| |||||||||||||||||||||||||||||||||
Standard atomic weight Ar°(Tl) | |||||||||||||||||||||||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Thallium (81Tl) has 41 isotopes with atomic masses that range from 176 to 216. 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 Tl radioisotopes. All isotopes of thallium are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.
Thallium-202 (half-life 12.23 days) can be made in a cyclotron [4] while thallium-204 (half-life 3.78 years) is made by the neutron activation of stable thallium in a nuclear reactor. [5]
In the fully ionized state, the isotope 205Tl81+ becomes beta-radioactive, undergoing bound-state β− decay to 205Pb81+ with a half-life of 291+33
−27 days, [6] [7] but 203Tl remains stable.
205Tl is the decay product of bismuth-209, an isotope that was once thought to be stable but is now known to undergo alpha decay with an extremely long half-life of 2.01×1019 y. [8] 205Tl is at the end of the neptunium series decay chain.
Nuclide [9] [n 1] | Historic name | Z | N | Isotopic mass (Da) [10] [n 2] [n 3] | Half-life [n 4] | Decay mode [n 5] | Daughter isotope [n 6] | Spin and parity [n 7] [n 4] | Natural abundance (mole fraction) | ||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Excitation energy [n 4] | Normal proportion | Range of variation | |||||||||||||||||
176Tl [11] | 81 | 95 | 176.00059(21)# | 2.4+1.6 −0.7 ms | p (~63%) | 175Hg | (3−, 4−, 5−) | ||||||||||||
α (~37%) | 172Au | ||||||||||||||||||
176mTl | ~671 keV | 290+200 −80 μs | p (~50%) | 175Hg | |||||||||||||||
α (~50%) | 172mAu | ||||||||||||||||||
177Tl [12] | 81 | 96 | 176.996427(27) | 18(5) ms | α (73%) | 173Au | (1/2+) | ||||||||||||
p (27%) | 176Hg | ||||||||||||||||||
177mTl | 807(18) keV | 230(40) μs | p (51%) | 176Hg | (11/2−) | ||||||||||||||
α (49%) | 173Au | ||||||||||||||||||
178Tl [13] | 81 | 97 | 177.99490(12)# | 255(9) ms | α (62%) | 174Au | (4-,5-) | ||||||||||||
β+ (38%) | 178Hg | ||||||||||||||||||
β+, SF (0.15%) | (various) | ||||||||||||||||||
179Tl [14] | 81 | 98 | 178.99109(5) | 437(9) ms | α (60%) | 175Au | (1/2+) | ||||||||||||
β+ (40%) | 179Hg | ||||||||||||||||||
179m1Tl | 825(10)# keV | 1.41(2) ms | α | 175Au | (11/2−) | ||||||||||||||
IT (rare) | 179Tl | ||||||||||||||||||
β+ (rare) | 179Hg | ||||||||||||||||||
179m2Tl | 904.5(9) keV | 119(14) ns | IT | 179Tl | (9/2−) | ||||||||||||||
180Tl [15] | 81 | 99 | 179.98991(13)# | 1.09(1) s | β+ (93%) | 180Hg | 4-# | ||||||||||||
α (7%) | 176Au | ||||||||||||||||||
β+, SF (0.0032%) | 100Ru, 80Kr [16] | ||||||||||||||||||
181Tl [17] | 81 | 100 | 180.986257(10) | 2.9(1) s | β+ (91.4%) | 181Hg | 1/2+# | ||||||||||||
α (8.6%) | 177Au | ||||||||||||||||||
181mTl | 834.9(4) keV | 1.40(3) ms | IT (99.60%) | 181Tl | (9/2−) | ||||||||||||||
α (0.40%) | 177Au | ||||||||||||||||||
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 | 47.1 ms | IT (99.911%) | (10−) | |||||||||||||||
α (.089%) | 180Au | ||||||||||||||||||
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+ | ||||||||||||||||
201Tl [n 8] | 81 | 120 | 200.970819(16) | 72.912(17) h | EC | 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 Stable [n 9] | 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) y | 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+) | ||||||||||||||||
205Tl [n 10] | 81 | 124 | 204.9744275(14) | Observationally Stable [n 11] [n 12] | 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− | Trace [n 13] | ||||||||||
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+ | Trace [n 14] | ||||||||||
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+ | Trace [n 15] | ||||||||||
209Tl | 81 | 128 | 208.985359(8) | 2.161(7) min | β− | 209Pb | 1/2+ | Trace [n 16] | |||||||||||
210Tl | Radium C″ | 81 | 129 | 209.990074(12) | 1.30(3) min | β− (99.991%) | 210Pb | (5+)# | Trace [n 13] | ||||||||||
β−, n (.009%) | 209Pb | ||||||||||||||||||
211Tl | 81 | 130 | 210.993480(50) | 80(16) s | β− (97.8%) | 211Pb | 1/2+ | ||||||||||||
β−, n (2.2%) | 210Pb | ||||||||||||||||||
212Tl | 81 | 131 | 211.998340(220)# | 31(8) s | β− (98.2%) | 212Pb | (5+) | ||||||||||||
β−, n (1.8%) | 211Pb | ||||||||||||||||||
213Tl | 81 | 132 | 213.001915(29) | 24(4) s | β− (92.4%) | 213Pb | 1/2+ | ||||||||||||
β−, n (7.6%) | 212Pb | ||||||||||||||||||
214Tl | 81 | 133 | 214.006940(210)# | 11(2) s | β− (66%) | 214Pb | 5+# | ||||||||||||
β−, n (34%) | 213Pb | ||||||||||||||||||
215Tl | 81 | 134 | 215.010640(320)# | 10(4) s | β− (95.4%) | 215Pb | 1/2+# | ||||||||||||
β−, n (4.6%) | 214Pb | ||||||||||||||||||
216Tl | 81 | 135 | 216.015800(320)# | 6(3) s | β− | 216Pb | 5+# | ||||||||||||
β−, n (<11.5%) | 215Pb | ||||||||||||||||||
This table header & footer: |
EC: | Electron capture |
IT: | Isomeric transition |
n: | Neutron emission |
p: | Proton emission |
Thallium-201 (201Tl) is a synthetic radioisotope of thallium. It has a half-life of 73 hours and decays by electron capture, emitting X-rays (~70–80 keV), and photons of 135 and 167 keV in 10% total abundance. [18] Thallium-201 is synthesized by the neutron activation of stable thallium in a nuclear reactor, [18] [19] or by the 203Tl(p, 3n)201Pb nuclear reaction in cyclotrons, as 201Pb naturally decays to 201Tl afterwards. [20] It is a radiopharmaceutical, as it has good imaging characteristics without excessive patient radiation dose. It is the most popular isotope used for thallium nuclear cardiac stress tests. [21]
Francium (87Fr) has no stable isotopes, thus a standard atomic weight cannot be given. Its most stable isotope is 223Fr with a half-life of 22 minutes, occurring in trace quantities in nature as an intermediate decay product of 235U.
There are 42 isotopes of polonium (84Po). They range in size from 186 to 227 nucleons. They are all radioactive. 210Po with a half-life of 138.376 days has the longest half-life of any naturally-occurring isotope of polonium and is the most common isotope of polonium. It is also the most easily synthesized polonium isotope. 209Po, which does not occur naturally, has the longest half-life of all isotopes of polonium at 124 years. 209Po can be made by using a cyclotron to bombard bismuth with protons, as can 208Po.
There are seven stable isotopes of mercury (80Hg) 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 40 radioisotopes have half-lives that are less than a day. 199Hg and 201Hg are the most often studied NMR-active nuclei, having spin quantum numbers of 1/2 and 3/2 respectively. All isotopes of mercury are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed. These isotopes are predicted to undergo either alpha decay or double beta decay.
Naturally occurring platinum (78Pt) consists of five stable isotopes (192Pt, 194Pt, 195Pt, 196Pt, 198Pt) and one very long-lived (half-life 4.83×1011 years) radioisotope (190Pt). There are also 34 known synthetic radioisotopes, the longest-lived of which is 193Pt with a half-life of 50 years. All other isotopes have half-lives under a year, most under a day. All isotopes of platinum are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed. Platinum-195 is the most abundant isotope.
There are two natural isotopes of iridium (77Ir), and 37 radioisotopes, the most stable radioisotope being 192Ir with a half-life of 73.83 days, and many nuclear isomers, the most stable of which is 192m2Ir with a half-life of 241 years. All other isomers have half-lives under a year, most under a day. All isotopes of iridium are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.
Naturally occurring thulium (69Tm) is composed of one stable isotope, 169Tm. Thirty-nine radioisotopes have been characterized, with the most stable being 171Tm with a half-life of 1.92 years, 170Tm with a half-life of 128.6 days, 168Tm with a half-life of 93.1 days, and 167Tm with a half-life of 9.25 days. All of the remaining radioactive isotopes have half-lives that are less than 64 hours, and the majority of these have half-lives that are less than 2 minutes. This element also has 26 meta states, with the most stable being 164mTm, 160mTm and 155mTm.
Naturally occurring erbium (68Er) is composed of six stable isotopes, with 166Er being the most abundant. Thirty-nine radioisotopes have been characterized with between 74 and 112 neutrons, or 142 to 180 nucleons, with the most stable being 169Er with a half-life of 9.4 days, 172Er with a half-life of 49.3 hours, 160Er with a half-life of 28.58 hours, 165Er with a half-life of 10.36 hours, and 171Er with a half-life of 7.516 hours. All of the remaining radioactive isotopes have half-lives that are less than 3.5 hours, and the majority of these have half-lives that are less than 4 minutes. This element also has numerous meta states, with the most stable being 167mEr.
Natural holmium (67Ho) contains one observationally stable isotope, 165Ho. The below table lists 39 isotopes spanning 140Ho through 178Ho as well as 40 nuclear isomers. Among the known synthetic radioactive isotopes; the most stable one is 163Ho, with a half-life of 4,570 years. All other radioisotopes have half-lives not greater than 1.117 days in their ground states, and most have half-lives under 3 hours.
Naturally occurring praseodymium (59Pr) is composed of one stable isotope, 141Pr. Thirty-eight radioisotopes have been characterized with the most stable being 143Pr, with a half-life of 13.57 days and 142Pr, with a half-life of 19.12 hours. All of the remaining radioactive isotopes have half-lives that are less than six hours and the majority of these have half-lives that are less than 33 seconds. This element also has 15 meta states with the most stable being 138mPr, 142mPr and 134mPr.
Naturally occurring cerium (58Ce) is composed of 4 stable isotopes: 136Ce, 138Ce, 140Ce, and 142Ce, with 140Ce being the most abundant and the only one theoretically stable; 136Ce, 138Ce, and 142Ce are predicted to undergo double beta decay but this process has never been observed. There are 35 radioisotopes that have been characterized, with the most stable being 144Ce, with a half-life of 284.893 days; 139Ce, with a half-life of 137.640 days and 141Ce, with a half-life of 32.501 days. All of the remaining radioactive isotopes have half-lives that are less than 4 days and the majority of these have half-lives that are less than 10 minutes. This element also has 10 meta states.
Naturally occurring silver (47Ag) is composed of the two stable isotopes 107Ag and 109Ag in almost equal proportions, with 107Ag being slightly more abundant. Notably, silver is the only element with all stable istopes having nuclear spins of 1/2. Thus both 107Ag and 109Ag nuclei produce narrow lines in nuclear magnetic resonance spectra.
Naturally occurring rhodium (45Rh) is composed of only one stable isotope, 103Rh. The most stable radioisotopes are 101Rh with a half-life of 3.3 years, 102Rh with a half-life of 207 days, and 99Rh with a half-life of 16.1 days. Thirty other radioisotopes have been characterized with atomic weights ranging from 88.949 u (89Rh) to 121.943 u (122Rh). Most of these have half-lives that are less than an hour except 100Rh and 105Rh. There are also numerous meta states with the most stable being 102mRh (0.141 MeV) with a half-life of about 3.7 years and 101mRh (0.157 MeV) with a half-life of 4.34 days.
Natural yttrium (39Y) is composed of a single isotope yttrium-89. The most stable radioisotopes are 88Y, which has a half-life of 106.6 days, and 91Y, with a half-life of 58.51 days. All the other isotopes have half-lives of less than a day, except 87Y, which has a half-life of 79.8 hours, and 90Y, with 64 hours. The dominant decay mode below the stable 89Y is electron capture and the dominant mode after it is beta emission. Thirty-five unstable isotopes have been characterized.
Naturally occurring vanadium (23V) is composed of one stable isotope 51V and one radioactive isotope 50V with a half-life of 2.71×1017 years. 24 artificial radioisotopes have been characterized (in the range of mass number between 40 and 65) with the most stable being 49V with a half-life of 330 days, and 48V with a half-life of 15.9735 days. All of the remaining radioactive isotopes have half-lives shorter than an hour, the majority of them below 10 seconds, the least stable being 42V with a half-life shorter than 55 nanoseconds, with all of the isotopes lighter than it, and none of the heavier, have unknown half-lives. In 4 isotopes, metastable excited states were found (including 2 metastable states for 60V), which adds up to 5 meta states.
Naturally occurring scandium (21Sc) is composed of one stable isotope, 45Sc. Twenty-seven radioisotopes have been characterized, with the most stable being 46Sc with a half-life of 83.8 days, 47Sc with a half-life of 3.35 days, and 48Sc with a half-life of 43.7 hours and 44Sc with a half-life of 3.97 hours. All the remaining isotopes have half-lives that are less than four hours, and the majority of these have half-lives that are less than two minutes, the least stable being proton unbound 39Sc with a half-life shorter than 300 nanoseconds. This element also has 13 meta states with the most stable being 44m2Sc.
Magnesium (12Mg) naturally occurs in three stable isotopes: 24
Mg, 25
Mg, and 26
Mg. There are 19 radioisotopes that have been discovered, ranging from 18
Mg to 40
Mg. The longest-lived radioisotope is 28
Mg with a half-life of 20.915(9) h. The lighter isotopes mostly decay to isotopes of sodium while the heavier isotopes decay to isotopes of aluminium. The shortest-lived is proton-unbound 18
Mg with a half-life of 4.0(3.4) zeptoseconds.
Berkelium (97Bk) is an artificial element, and thus a standard atomic weight cannot be given. Like all artificial elements, it has no stable isotopes. The first isotope to be synthesized was 243Bk in 1949. There are twenty known radioisotopes, from 233Bk and 233Bk to 253Bk, and six nuclear isomers. The longest-lived isotope is 247Bk with a half-life of 1,380 years.
Fermium (100Fm) is a synthetic element, and thus a standard atomic weight cannot be given. Like all artificial elements, it has no stable isotopes. The first isotope to be discovered was 255Fm in 1952. 250Fm was independently synthesized shortly after the discovery of 255Fm. There are 20 known radioisotopes ranging in atomic mass from 241Fm to 260Fm, and 4 nuclear isomers, 247mFm, 250mFm, 251mFm, and 253mFm. The longest-lived isotope is 257Fm with a half-life of 100.5 days, and the longest-lived isomer is 247mFm with a half-life of 5.1 seconds.
Einsteinium (99Es) is a synthetic element, and thus a standard atomic weight cannot be given. Like all synthetic elements, it has no stable isotopes. The first isotope to be discovered was 253Es in 1952. There are 18 known radioisotopes from 240Es to 257Es, and 4 nuclear isomers. The longest-lived isotope is 252Es with a half-life of 471.7 days, or around 1.293 years.
Mendelevium (101Md) is a synthetic element, and thus a standard atomic weight cannot be given. Like all artificial elements, it has no stable isotopes. The first isotope to be synthesized was 256Md in 1955. There are 17 known radioisotopes, ranging in atomic mass from 244Md to 260Md, and 5 isomers. The longest-lived isotope is 258Md with a half-life of 51.3 days, and the longest-lived isomer is 258mMd with a half-life of 57 minutes.