Isotopes of thulium

Last updated
Isotopes of thulium  (69Tm)
Main isotopes [1] Decay
abun­dance half-life (t1/2) mode pro­duct
167Tm synth 9.25 d ε 167Er
168Tmsynth93.1 d β+ 168Er
169Tm100% stable
170Tm synth128.6 d β 170Yb
171Tmsynth1.92 yβ 171Yb
Standard atomic weight Ar°(Tm)

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).

Contents

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

Nuclide
[n 1]
Z N Isotopic mass (Da)
[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 proportionRange of variation
144Tm [4] 69751.9+1.2
−0.5
 μs
p 143Er(10+)
145Tm6976144.97007(43)#3.1(3) μsp144Er(11/2−)
146Tm6977145.96643(43)#240(30) msp145Er(6−)
β+ (rare)146Er
146mTm71(6) keV72(23) msp145Er(10+)
β+ (rare)146Er
147Tm6978146.96096(32)#0.58(3) sβ+ (85%)147Er11/2−
p (15%)146Er
147mTm60(5) keV360(40) μs3/2+
148Tm6979147.95784(43)#0.7(2) sβ+148Er(10+)
148mTm0.7 s
149Tm6980148.95272(32)#0.9(2) sβ+ (99.74%)149Er(11/2−)
β+, p (.26%)148Ho
150Tm6981149.94996(21)#3# sβ+150Er(1+)
150m1Tm140(140)# keV2.20(6) sβ+ (98.8%)150Er(6−)
β+, p (1.2%)149Ho
150m2Tm810(140)# keV5.2(3) ms(10+)
151Tm6982150.945483(22)4.17(10) sβ+151Er(11/2−)
151m1Tm92(7) keV6.6(14) sβ+151Er(1/2+)
151m2Tm2655.67(22) keV451(24) ns(27/2−)
152Tm6983151.94442(8)8.0(10) sβ+152Er(2#)−
152m1Tm100(80)# keV5.2(6) sβ+152Er(9)+
152m2Tm2555.05(19)+X keV294(12) ns(17+)
153Tm6984152.942012(20)1.48(1) s α (91%)149Ho(11/2−)
β+ (9%)153Er
153mTm43.2(2) keV2.5(2) sα (92%)149Ho(1/2+)
β+ (8%)153Er
154Tm6985153.941568(15)8.1(3) sβ+ (56%)154Er(2−)
α (44%)150Ho
154mTm70(50) keV3.30(7) sα (90%)150Ho(9+)
β+ (10%)154Er
155Tm6986154.939199(14)21.6(2) sβ+ (98.1%)155Er(11/2−)
α (1.9%)151Ho
155mTm41(6) keV45(3) sβ+ (92%)155Er(1/2+)
α (8%)151Ho
156Tm6987155.938980(17)83.8(18) sβ+ (99.93%)156Er2−
α (.064%)152Er
156mTm203.6(5) keV~400 ns(11−)
157Tm6988156.93697(3)3.63(9) minβ+157Er1/2+
158Tm6989157.936980(27)3.98(6) minβ+158Er2−
158mTm50(100)# keV~20 ns(5+)
159Tm6990158.93498(3)9.13(16) minβ+159Er5/2+
160Tm6991159.93526(4)9.4(3) minβ+160Er1−
160m1Tm70(20) keV74.5(15) s IT (85%)160Tm5(+#)
β+ (15%)160Er
160m2Tm98.2+X keV~200 ns(8)
161Tm6992160.93355(3)30.2(8) minβ+161Er7/2+
161m1Tm7.4(2) keV5# min1/2+
161m2Tm78.20(3) keV110(3) ns7/2−
162Tm6993161.933995(28)21.70(19) minβ+162Er1−
162mTm130(40) keV24.3(17) sIT (82%)162Tm5+
β+ (18%)162Er
163Tm6994162.932651(6)1.810(5) hβ+163Er1/2+
164Tm6995163.93356(3)2.0(1) minβ+164Er1+
164mTm10(6) keV5.1(1) minIT (80%)164Tm6−
β+ (20%)164Er
165Tm6996164.932435(4)30.06(3) hβ+165Er1/2+
166Tm6997165.933554(13)7.70(3) hβ+166Er2+
166mTm122(8) keV340(25) msIT166Tm6−
167Tm6998166.9328516(29)9.25(2) d EC 167Er1/2+
167m1Tm179.480(19) keV1.16(6) μs(7/2)+
167m2Tm292.820(20) keV0.9(1) μs7/2−
168Tm6999167.934173(3)93.1(2) dβ+ (99.99%)168Er3+
β (.01%)168Yb
169Tm69100168.9342133(27) Observationally Stable [n 8] 1/2+1.0000
170Tm 69101169.9358014(27)128.6(3) dβ (99.86%)170Yb1−
EC (.14%)170Er
170mTm183.197(4) keV4.12(13) μs(3)+
171Tm69102170.9364294(28)1.92(1) yβ171Yb1/2+
171mTm424.9560(15) keV2.60(2) μs7/2−
172Tm69103171.938400(6)63.6(2) hβ172Yb2−
173Tm69104172.939604(5)8.24(8) hβ173Yb(1/2+)
173mTm317.73(20) keV10(3) μs(7/2−)
174Tm69105173.94217(5)5.4(1) minβ174Yb(4)−
175Tm69106174.94384(5)15.2(5) minβ175Yb(1/2+)
176Tm69107175.94699(11)1.85(3) minβ176Yb(4+)
177Tm69108176.94904(32)#90(6) sβ177Yb(7/2−)
178Tm69109177.95264(43)#30# sβ178Yb
179Tm69110178.95534(54)#20# sβ179Yb1/2+#
180Tm69111179.95902(43)#3# sβ180Yb
181Tm69112180.96195(54)#7# sβ181Yb1/2+#
182Tm [5] 69113181.96619(54)#
183Tm [5] 69114
This table header & footer:
  1. mTm  Excited nuclear isomer.
  2. ()  Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
  3. #  Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4. 1 2 3 #  Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  5. Modes of decay:
    EC: Electron capture
    IT: Isomeric transition
    p: Proton emission
  6. Bold symbol as daughter  Daughter product is stable.
  7. () spin value  Indicates spin with weak assignment arguments.
  8. Believed to undergo α decay to 165Ho

Thulium-170

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. [1] Due to its low-energy X-ray emissions, it has been proposed for radiotherapy [6] and as a source in a radiothermal generator. [7]

Related Research Articles

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<span class="mw-page-title-main">Isotopes of lanthanum</span> Nuclides with atomic number of 57 but with different mass numbers

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References

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