Isotopes of mercury
Encyclopedia
There are seven stable isotope
s of mercury
(Hg) with 202Hg being the most abundant (29.86%). The longest-lived radioisotopes are 194Hg with a half-life
of 444 years, and 203Hg with a half-life of 46.612 days. Most of the remaining radioisotopes have half-lives that are less than a day. 199Hg and 201Hg are the most often studied NMR
-active nuclei, having spins of 1/2 and 3/2 respectively.
Mercury-180, producible from thallium-180 was found in 2010 to be capable of an unusual form of spontaneous fission
.
Standard atomic mass: 200.59(2) u
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 of mercury
Mercury (element)
Mercury is a chemical element with the symbol Hg and atomic number 80. It is also known as quicksilver or hydrargyrum...
(Hg) with 202Hg being the most abundant (29.86%). The longest-lived radioisotopes are 194Hg 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 444 years, and 203Hg with a half-life of 46.612 days. Most of the remaining radioisotopes have half-lives that are less than a day. 199Hg and 201Hg are the most often studied NMR
Nuclear magnetic resonance
Nuclear magnetic resonance is a physical phenomenon in which magnetic nuclei in a magnetic field absorb and re-emit electromagnetic radiation...
-active nuclei, having spins of 1/2 and 3/2 respectively.
Mercury-180, producible from thallium-180 was found in 2010 to be capable of an unusual form 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...
.
Standard atomic mass: 200.59(2) 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-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 | |||||||||
171Hg | 80 | 91 | 171.00376(32)# | 80(30) µs [59(+36-16) µs] |
3/2-# | ||||
172Hg | 80 | 92 | 171.99883(22) | 420(240) µs [0.25(+35-9) ms] |
0 | ||||
173Hg | 80 | 93 | 172.99724(22)# | 1.1(4) ms [0.6(+5-2) ms] |
3/2-# | ||||
174Hg | 80 | 94 | 173.992864(21) | 2.0(4) ms [2.1(+18-7) ms] |
0+ | ||||
175Hg | 80 | 95 | 174.99142(11) | 10.8(4) ms | 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... |
171Pt | 5/2-# | ||
176Hg | 80 | 96 | 175.987355(15) | 20.4(15) ms | α (98.6%) | 172Pt | 0+ | ||
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... (1.4%) |
176Au | ||||||||
177Hg | 80 | 97 | 176.98628(8) | 127.3(18) ms | α (85%) | 173Pt | 5/2-# | ||
β+ (15%) | 177Au | ||||||||
178Hg | 80 | 98 | 177.982483(14) | 0.269(3) s | α (70%) | 174Pt | 0+ | ||
β+ (30%) | 178Au | ||||||||
179Hg | 80 | 99 | 178.981834(29) | 1.09(4) s | α (53%) | 175Pt | 5/2-# | ||
β+ (47%) | 179Au | ||||||||
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... (.15%) |
178Pt | ||||||||
180HgWhen produced from 180Tl can also undergo fission to 100Ru and 80Kr | 80 | 100 | 179.978266(15) | 2.58(1) s | β+ (52%) | 180Au | 0+ | ||
α (48%) | 176Pt | ||||||||
80Kr | 100Ru, 80Kr | ||||||||
181Hg | 80 | 101 | 180.977819(17) | 3.6(1) s | β+ (64%) | 181Au | 1/2(-) | ||
α (36%) | 177Pt | ||||||||
β+, p (.014%) | 180Pt | ||||||||
β+, α (9×10−6%) | 177Ir | ||||||||
181mHg | 210(40)# keV | 13/2+ | |||||||
182Hg | 80 | 102 | 181.97469(1) | 10.83(6) s | β+ (84.8%) | 182Au | 0+ | ||
α (15.2%) | 178Pt | ||||||||
β+, p (10−5%) | 181Pt | ||||||||
183Hg | 80 | 103 | 182.974450(9) | 9.4(7) s | β+ (74.5%) | 183Au | 1/2- | ||
α (25.5%) | 179Pt | ||||||||
β+, p (5.6×10−4%) | 182Pt | ||||||||
183m1Hg | 198(14) keV | 13/2+# | |||||||
183m2Hg | 240(40)# keV | 5# s | β+ | 183Au | 13/2+# | ||||
184Hg | 80 | 104 | 183.971713(11) | 30.6(3) s | β+ (98.89%) | 184Au | 0+ | ||
α (1.11%) | 180Pt | ||||||||
185Hg | 80 | 105 | 184.971899(17) | 49.1(10) s | β+ (94%) | 185Au | 1/2- | ||
α (6%) | 181Pt | ||||||||
185mHg | 99.3(5) keV | 21.6(15) s | 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.... (54%) |
185Hg | 13/2+ | ||||
β+ (46%) | 185Au | ||||||||
α (.03%) | 181Pt | ||||||||
186Hg | 80 | 106 | 185.969362(12) | 1.38(6) min | β+ (99.92%) | 186Au | 0+ | ||
α (.016%) | 182Pt | ||||||||
186mHg | 2217.3(4) keV | 82(5) µs | (8-) | ||||||
187Hg | 80 | 107 | 186.969814(15) | 1.9(3) min | β+ | 187Au | 3/2- | ||
α (1.2×10−4%) | 183Pt | ||||||||
187mHg | 59(16) keV | 2.4(3) min | β+ | 187Au | 13/2+ | ||||
α (2.5×10−4%) | 183Pt | ||||||||
188Hg | 80 | 108 | 187.967577(12) | 3.25(15) min | β+ | 188Au | 0+ | ||
α (3.7×10−5%) | 184Pt | ||||||||
188mHg | 2724.3(4) keV | 134(15) ns | (12+) | ||||||
189Hg | 80 | 109 | 188.96819(4) | 7.6(1) min | β+ | 189Au | 3/2- | ||
α (3×10−5%) | 185Pt | ||||||||
189mHg | 80(30) keV | 8.6(1) min | β+ | 189Au | 13/2+ | ||||
α (3×10−5%) | 185Pt | ||||||||
190Hg | 80 | 110 | 189.966322(17) | 20.0(5) min | β+ | 190Au | 0+ | ||
α (5×10−5%) | 186Pt | ||||||||
191Hg | 80 | 111 | 190.967157(24) | 49(10) min | β+ | 191Au | 3/2(-) | ||
191mHg | 128(22) keV | 50.8(15) min | β+ | 191Au | 13/2+ | ||||
192Hg | 80 | 112 | 191.965634(17) | 4.85(20) 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... |
192Au | 0+ | ||
α (4×10−6%) | 188Pt | ||||||||
193Hg | 80 | 113 | 192.966665(17) | 3.80(15) h | β+ | 193Au | 3/2- | ||
193mHg | 140.76(5) keV | 11.8(2) h | β+ (92.9%) | 193Au | 13/2+ | ||||
IT (7.1%) | 193Hg | ||||||||
194Hg | 80 | 114 | 193.965439(13) | 444(77) a | EC | 194Au | 0+ | ||
195Hg | 80 | 115 | 194.966720(25) | 10.53(3) h | β+ | 195Au | 1/2- | ||
195mHg | 176.07(4) keV | 41.6(8) h | IT (54.2%) | 195Hg | 13/2+ | ||||
β+ (45.8%) | 195Au | ||||||||
196Hg | 80 | 116 | 195.965833(3) | Observationally StableBelieved to undergo α decay to 192Pt or β+β+ decay to 196Pt with a half-life over 2.5×1018 years | 0+ | 0.0015(1) | |||
197Hg | 80 | 117 | 196.967213(3) | 64.14(5) h | EC | 197Au | 1/2- | ||
197mHg | 298.93(8) keV | 23.8(1) h | IT (91.4%) | 197Hg | 13/2+ | ||||
EC (8.6%) | 197Au | ||||||||
198Hg | 80 | 118 | 197.9667690(4) | Observationally StableBelieved to undergo α decay to 194Pt | 0+ | 0.0997(20) | |||
199Hg | 80 | 119 | 198.9682799(4) | Observationally StableBelieved to undergo α decay to 195Pt | 1/2- | 0.1687(22) | |||
199mHg | 532.48(10) keV | 42.66(8) min | IT | 199Hg | 13/2+ | ||||
200Hg | 80 | 120 | 199.9683260(4) | Observationally StableBelieved to undergo α decay to 196Pt | 0+ | 0.2310(19) | |||
201Hg | 80 | 121 | 200.9703023(6) | Observationally StableBelieved to undergo α decay to 197Pt | 3/2- | 0.1318(9) | |||
201mHg | 766.22(15) keV | 94(3) µs | 13/2+ | ||||||
202Hg | 80 | 122 | 201.9706430(6) | Observationally StableBelieved to undergo α decay to 198Pt | 0+ | 0.2986(26) | |||
203Hg | 80 | 123 | 202.9728725(18) | 46.595(6) d | β- | 203Tl | 5/2- | ||
203mHg | 933.14(23) keV | 24(4) µs | (13/2+) | ||||||
204Hg | 80 | 124 | 203.9734939(4) | Observationally StableBelieved to undergo α decay to 200Pt or β-β- decay to 204Pb | 0+ | 0.0687(15) | |||
205Hg | 80 | 125 | 204.976073(4) | 5.14(9) min | β- | 205Tl | 1/2- | ||
205mHg | 1556.40(17) keV | 1.09(4) ms | IT | 205Hg | 13/2+ | ||||
206Hg | 80 | 126 | 205.977514(22) | 8.15(10) min | β- | 206Tl | 0+ | ||
207Hg | 80 | 127 | 206.98259(16) | 2.9(2) min | β- | 207Tl | (9/2+) | ||
208Hg | 80 | 128 | 207.98594(32)# | 42(5) min [41(+5-4) min] |
β- | 208Tl | 0+ | ||
209Hg | 80 | 129 | 208.99104(21)# | 37(8) s | 9/2+# | ||||
210Hg | 80 | 130 | 209.99451(32)# | 10# min [>300 ns] |
0+ |