leukemias, directly). Taking large amounts of iodide saturates thyroid receptors and prevents uptake of most radioactive iodine-131 that may be present from fission product exposure (although it does not protect from other radioisotopes, nor from any other form of direct radiation). The protective effect of KI lasts approximately 24 hours, so must be dosed daily until a risk of significant exposure to radioiodines from fission products no longer exists. [13] [14] Iodine-131 (the most common radioiodine contaminant in fallout) also decays relatively rapidly with a half-life of eight days, so that 99.95% of the original radioiodine has vanished after three months.
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.
A synthetic radioisotope is a radionuclide that is not found in nature: no natural process or mechanism exists which produces it, or it is so unstable that it decays away in a very short period of time. Frédéric Joliot-Curie and Irène Joliot-Curie were the first to produce a synthetic radioisotope in the 20th century. Examples include technetium-99 and promethium-146. Many of these are found in, and harvested from, spent nuclear fuel assemblies. Some must be manufactured in particle accelerators.
Radionuclide therapy uses radioactive substances called radiopharmaceuticals to treat medical conditions, particularly cancer. These are introduced into the body by various means and localise to specific locations, organs or tissues depending on their properties and administration routes. This includes anything from a simple compound such as sodium iodide that locates to the thyroid via trapping the iodide ion, to complex biopharmaceuticals such as recombinant antibodies which are attached to radionuclides and seek out specific antigens on cell surfaces.
A radioactive tracer, radiotracer, or radioactive label is a synthetic derivative of a natural compound in which one or more atoms have been replaced by a radionuclide. By virtue of its radioactive decay, it can be used to explore the mechanism of chemical reactions by tracing the path that the radioisotope follows from reactants to products. Radiolabeling or radiotracing is thus the radioactive form of isotopic labeling. In biological contexts, experiments that use radioisotope tracers are sometimes called radioisotope feeding experiments.
Nuclear fission products are the atomic fragments left after a large atomic nucleus undergoes nuclear fission. Typically, a large nucleus like that of uranium fissions by splitting into two smaller nuclei, along with a few neutrons, the release of heat energy, and gamma rays. The two smaller nuclei are the fission products..
Potassium iodide is a chemical compound, medication, and dietary supplement. It is a medication used for treating hyperthyroidism, in radiation emergencies, and for protecting the thyroid gland when certain types of radiopharmaceuticals are used. In the third world it is also used for treating skin sporotrichosis and phycomycosis. It is a supplement used by people with low dietary intake of iodine. It is administered orally.
Iodine-131 is an important radioisotope of iodine discovered by Glenn Seaborg and John Livingood in 1938 at the University of California, Berkeley. It has a radioactive decay half-life of about eight days. It is associated with nuclear energy, medical diagnostic and treatment procedures, and natural gas production. It also plays a major role as a radioactive isotope present in nuclear fission products, and was a significant contributor to the health hazards from open-air atomic bomb testing in the 1950s, and from the Chernobyl disaster, as well as being a large fraction of the contamination hazard in the first weeks in the Fukushima nuclear crisis. This is because 131I is a major fission product of uranium and plutonium, comprising nearly 3% of the total products of fission. See fission product yield for a comparison with other radioactive fission products. 131I is also a major fission product of uranium-233, produced from thorium.
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.
Caesium (55Cs) has 41 known isotopes, the atomic masses of these isotopes range from 112 to 152. Only one isotope, 133Cs, is stable. The longest-lived radioisotopes are 135Cs with a half-life of 1.33 million years, 137
Cs
with a half-life of 30.1671 years and 134Cs with a half-life of 2.0652 years. All other isotopes have half-lives less than 2 weeks, most under an hour.
Naturally occurring zirconium (40Zr) is composed of four stable isotopes (of which one may in the future be found radioactive), and one very long-lived radioisotope (96Zr), a primordial nuclide that decays via double beta decay with an observed half-life of 2.0×1019 years; it can also undergo single beta decay, which is not yet observed, but the theoretically predicted value of t1/2 is 2.4×1020 years. The second most stable radioisotope is 93Zr, which has a half-life of 1.53 million years. Thirty other radioisotopes have been observed. All have half-lives less than a day except for 95Zr (64.02 days), 88Zr (83.4 days), and 89Zr (78.41 hours). The primary decay mode is electron capture for isotopes lighter than 92Zr, and the primary mode for heavier isotopes is beta decay.
Radionuclides which emit gamma radiation are valuable in a range of different industrial, scientific and medical technologies. This article lists some common gamma-emitting radionuclides of technological importance, and their properties.
Iodine-125 (125I) is a radioisotope of iodine which has uses in biological assays, nuclear medicine imaging and in radiation therapy as brachytherapy to treat a number of conditions, including prostate cancer, uveal melanomas, and brain tumors. It is the second longest-lived radioisotope of iodine, after iodine-129.
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.
Iodine-123 (123I) is a radioactive isotope of iodine used in nuclear medicine imaging, including single-photon emission computed tomography (SPECT) or SPECT/CT exams. The isotope's half-life is 13.2232 hours; the decay by electron capture to tellurium-123 emits gamma radiation with a predominant energy of 159 keV. In medical applications, the radiation is detected by a gamma camera. The isotope is typically applied as iodide-123, the anionic form.
Technetium-99m (99mTc) is a metastable nuclear isomer of technetium-99, symbolized as 99mTc, that is used in tens of millions of medical diagnostic procedures annually, making it the most commonly used medical radioisotope in the world.
Iodine-129 (129I) is a long-lived radioisotope of iodine that occurs naturally but is also of special interest in the monitoring and effects of man-made nuclear fission products, where it serves as both a tracer and a potential radiological contaminant.
Long-lived fission products (LLFPs) are radioactive materials with a long half-life produced by nuclear fission of uranium and plutonium. Because of their persistent radiotoxicity, it is necessary to isolate them from humans and the biosphere and to confine them in nuclear waste repositories for geological periods of time. The focus of this article is radioisotopes (radionuclides) generated by fission reactors.
The radioactive iodine uptake test is a type of scan used in the diagnosis of thyroid problems, particularly hyperthyroidism. It is entirely different from radioactive iodine therapy, which uses much higher doses to destroy cancerous cells. The RAIU test is also used as a follow-up to RAI therapy to verify that no thyroid cells survived, which could still be cancerous.
The committed dose in radiological protection is a measure of the stochastic health risk due to an intake of radioactive material into the human body. Stochastic in this context is defined as the probability of cancer induction and genetic damage, due to low levels of radiation. The SI unit of measure is the sievert.
Radiopharmaceuticals, or medicinal radiocompounds, are a group of pharmaceutical drugs containing radioactive isotopes. Radiopharmaceuticals can be used as diagnostic and therapeutic agents. Radiopharmaceuticals emit radiation themselves, which is different from contrast media which absorb or alter external electromagnetism or ultrasound. Radiopharmacology is the branch of pharmacology that specializes in these agents.