Isotopes of thallium
Encyclopedia
Thallium
(Tl) has 37 isotope
s which have atomic mass
es that range from 176 to 212. 203Tl and 205Tl are the only stable isotopes and 204Tl is the most stable radioisotope with a half-life
of 3.78 years. 207Tl, with a half-life of 4.77 minutes, has the longest half-life of naturally occurring radioisotopes.
Thallium-202 (half-life 12.23 days) can be made in a cyclotron while thallium-204 (half-life 3.78 years) is made by the neutron activation
of stable thallium in a nuclear reactor
.
Standard atomic mass: 204.3833(2) u
Thallium
Thallium is a chemical element with the symbol Tl and atomic number 81. This soft gray poor metal resembles tin but discolors when exposed to air. The two chemists William Crookes and Claude-Auguste Lamy discovered thallium independently in 1861 by the newly developed method of flame spectroscopy...
(Tl) has 37 isotope
Isotope
Isotopes are variants of atoms of a particular chemical element, which have differing numbers of neutrons. Atoms of a particular element by definition must contain the same number of protons but may have a distinct number of neutrons which differs from atom to atom, without changing the designation...
s which have atomic mass
Atomic mass
The atomic mass is the mass of a specific isotope, most often expressed in unified atomic mass units. The atomic mass is the total mass of protons, neutrons and electrons in a single atom....
es that range from 176 to 212. 203Tl and 205Tl are the only stable isotopes and 204Tl is the most stable radioisotope with a half-life
Half-life
Half-life, abbreviated t½, is the period of time it takes for the amount of a substance undergoing decay to decrease by half. The name was originally used to describe a characteristic of unstable atoms , but it may apply to any quantity which follows a set-rate decay.The original term, dating to...
of 3.78 years. 207Tl, with a half-life of 4.77 minutes, has the longest half-life of naturally occurring radioisotopes.
Thallium-202 (half-life 12.23 days) can be made in a cyclotron while thallium-204 (half-life 3.78 years) is made by the neutron activation
Neutron activation
Neutron activation is the process in which neutron radiation induces radioactivity in materials, and occurs when atomic nuclei capture free neutrons, becoming heavier and entering excited states. The excited nucleus often decays immediately by emitting particles such as neutrons, protons, or alpha...
of stable thallium in a nuclear reactor
Nuclear reactor
A nuclear reactor is a device to initiate and control a sustained nuclear chain reaction. Most commonly they are used for generating electricity and for the propulsion of ships. Usually heat from nuclear fission is passed to a working fluid , which runs through turbines that power either ship's...
.
Standard atomic mass: 204.3833(2) u
Table
nuclide symbol |
historic name |
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-life | 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 |
nuclear spin |
representative isotopic composition (mole fraction) |
range of natural variation (mole fraction) |
---|---|---|---|---|---|---|---|---|---|---|
excitation energy | ||||||||||
176Tl | 81 | 95 | 176.00059(21)# | 5.2(+30-14) ms | (3-,4-,5-) | |||||
177Tl | 81 | 100 | 176.996427(27) | 18(5) ms | 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... |
176Hg | (1/2+) | |||
α Alpha decay Alpha decay is a type of radioactive decay in which an atomic nucleus emits an alpha particle and thereby transforms into an atom with a mass number 4 less and atomic number 2 less... (rare) |
173Au | |||||||||
177mTl | 807(18) keV | 230(40) µs | p | 176Hg | (11/2-) | |||||
α | 173Au | |||||||||
178Tl | 81 | 97 | 177.99490(12)# | 255(10) ms | α | 174Au | ||||
p (rare) | 177Hg | |||||||||
179Tl | 81 | 98 | 178.99109(5) | 270(30) ms | α | 175Au | (1/2+) | |||
p (rare) | 178Hg | |||||||||
179mTl | 860(30)# keV | 1.60(16) ms | α | 175Au | (9/2-) | |||||
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.... (rare) |
179Tl | |||||||||
180Tl | 81 | 99 | 179.98991(13)# | 1.5(2) s | α (75%) | 176Au | ||||
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... (25%) |
180Hg | |||||||||
β+, 80Kr (10−4%) | 100Ru, 80Kr | |||||||||
181Tl | 81 | 100 | 180.986257(10) | 3.2(3) s | α | 177Au | 1/2+# | |||
β+ | 181Hg | |||||||||
181mTl | 857(29) keV | 1.7(4) ms | α | 177Au | 9/2-# | |||||
β+ | 181Hg | |||||||||
182Tl | 81 | 101 | 181.98567(8) | 2.0(3) s | β+ (96%) | 182Hg | 2-# | |||
α (4%) | 178Au | |||||||||
182m1Tl | 100(100)# keV | 2.9(5) s | α | 178Au | (7+) | |||||
β+ (rare) | 182Hg | |||||||||
182m2Tl | 600(140)# keV | 10- | ||||||||
183Tl | 81 | 102 | 182.982193(10) | 6.9(7) s | β+ (98%) | 183Hg | 1/2+# | |||
α (2%) | 179Au | |||||||||
183m1Tl | 630(17) keV | 53.3(3) ms | IT (99.99%) | 183Tl | 9/2-# | |||||
α (.01%) | 179Au | |||||||||
183m2Tl | 976.8(3) keV | 1.48(10) µs | (13/2+) | |||||||
184Tl | 81 | 103 | 183.98187(5) | 9.7(6) s | β+ | 184Hg | 2-# | |||
184m1Tl | 100(100)# keV | 10# s | β+ (97.9%) | 184Hg | 7+# | |||||
α (2.1%) | 180Au | |||||||||
184m2Tl | 500(140)# keV | >20 ns | (10-) | |||||||
185Tl | 81 | 104 | 184.97879(6) | 19.5(5) s | α | 181Au | 1/2+# | |||
β+ | 185Hg | |||||||||
185mTl | 452.8(20) keV | 1.93(8) s | IT (99.99%) | 185Tl | 9/2-# | |||||
α (.01%) | 181Au | |||||||||
β+ | 185Hg | |||||||||
186Tl | 81 | 105 | 185.97833(20) | 40# s | β+ | 186Hg | (2-) | |||
α (.006%) | 182Au | |||||||||
186m1Tl | 320(180) keV | 27.5(10) s | β+ | 186Hg | (7+) | |||||
186m2Tl | 690(180) keV | 2.9(2) s | (10-) | |||||||
187Tl | 81 | 106 | 186.975906(9) | ~51 s | β+ | 187Hg | (1/2+) | |||
α (rare) | 183Au | |||||||||
187mTl | 335(3) keV | 15.60(12) s | α | 183Au | (9/2-) | |||||
IT | 187Tl | |||||||||
β+ | 187Hg | |||||||||
188Tl | 81 | 107 | 187.97601(4) | 71(2) s | β+ | 188Hg | (2-) | |||
188m1Tl | 40(30) keV | 71(1) s | β+ | 188Hg | (7+) | |||||
188m2Tl | 310(30) keV | 41(4) ms | (9-) | |||||||
189Tl | 81 | 108 | 188.973588(12) | 2.3(2) min | β+ | 189Hg | (1/2+) | |||
189mTl | 257.6(13) keV | 1.4(1) min | β+ (96%) | 189Hg | (9/2-) | |||||
IT (4%) | 189Tl | |||||||||
190Tl | 81 | 109 | 189.97388(5) | 2.6(3) min | β+ | 190Hg | 2(-) | |||
190m1Tl | 130(90)# keV | 3.7(3) min | β+ | 190Hg | 7(+#) | |||||
190m2Tl | 290(70)# keV | 750(40) µs | (8-) | |||||||
190m3Tl | 410(70)# keV | >1 µs | 9- | |||||||
191Tl | 81 | 110 | 190.971786(8) | 20# min | β+ | 191Hg | (1/2+) | |||
191mTl | 297(7) keV | 5.22(16) min | β+ | 191Hg | 9/2(-) | |||||
192Tl | 81 | 111 | 191.97223(3) | 9.6(4) min | β+ | 192Hg | (2-) | |||
192m1Tl | 160(50) keV | 10.8(2) min | β+ | 192Hg | (7+) | |||||
192m2Tl | 407(54) keV | 296(5) ns | (8-) | |||||||
193Tl | 81 | 112 | 192.97067(12) | 21.6(8) min | β+ | 193Hg | 1/2(+#) | |||
193mTl | 369(4) keV | 2.11(15) min | IT (75%) | 193Tl | 9/2- | |||||
β+ (25%) | 193Hg | |||||||||
194Tl | 81 | 113 | 193.97120(15) | 33.0(5) min | β+ | 194Hg | 2- | |||
α (10−7%) | 190Au | |||||||||
194mTl | 300(200)# keV | 32.8(2) min | β+ | 194Hg | (7+) | |||||
195Tl | 81 | 114 | 194.969774(15) | 1.16(5) h | β+ | 195Hg | 1/2+ | |||
195mTl | 482.63(17) keV | 3.6(4) s | IT | 195Tl | 9/2- | |||||
196Tl | 81 | 115 | 195.970481(13) | 1.84(3) h | β+ | 196Hg | 2- | |||
196mTl | 394.2(5) keV | 1.41(2) h | β+ (95.5%) | 196Hg | (7+) | |||||
IT (4.5%) | 196Tl | |||||||||
197Tl | 81 | 116 | 196.969575(18) | 2.84(4) h | β+ | 197Hg | 1/2+ | |||
197mTl | 608.22(8) keV | 540(10) ms | IT | 197Tl | 9/2- | |||||
198Tl | 81 | 117 | 197.97048(9) | 5.3(5) h | β+ | 198Hg | 2- | |||
198m1Tl | 543.5(4) keV | 1.87(3) h | β+ (54%) | 198Hg | 7+ | |||||
IT (46%) | 198Tl | |||||||||
198m2Tl | 687.2(5) keV | 150(40) ns | (5+) | |||||||
198m3Tl | 742.3(4) keV | 32.1(10) ms | (10-)# | |||||||
199Tl | 81 | 118 | 198.96988(3) | 7.42(8) h | β+ | 199Hg | 1/2+ | |||
199mTl | 749.7(3) keV | 28.4(2) ms | IT | 199Tl | 9/2- | |||||
200Tl | 81 | 119 | 199.970963(6) | 26.1(1) h | β+ | 200Hg | 2- | |||
200m1Tl | 753.6(2) keV | 34.3(10) ms | IT | 200Tl | 7+ | |||||
200m2Tl | 762.0(2) keV | 0.33(5) µs | 5+ | |||||||
201TlMain isotope used in scintigraphy Scintigraphy Scintigraphy is a form of diagnostic test used in nuclear medicine, wherein radioisotopes are taken internally, and the emitted radiation is captured by external detectors to form two-dimensional images... |
81 | 120 | 200.970819(16) | 72.912(17) h | EC Electron capture Electron capture is a process in which a proton-rich nuclide absorbs an inner atomic electron and simultaneously emits a neutrino... |
201Hg | 1/2+ | |||
201mTl | 919.50(9) keV | 2.035(7) ms | IT | 201Tl | (9/2-) | |||||
202Tl | 81 | 121 | 201.972106(16) | 12.23(2) d | β+ | 202Hg | 2- | |||
202mTl | 950.19(10) keV | 572(7) µs | 7+ | |||||||
203Tl | 81 | 122 | 202.9723442(14) | Observationally StableBelieved to undergo α decay to 199Au | 1/2+ | 0.2952(1) | 0.29494-0.29528 | |||
203mTl | 3400(300) keV | 7.7(5) µs | (25/2+) | |||||||
204Tl | 81 | 123 | 203.9738635(13) | 3.78(2) a | β- (97.1%) | 204Pb | 2- | |||
EC (2.9%) | 204Hg | |||||||||
204m1Tl | 1104.0(4) keV | 63(2) µs | (7)+ | |||||||
204m2Tl | 2500(500) keV | 2.6(2) µs | (12-) | |||||||
204m3Tl | 3500(500) keV | 1.6(2) µs | (20+) | |||||||
205TlFinal decay product of 4n+1 decay chain Decay chain In nuclear science, the decay chain refers to the radioactive decay of different discrete radioactive decay products as a chained series of transformations... (the Neptunium series) |
81 | 124 | 204.9744275(14) | Observationally StableBelieved to undergo α decay to 201Au | 1/2+ | 0.7048(1) | 0.70472-0.70506 | |||
205m1Tl | 3290.63(17) keV | 2.6(2) µs | 25/2+ | |||||||
205m2Tl | 4835.6(15) keV | 235(10) ns | (35/2-) | |||||||
206Tl | Radium E | 81 | 125 | 205.9761103(15) | 4.200(17) min | β- | 206Pb | 0- | TraceIntermediate decay product Decay product In nuclear physics, a decay product is the remaining nuclide left over from radioactive decay. Radioactive decay often involves a sequence of steps... of 238U Uranium-238 Uranium-238 is the most common isotope of uranium found in nature. It is not fissile, but is a fertile material: it can capture a slow neutron and after two beta decays become fissile plutonium-239... |
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206mTl | 2643.11(19) keV | 3.74(3) min | IT | 206Tl | (12-) | |||||
207Tl | Actinium C | 81 | 126 | 206.977419(6) | 4.77(2) min | β- | 207Pb | 1/2+ | TraceIntermediate decay product Decay product In nuclear physics, a decay product is the remaining nuclide left over from radioactive decay. Radioactive decay often involves a sequence of steps... of 235U Uranium-235 - References :* .* DOE Fundamentals handbook: Nuclear Physics and Reactor theory , .* A piece of U-235 the size of a grain of rice can produce energy equal to that contained in three tons of coal or fourteen barrels of oil. -External links:* * * one of the earliest articles on U-235 for the... |
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207mTl | 1348.1(3) keV | 1.33(11) s | IT (99.9%) | 207Tl | 11/2- | |||||
β- (.1%) | 207Pb | |||||||||
208Tl | Thorium C | 81 | 127 | 207.9820187(21) | 3.053(4) min | β- | 208Pb | 5(+) | TraceIntermediate decay product Decay product In nuclear physics, a decay product is the remaining nuclide left over from radioactive decay. Radioactive decay often involves a sequence of steps... of 232Th |
|
209Tl | 81 | 128 | 208.985359(8) | 2.161(7) min | β- | 209Pb | (1/2+) | |||
210Tl | Radium C | 81 | 129 | 209.990074(12) | 1.30(3) min | β- (99.991%) | 210Pb | (5+)# | Trace | |
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... (.009%) |
209Pb | |||||||||
211Tl | 81 | 130 | 210.99348(22)# | 1# min [>300 ns] |
1/2+# | |||||
212Tl | 81 | 131 | 211.99823(32)# | 30# s [>300 ns] |
5+# |