Английская Википедия:Isotopes of thulium
Шаблон:Short description Шаблон:Infobox thulium isotopes Naturally occurring thulium (69Tm) is composed of one stable isotope, 169Tm (100% natural abundance). 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 (t1/2 5.1 minutes), 160mTm (t1/2 74.5 seconds) and 155mTm (t1/2 45 seconds).
The known isotopes of thulium range from 144Tm to 183Tm. The primary decay mode before the most abundant stable isotope, 169Tm, is electron capture, and the primary mode after is beta emission. The primary decay products before 169Tm are erbium isotopes, and the primary products after are ytterbium isotopes. All isotopes of thulium are either radioactive or, in the case of 169Tm, observationally stable, meaning that 169Tm is predicted to be radioactive but no actual decay has been observed.
List of isotopes
Шаблон:Isotopes table |- | 144Tm[1] | style="text-align:right" | 69 | style="text-align:right" | 75 | | Шаблон:Val | p | 143Er | (10+) | | |- | 145Tm | style="text-align:right" | 69 | style="text-align:right" | 76 | 144.97007(43)# | 3.1(3) μs | p | 144Er | (11/2−) | | |- | rowspan=2|146Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 77 | rowspan=2|145.96643(43)# | rowspan=2|240(30) ms | p | 145Er | rowspan=2|(6−) | rowspan=2| | rowspan=2| |- | β+ (rare) | 146Er |- | rowspan=2 style="text-indent:1em" | 146mTm | rowspan=2 colspan="3" style="text-indent:2em" | 71(6) keV | rowspan=2|72(23) ms | p | 145Er | rowspan=2|(10+) | rowspan=2| | rowspan=2| |- | β+ (rare) | 146Er |- | rowspan=2|147Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 78 | rowspan=2|146.96096(32)# | rowspan=2|0.58(3) s | β+ (85%) | 147Er | rowspan=2|11/2− | rowspan=2| | rowspan=2| |- | p (15%) | 146Er |- | style="text-indent:1em" | 147mTm | colspan="3" style="text-indent:2em" | 60(5) keV | 360(40) μs | | | 3/2+ | | |- | 148Tm | style="text-align:right" | 69 | style="text-align:right" | 79 | 147.95784(43)# | 0.7(2) s | β+ | 148Er | (10+) | | |- | style="text-indent:1em" | 148mTm | colspan="3" style="text-indent:2em" | | 0.7 s | | | | | |- | rowspan=2|149Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 80 | rowspan=2|148.95272(32)# | rowspan=2|0.9(2) s | β+ (99.74%) | 149Er | rowspan=2|(11/2−) | rowspan=2| | rowspan=2| |- | β+, p (.26%) | 148Ho |- | 150Tm | style="text-align:right" | 69 | style="text-align:right" | 81 | 149.94996(21)# | 3# s | β+ | 150Er | (1+) | | |- | rowspan=2 style="text-indent:1em" | 150m1Tm | rowspan=2 colspan="3" style="text-indent:2em" | 140(140)# keV | rowspan=2|2.20(6) s | β+ (98.8%) | 150Er | rowspan=2|(6−) | rowspan=2| | rowspan=2| |- | β+, p (1.2%) | 149Ho |- | style="text-indent:1em" | 150m2Tm | colspan="3" style="text-indent:2em" | 810(140)# keV | 5.2(3) ms | | | (10+) | | |- | 151Tm | style="text-align:right" | 69 | style="text-align:right" | 82 | 150.945483(22) | 4.17(10) s | β+ | 151Er | (11/2−) | | |- | style="text-indent:1em" | 151m1Tm | colspan="3" style="text-indent:2em" | 92(7) keV | 6.6(14) s | β+ | 151Er | (1/2+) | | |- | style="text-indent:1em" | 151m2Tm | colspan="3" style="text-indent:2em" | 2655.67(22) keV | 451(24) ns | | | (27/2−) | | |- | 152Tm | style="text-align:right" | 69 | style="text-align:right" | 83 | 151.94442(8) | 8.0(10) s | β+ | 152Er | (2#)− | | |- | style="text-indent:1em" | 152m1Tm | colspan="3" style="text-indent:2em" | 100(80)# keV | 5.2(6) s | β+ | 152Er | (9)+ | | |- | style="text-indent:1em" | 152m2Tm | colspan="3" style="text-indent:2em" | 2555.05(19)+X keV | 294(12) ns | | | (17+) | | |- | rowspan=2|153Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 84 | rowspan=2|152.942012(20) | rowspan=2|1.48(1) s | α (91%) | 149Ho | rowspan=2|(11/2−) | rowspan=2| | rowspan=2| |- | β+ (9%) | 153Er |- | rowspan=2 style="text-indent:1em" | 153mTm | rowspan=2 colspan="3" style="text-indent:2em" | 43.2(2) keV | rowspan=2|2.5(2) s | α (92%) | 149Ho | rowspan=2|(1/2+) | rowspan=2| | rowspan=2| |- | β+ (8%) | 153Er |- | rowspan=2|154Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 85 | rowspan=2|153.941568(15) | rowspan=2|8.1(3) s | β+ (56%) | 154Er | rowspan=2|(2−) | rowspan=2| | rowspan=2| |- | α (44%) | 150Ho |- | rowspan=2 style="text-indent:1em" | 154mTm | rowspan=2 colspan="3" style="text-indent:2em" | 70(50) keV | rowspan=2|3.30(7) s | α (90%) | 150Ho | rowspan=2|(9+) | rowspan=2| | rowspan=2| |- | β+ (10%) | 154Er |- | rowspan=2|155Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 86 | rowspan=2|154.939199(14) | rowspan=2|21.6(2) s | β+ (98.1%) | 155Er | rowspan=2|(11/2−) | rowspan=2| | rowspan=2| |- | α (1.9%) | 151Ho |- | rowspan=2 style="text-indent:1em" | 155mTm | rowspan=2 colspan="3" style="text-indent:2em" | 41(6) keV | rowspan=2|45(3) s | β+ (92%) | 155Er | rowspan=2|(1/2+) | rowspan=2| | rowspan=2| |- | α (8%) | 151Ho |- | rowspan=2|156Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 87 | rowspan=2|155.938980(17) | rowspan=2|83.8(18) s | β+ (99.93%) | 156Er | rowspan=2|2− | rowspan=2| | rowspan=2| |- | α (.064%) | 152Er |- | style="text-indent:1em" | 156mTm | colspan="3" style="text-indent:2em" | 203.6(5) keV | ~400 ns | | | (11−) | | |- | 157Tm | style="text-align:right" | 69 | style="text-align:right" | 88 | 156.93697(3) | 3.63(9) min | β+ | 157Er | 1/2+ | | |- | 158Tm | style="text-align:right" | 69 | style="text-align:right" | 89 | 157.936980(27) | 3.98(6) min | β+ | 158Er | 2− | | |- | style="text-indent:1em" | 158mTm | colspan="3" style="text-indent:2em" | 50(100)# keV | ~20 ns | | | (5+) | | |- | 159Tm | style="text-align:right" | 69 | style="text-align:right" | 90 | 158.93498(3) | 9.13(16) min | β+ | 159Er | 5/2+ | | |- | 160Tm | style="text-align:right" | 69 | style="text-align:right" | 91 | 159.93526(4) | 9.4(3) min | β+ | 160Er | 1− | | |- | rowspan=2 style="text-indent:1em" | 160m1Tm | rowspan=2 colspan="3" style="text-indent:2em" | 70(20) keV | rowspan=2|74.5(15) s | IT (85%) | 160Tm | rowspan=2|5(+#) | rowspan=2| | rowspan=2| |- | β+ (15%) | 160Er |- | style="text-indent:1em" | 160m2Tm | colspan="3" style="text-indent:2em" | 98.2+X keV | ~200 ns | | | (8) | | |- | 161Tm | style="text-align:right" | 69 | style="text-align:right" | 92 | 160.93355(3) | 30.2(8) min | β+ | 161Er | 7/2+ | | |- | style="text-indent:1em" | 161m1Tm | colspan="3" style="text-indent:2em" | 7.4(2) keV | 5# min | | | 1/2+ | | |- | style="text-indent:1em" | 161m2Tm | colspan="3" style="text-indent:2em" | 78.20(3) keV | 110(3) ns | | | 7/2− | | |- | 162Tm | style="text-align:right" | 69 | style="text-align:right" | 93 | 161.933995(28) | 21.70(19) min | β+ | 162Er | 1− | | |- | rowspan=2 style="text-indent:1em" | 162mTm | rowspan=2 colspan="3" style="text-indent:2em" | 130(40) keV | rowspan=2|24.3(17) s | IT (82%) | 162Tm | rowspan=2|5+ | rowspan=2| | rowspan=2| |- | β+ (18%) | 162Er |- | 163Tm | style="text-align:right" | 69 | style="text-align:right" | 94 | 162.932651(6) | 1.810(5) h | β+ | 163Er | 1/2+ | | |- | 164Tm | style="text-align:right" | 69 | style="text-align:right" | 95 | 163.93356(3) | 2.0(1) min | β+ | 164Er | 1+ | | |- | rowspan=2 style="text-indent:1em" | 164mTm | rowspan=2 colspan="3" style="text-indent:2em" | 10(6) keV | rowspan=2|5.1(1) min | IT (80%) | 164Tm | rowspan=2|6− | rowspan=2| | rowspan=2| |- | β+ (20%) | 164Er |- | 165Tm | style="text-align:right" | 69 | style="text-align:right" | 96 | 164.932435(4) | 30.06(3) h | β+ | 165Er | 1/2+ | | |- | 166Tm | style="text-align:right" | 69 | style="text-align:right" | 97 | 165.933554(13) | 7.70(3) h | β+ | 166Er | 2+ | | |- | style="text-indent:1em" | 166mTm | colspan="3" style="text-indent:2em" | 122(8) keV | 340(25) ms | IT | 166Tm | 6− | | |- | 167Tm | style="text-align:right" | 69 | style="text-align:right" | 98 | 166.9328516(29) | 9.25(2) d | EC | 167Er | 1/2+ | | |- | style="text-indent:1em" | 167m1Tm | colspan="3" style="text-indent:2em" | 179.480(19) keV | 1.16(6) μs | | | (7/2)+ | | |- | style="text-indent:1em" | 167m2Tm | colspan="3" style="text-indent:2em" | 292.820(20) keV | 0.9(1) μs | | | 7/2− | | |- | rowspan=2|168Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 99 | rowspan=2|167.934173(3) | rowspan=2|93.1(2) d | β+ (99.99%) | 168Er | rowspan=2|3+ | rowspan=2| | rowspan=2| |- | β− (.01%) | 168Yb |- | 169Tm | style="text-align:right" | 69 | style="text-align:right" | 100 | 168.9342133(27) | colspan=3 align=center|Observationally Stable[n 1] | 1/2+ | 1.0000 | |- | rowspan=2|170Tm | rowspan=2 style="text-align:right" | 69 | rowspan=2 style="text-align:right" | 101 | rowspan=2|169.9358014(27) | rowspan=2|128.6(3) d | β− (99.86%) | 170Yb | rowspan=2|1− | rowspan=2| | rowspan=2| |- | EC (.14%) | 170Er |- | style="text-indent:1em" | 170mTm | colspan="3" style="text-indent:2em" | 183.197(4) keV | 4.12(13) μs | | | (3)+ | | |- | 171Tm | style="text-align:right" | 69 | style="text-align:right" | 102 | 170.9364294(28) | 1.92(1) y | β− | 171Yb | 1/2+ | | |- | style="text-indent:1em" | 171mTm | colspan="3" style="text-indent:2em" | 424.9560(15) keV | 2.60(2) μs | | | 7/2− | | |- | 172Tm | style="text-align:right" | 69 | style="text-align:right" | 103 | 171.938400(6) | 63.6(2) h | β− | 172Yb | 2− | | |- | 173Tm | style="text-align:right" | 69 | style="text-align:right" | 104 | 172.939604(5) | 8.24(8) h | β− | 173Yb | (1/2+) | | |- | style="text-indent:1em" | 173mTm | colspan="3" style="text-indent:2em" | 317.73(20) keV | 10(3) μs | | | (7/2−) | | |- | 174Tm | style="text-align:right" | 69 | style="text-align:right" | 105 | 173.94217(5) | 5.4(1) min | β− | 174Yb | (4)− | | |- | 175Tm | style="text-align:right" | 69 | style="text-align:right" | 106 | 174.94384(5) | 15.2(5) min | β− | 175Yb | (1/2+) | | |- | 176Tm | style="text-align:right" | 69 | style="text-align:right" | 107 | 175.94699(11) | 1.85(3) min | β− | 176Yb | (4+) | | |- | 177Tm | style="text-align:right" | 69 | style="text-align:right" | 108 | 176.94904(32)# | 90(6) s | β− | 177Yb | (7/2−) | | |- | 178Tm | style="text-align:right" | 69 | style="text-align:right" | 109 | 177.95264(43)# | 30# s | β− | 178Yb | | | |- | 179Tm | style="text-align:right" | 69 | style="text-align:right" | 110 | 178.95534(54)# | 20# s | β− | 179Yb | 1/2+# | | |- | 180Tm | style="text-align:right" | 69 | style="text-align:right" | 111 | 179.95902(43)# | 3# s | β− | 180Yb | | | |- | 181Tm | style="text-align:right" | 69 | style="text-align:right" | 112 | 180.96195(54)# | 7# s | β− | 181Yb | 1/2+# | | |- | 182Tm[2] | style="text-align:right" | 69 | style="text-align:right" | 113 | 181.96619(54)# | | | | | | |- | 183Tm[2] | style="text-align:right" | 69 | style="text-align:right" | 114 | | | | | | | Шаблон:Isotopes table/footer
Thulium-170
Шаблон:Main Thulium-170 has a half-life of 128.6 days, decaying by β− decay about 99.87% of the time and electron capture the remaining 0.13% of the time.Шаблон:NUBASE2020 Due to its low-energy X-ray emissions, it has been proposed for radiotherapy[3] and as a source in a radiothermal generator.[4]
References
- Isotope masses from:
- Isotopic compositions and standard atomic masses from:
- Half-life, spin, and isomer data selected from the following sources.
Шаблон:Navbox element isotopes
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