Isotopes of erbium

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Isotopes of erbium (68Er)
Main isotopes[1]Decay
Isotopeabun­dancehalf-life (t1/2)modepro­duct
162Er0.139%stable
164Er1.60%stable
165Ersynth10.36 hε165Ho
166Er33.5%stable
167Er22.9%stable
168Er27.0%stable
169Ersynth9.39 dβ169Tm
170Er14.9%stable
Standard atomic weight Ar°(Er)

Naturally occurring erbium (68Er) is composed of six stable isotopes, with 166Er being the most abundant (33.503% natural abundance). Radioisotopes have been characterized with from 145Er to 175Er, all having half-lives less than ten days: the most stable are 169Er (9.39 days), 172Er (49.3 hours), and 160Er (28.58 hours). All of the remaining radioactive isotopes have half-lives that are less than 11 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 149m1Er (t1/2 = 8.9 seconds).

The primary decay mode before the most abundant stable isotope, 166Er, is electron capture to holmium isotopes, and the primary mode after is beta decay to thulium isotopes. All isotopes of erbium are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.

List of isotopes

[edit]

Nuclide
[n 1]
ZNIsotopic mass (Da)[4]
[n 2][n 3]
Half-life[1]
[n 4]
Decay
mode
[1]
[n 5]
Daughter
isotope

[n 6]
Spin and
parity[1]
[n 7][n 4]
Natural abundance (mole fraction)
Excitation energy[n 4]Normal proportion[1]Range of variation
143Er6875142.96655(43)#200# ms9/2−#
144Er6876143.96070(21)#400# ms
[> 200 ns]
0+
145Er6877144.95787(22)#900(200) msβ+145Ho1/2+#
β+, p (?%)144Dy
145mEr205(4)# keV1.0(3) sβ+145Ho(11/2-)
β+, p (?%)144Dy
146Er6878145.952418(7)1.7(6) sβ+146Ho0+
β+, p (?%)145Dy
147Er6879146.94996(4)#3.2(12) sβ+147Ho(1/2+)
β+, p (?%)146Dy
147mEr[n 8]100(50)# keV1.6(2) sβ+147Ho(11/2−)
β+, p (?%)146Dy
148Er6880147.944735(11)#4.6(2) sβ+ (99.85%)148Ho0+
β+, p (0.15%)147Dy
148mEr2.9132(4) MeV13(3) μsIT148Er(10+)
149Er6881148.94231(3)4(2) sβ+ (93%)149Ho(1/2+)
β+, p (7%)148Dy
149m1Er741.8(2) keV8.9(2) sβ+ (96.3%)149Ho(11/2−)
IT (3.5%)149Er
β+, p (0.18%)148Dy
149m2Er2.6111(3) MeV0.61(8) μsIT149Er(19/2+)
149m3Er3.302(7) MeV4.8(1) μsIT149Er(27/2−)
150Er6882149.937916(18)18.5(7) sβ+150Ho0+
150mEr2.7965(5) MeV2.55(10) μsIT150Er10+
151Er6883150.937449(18)23.5(20) sβ+151Ho(7/2−)
151m1Er2.5860(5) MeV580(20) msIT (95.3%)151Er(27/2−)
β+ (4.7%)151Ho
151m2Er10.2866(10) MeV0.42(5) μsIT151Er(65/2-, 61/2+)
152Er6884151.935050(9)10.3(1) sα (90%)148Dy0+
β+ (10%)152Ho
153Er6885152.935086(10)37.1(2) sα (53%)149Dy7/2−
β+ (47%)153Ho
153m1Er2.7982(10) MeV373(9) nsIT153Er(27/2-)
153m2Er5.2481(10) MeV248(32) nsIT153Er(41/2-)
154Er6886153.932791(5)3.73(9) minβ+ (99.53%)154Ho0+
α (0.47%)150Dy
155Er6887154.933216(7)5.3(3) minβ+ (99.978%)155Ho7/2−
α (0.022%)151Dy
156Er6888155.931066(26)19.5(10) minβ+156Ho0+
α (1.2×10−5%)152Dy
157Er6889156.931923(28)18.65(10) minβ+157Ho3/2−
157mEr155.4(3) keV76(6) msIT157Er9/2+
158Er6890157.929893(27)2.29(6) hEC158Ho0+
159Er6891158.930691(4)36(1) minβ+159Ho3/2−
159m1Er182.602(24) keV337(14) nsIT159Er9/2+
159m2Er429.05(3) keV590(60) nsIT159Er11/2−
160Er6892159.929077(26)28.58(9) hEC160Ho0+
161Er6893160.930004(9)3.21(3) hβ+161Ho3/2−
161mEr396.44(4) keV7.5(7) μsIT161Er11/2−
162Er6894161.9287873(8)Observationally Stable[n 9]0+0.00139(5)
162mEr2.02601(13) MeV88(16) nsIT162Er7(-)
163Er6895162.930040(5)75.0(4) minβ+163Ho5/2−
163mEr445.5(6) keV580(100) nsIT163Er(11/2−)
164Er6896163.9292077(8)Observationally Stable[n 10]0+0.01601(3)
165Er6897164.9307335(10)10.36(4) hEC165Ho5/2−
165m1Er551.3(6) keV250(30) nsIT165Er11/2-
165m2Er1.8230(6) MeV370(40) nsIT165Er(19/2)
166Er6898165.9303011(4)Observationally Stable[n 11]0+0.33503(36)
167Er6899166.9320562(3)Observationally Stable[n 12]7/2+0.22869(9)
167mEr207.801(5) keV2.269(6) sIT167Er1/2−
168Er68100167.93237828(28)Observationally Stable[n 13]0+0.26978(18)
168mEr1.0940383(16) MeV109.0(7) nsIT168Er4-
169Er68101168.9345984(3)9.392(18) dβ169Tm1/2−
169m1Er92.05(10) keV285(20) nsIT169Er(5/2)-
169m2Er243.69(17) keV200(10) nsIT169Er7/2+
170Er68102169.9354719(15)Observationally Stable[n 14]0+0.14910(36)
171Er68103170.9380374(15)7.516(2) hβ171Tm5/2−
171mEr198.61(9) keV210(10) nsIT171Er1/2−
172Er68104171.939363(4)49.3(5) hβ172Tm0+
172mEr1.5009(3) MeV579(62) nsIT172Er(6+)
173Er68105172.94240(21)#1.434(17) minβ173Tm(7/2−)
174Er68106173.94423(32)#3.2(2) minβ174Tm0+
174mEr1.1115(7) MeV3.9(3) sIT174Er8-
175Er68107174.94777(43)#1.2(3) minβ175Tm9/2+#
176Er68108175.94994(43)#12# s
[>300 ns]
0+
177Er68109176.95399(54)#8# s
[>300 ns]
1/2−#
178Er68110177.95678(64)#4# s
[>300 ns]
0+
179Er68111178.96127(54)#3# s
[>550 ns)]
3/2−#
180Er68112179.96438(54)#2# s
[>550 ns]
0+
This table header & footer:
  1. ^ mEr – 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. ^ a b c # – 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. ^ Order of ground state and isomer is uncertain.
  9. ^ Believed to undergo α decay to 158Dy or β+β+ to 162Dy with a half-life over 1.40×1014 years
  10. ^ Believed to undergo α decay to 160Dy or β+β+ to 164Dy
  11. ^ Believed to undergo α decay to 162Dy
  12. ^ Believed to undergo α decay to 163Dy
  13. ^ Believed to undergo α decay to 164Dy
  14. ^ Believed to undergo α decay to 166Dy or ββ to 170Yb with a half-life over 4.10×1017 years

See also

[edit]

Daughter products other than erbium

References

[edit]
  1. ^ a b c d e Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3) 030001. doi:10.1088/1674-1137/abddae.
  2. ^ "Standard Atomic Weights: Erbium". CIAAW. 1999.
  3. ^ Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.
  4. ^ Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3) 030003. doi:10.1088/1674-1137/abddaf.

    Isotopes of erbium (68Er)
    Main isotopes[1]Decay
    Isotopeabun­dancehalf-life (t1/2)modepro­duct
    162Er0.139%stable
    164Er1.60%stable
    165Ersynth10.36 hε165Ho
    166Er33.5%stable
    167Er22.9%stable
    168Er27.0%stable
    169Ersynth9.39 dβ169Tm
    170Er14.9%stable
    Standard atomic weight Ar°(Er)
    • 167.259±0.003[2]
    • 167.26±0.01 (abridged)[3]

    Naturally occurring erbium (68Er) is composed of six stable isotopes, with 166Er being the most abundant (33.503% natural abundance). Radioisotopes have been characterized with from 145Er to 175Er, all having half-lives less than ten days: the most stable are 169Er (9.39 days), 172Er (49.3 hours), and 160Er (28.58 hours). All of the remaining radioactive isotopes have half-lives that are less than 11 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 149m1Er (t1/2 = 8.9 seconds).

    The primary decay mode before the most abundant stable isotope, 166Er, is electron capture to holmium isotopes, and the primary mode after is beta decay to thulium isotopes. All isotopes of erbium are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.

    List of isotopes

    Nuclide
    [n 1]
    ZNIsotopic mass (Da)[4]
    [n 2][n 3]
    Half-life[1]
    [n 4]
    Decay
    mode
    [1]
    [n 5]
    Daughter
    isotope

    [n 6]
    Spin and
    parity[1]
    [n 7][n 4]
    Natural abundance (mole fraction)
    Excitation energy[n 4]Normal proportion[1]Range of variation
    143Er6875142.96655(43)#200# ms9/2−#
    144Er6876143.96070(21)#400# ms
    [> 200 ns]
    0+
    145Er6877144.95787(22)#900(200) msβ+145Ho1/2+#
    β+, p (?%)144Dy
    145mEr205(4)# keV1.0(3) sβ+145Ho(11/2-)
    β+, p (?%)144Dy
    146Er6878145.952418(7)1.7(6) sβ+146Ho0+
    β+, p (?%)145Dy
    147Er6879146.94996(4)#3.2(12) sβ+147Ho(1/2+)
    β+, p (?%)146Dy
    147mEr[n 8]100(50)# keV1.6(2) sβ+147Ho(11/2−)
    β+, p (?%)146Dy
    148Er6880147.944735(11)#4.6(2) sβ+ (99.85%)148Ho0+
    β+, p (0.15%)147Dy
    148mEr2.9132(4) MeV13(3) μsIT148Er(10+)
    149Er6881148.94231(3)4(2) sβ+ (93%)149Ho(1/2+)
    β+, p (7%)148Dy
    149m1Er741.8(2) keV8.9(2) sβ+ (96.3%)149Ho(11/2−)
    IT (3.5%)149Er
    β+, p (0.18%)148Dy
    149m2Er2.6111(3) MeV0.61(8) μsIT149Er(19/2+)
    149m3Er3.302(7) MeV4.8(1) μsIT149Er(27/2−)
    150Er6882149.937916(18)18.5(7) sβ+150Ho0+
    150mEr2.7965(5) MeV2.55(10) μsIT150Er10+
    151Er6883150.937449(18)23.5(20) sβ+151Ho(7/2−)
    151m1Er2.5860(5) MeV580(20) msIT (95.3%)151Er(27/2−)
    β+ (4.7%)151Ho
    151m2Er10.2866(10) MeV0.42(5) μsIT151Er(65/2-, 61/2+)
    152Er6884151.935050(9)10.3(1) sα (90%)148Dy0+
    β+ (10%)152Ho
    153Er6885152.935086(10)37.1(2) sα (53%)149Dy7/2−
    β+ (47%)153Ho
    153m1Er2.7982(10) MeV373(9) nsIT153Er(27/2-)
    153m2Er5.2481(10) MeV248(32) nsIT153Er(41/2-)
    154Er6886153.932791(5)3.73(9) minβ+ (99.53%)154Ho0+
    α (0.47%)150Dy
    155Er6887154.933216(7)5.3(3) minβ+ (99.978%)155Ho7/2−
    α (0.022%)151Dy
    156Er6888155.931066(26)19.5(10) minβ+156Ho0+
    α (1.2×10−5%)152Dy
    157Er6889156.931923(28)18.65(10) minβ+157Ho3/2−
    157mEr155.4(3) keV76(6) msIT157Er9/2+
    158Er6890157.929893(27)2.29(6) hEC158Ho0+
    159Er6891158.930691(4)36(1) minβ+159Ho3/2−
    159m1Er182.602(24) keV337(14) nsIT159Er9/2+
    159m2Er429.05(3) keV590(60) nsIT159Er11/2−
    160Er6892159.929077(26)28.58(9) hEC160Ho0+
    161Er6893160.930004(9)3.21(3) hβ+161Ho3/2−
    161mEr396.44(4) keV7.5(7) μsIT161Er11/2−
    162Er6894161.9287873(8)Observationally Stable[n 9]0+0.00139(5)
    162mEr2.02601(13) MeV88(16) nsIT162Er7(-)
    163Er6895162.930040(5)75.0(4) minβ+163Ho5/2−
    163mEr445.5(6) keV580(100) nsIT163Er(11/2−)
    164Er6896163.9292077(8)Observationally Stable[n 10]0+0.01601(3)
    165Er6897164.9307335(10)10.36(4) hEC165Ho5/2−
    165m1Er551.3(6) keV250(30) nsIT165Er11/2-
    165m2Er1.8230(6) MeV370(40) nsIT165Er(19/2)
    166Er6898165.9303011(4)Observationally Stable[n 11]0+0.33503(36)
    167Er6899166.9320562(3)Observationally Stable[n 12]7/2+0.22869(9)
    167mEr207.801(5) keV2.269(6) sIT167Er1/2−
    168Er68100167.93237828(28)Observationally Stable[n 13]0+0.26978(18)
    168mEr1.0940383(16) MeV109.0(7) nsIT168Er4-
    169Er68101168.9345984(3)9.392(18) dβ169Tm1/2−
    169m1Er92.05(10) keV285(20) nsIT169Er(5/2)-
    169m2Er243.69(17) keV200(10) nsIT169Er7/2+
    170Er68102169.9354719(15)Observationally Stable[n 14]0+0.14910(36)
    171Er68103170.9380374(15)7.516(2) hβ171Tm5/2−
    171mEr198.61(9) keV210(10) nsIT171Er1/2−
    172Er68104171.939363(4)49.3(5) hβ172Tm0+
    172mEr1.5009(3) MeV579(62) nsIT172Er(6+)
    173Er68105172.94240(21)#1.434(17) minβ173Tm(7/2−)
    174Er68106173.94423(32)#3.2(2) minβ174Tm0+
    174mEr1.1115(7) MeV3.9(3) sIT174Er8-
    175Er68107174.94777(43)#1.2(3) minβ175Tm9/2+#
    176Er68108175.94994(43)#12# s
    [>300 ns]
    0+
    177Er68109176.95399(54)#8# s
    [>300 ns]
    1/2−#
    178Er68110177.95678(64)#4# s
    [>300 ns]
    0+
    179Er68111178.96127(54)#3# s
    [>550 ns)]
    3/2−#
    180Er68112179.96438(54)#2# s
    [>550 ns]
    0+
    This table header & footer:
    1. ^ mEr – 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. ^ a b c # – 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. ^ Order of ground state and isomer is uncertain.
    9. ^ Believed to undergo α decay to 158Dy or β+β+ to 162Dy with a half-life over 1.40×1014 years
    10. ^ Believed to undergo α decay to 160Dy or β+β+ to 164Dy
    11. ^ Believed to undergo α decay to 162Dy
    12. ^ Believed to undergo α decay to 163Dy
    13. ^ Believed to undergo α decay to 164Dy
    14. ^ Believed to undergo α decay to 166Dy or ββ to 170Yb with a half-life over 4.10×1017 years

    See also

    Daughter products other than erbium

    References

    1. ^ a b c d e Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3) 030001. doi:10.1088/1674-1137/abddae.
    2. ^ "Standard Atomic Weights: Erbium". CIAAW. 1999.
    3. ^ Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.
    4. ^ Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3) 030003. doi:10.1088/1674-1137/abddaf.
    • Isotope masses from:
      • Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3) 030003. doi:10.1088/1674-1137/abddaf.
    • Isotopic compositions and standard atomic masses from:
      • Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3) 030001. doi:10.1088/1674-1137/abddae.
      • de Laeter, John Robert; Böhlke, John Karl; De Bièvre, Paul; Hidaka, Hiroshi; Peiser, H. Steffen; Rosman, Kevin J. R.; Taylor, Philip D. P. (2003). "Atomic weights of the elements. Review 2000 (IUPAC Technical Report)". Pure and Applied Chemistry. 75 (6): 683–800. doi:10.1351/pac200375060683.
      • Wieser, Michael E. (2006). "Atomic weights of the elements 2005 (IUPAC Technical Report)". Pure and Applied Chemistry. 78 (11): 2051–2066. doi:10.1351/pac200678112051.
    • "News & Notices: Standard Atomic Weights Revised". International Union of Pure and Applied Chemistry. 19 October 2005.
    • Half-life, spin, and isomer data selected from the following sources.
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