{{Short description|none}} {{Infobox zirconium isotopes}} Naturally occurring zirconium (<sub>40</sub>Zr) is composed of four stable isotopes (one, <sup>94</sup>Zr, may in the future be found radioactive), and one very long-lived radioisotope (<sup>96</sup>Zr), a primordial nuclide that decays via double beta decay with an observed half-life of 2.34 × 10<sup>19</sup> years;<ref>{{cite web |title=List of Adopted Double Beta (ββ) Decay Values |publisher=National Nuclear Data Center, Brookhaven National Laboratory |url=http://www.nndc.bnl.gov/bbdecay/list.html |access-date=2007-09-22 |archive-date=2008-10-12 |archive-url=https://web.archive.org/web/20081012211202/http://www.nndc.bnl.gov/bbdecay/list.html |url-status=dead }}</ref> it can also undergo single beta decay, with a partial half-life of [2.27{{su|p=+0.53|b=−0.36}} (stat) ± 0.27 (syst)] × 10<sup>20</sup> years.<ref name=Barabash>{{cite arXiv |first1=A. S. |last1=Barabash |first2=S. |last2=Evseev |first3=D. |last3=Filosofov |first4=Yu. M. |last4=Gavrilyuk |first5=A. M. |last5=Gangapshev |first6=N. |last6=Gorshkov |first7=V. V. |last7=Kazalov |first8=S. |last8=Kazartsev |first9=T. |last9=Khussainov |first10=V. V. |last10=Kuzminov |first11=A. |last11=Lubashevskiy |first12=D. V. |last12=Ponomarev |first13=S. |last13=Rozov |first14=N. |last14=Temerbulatova |first15=S. |last15=Vasilyev |first16=E. A. |last16=Yakushev |first17=V. I. |last17=Yumatov |date=19 May 2026 |title=First observation of single beta decay of <sup>96</sup>Zr |arxiv=2605.18344 |class=nucl-ex}}</ref> The second most stable radioisotope is <sup>93</sup>Zr, which has a half-life of 1.61 million years. Thirty other radioisotopes have been observed from <sup>77</sup>Zr to <sup>114</sup>Zr; all have half-lives less than a day except for <sup>95</sup>Zr (64.032 days), <sup>88</sup>Zr (83.4 days), and <sup>89</sup>Zr (78.36 hours). The most stable of the isomeric states is just 4.16 minutes for <sup>89m</sup>Zr.
Radioactive isotopes above the theoretically stable mass numbers 90–92 decay by electron emission resulting in niobium isotopes, whereas those below by positron emission or electron capture, resulting in yttrium isotopes.
== List of isotopes == {{Anchor}}
<!--Please delete anchor(s) from the list above or table below if adding a dedicated isotope section(s).-->
{{Isotopes table |symbol=Zr |refs=NUBASE2020, AME2020 II,<!-- updated 2024-12-29 --> IsotopeFRIB, IsomerFRIB |notes=m, unc(), mass#, hl#, hl-nst, spin(), spin#, daughter-st, discoveryname }} |-id=Zirconium-77 | <sup>77</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 37 | 76.96608(43)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/77.pdf 2017] | 100# μs | | | 3/2−# | | |-id=Zirconium-78 | <sup>78</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 38 | 77.95615(43)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/78.pdf 2001] | 50# ms<br/>[>200 ns] | | | 0+ | | |-id=Zirconium-79 | <sup>79</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 39 | 78.94979(32)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/79.pdf 1999] | 56(30) ms | β<sup>+</sup> | <sup>79</sup>Y | 5/2+# | | |-id=Zirconium-80 | <sup>80</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 40 | 79.940818(86)<ref name="hamaker2021">{{cite journal |last1=Hamaker |first1=A. |last2=Leistenschneider |first2=E. |last3=Jain |first3=R. |last4=Bollen |first4=G. |last5=Giuliani |first5=S. A. |last6=Lund |first6=K. |last7=Nazarewicz |first7=W. |last8=Neufcourt |first8=L. |last9=Nicoloff |first9=C. R. |last10=Puentes |first10=D. |last11=Ringle |first11=R. |last12=Sumithrarachchi |first12=C. S. |last13=Yandow |first13=I. T. |title=Precision mass measurement of lightweight self-conjugate nucleus 80Zr |journal=Nature Physics |date=December 2021 |volume=17 |issue=12 |pages=1408–1412 |doi=10.1038/s41567-021-01395-w |osti=1870105 }}</ref> | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/80.pdf 1987] | 4.6(6) s | β<sup>+</sup> | <sup>80</sup>Y | 0+ | | |-id=Zirconium-81 | rowspan=2|<sup>81</sup>Zr | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 41 | rowspan=2|80.938211(11)<ref name="hamaker2021"/> | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/81.pdf 1997] | rowspan=2|5.5(4) s | β<sup>+</sup> (99.88%) | <sup>81</sup>Y | rowspan=2|(3/2−) | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (0.12%) | <sup>80</sup>Sr |-id=Zirconium-82 | <sup>82</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 42 | 81.9317075(17) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/82.pdf 1982] | 32(5) s | β<sup>+</sup> | <sup>82</sup>Y | 0+ | | |-id=Zirconium-83 | rowspan=2|<sup>83</sup>Zr | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 43 | rowspan=2|82.92923591(70)<ref name="hamaker2021"/> | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/83.pdf 1974] | rowspan=2|42(2) s | β<sup>+</sup> | <sup>83</sup>Y | rowspan=2|1/2−# | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (?%) | <sup>82</sup>Sr |-id=Zirconium-83m1 | style="text-indent:1em" | <sup>83m1</sup>Zr | colspan="3" style="text-indent:2em" | 52.72(5) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/83Zr-2.pdf 1988] | 0.53(12) μs | IT | <sup>83</sup>Zr | (5/2−) | | |-id=Zirconium-83m2 | style="text-indent:1em" | <sup>83m2</sup>Zr | colspan="3" style="text-indent:2em" | 77.04(7) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/83Zr-1.pdf 1988] | 1.8(1) μs | IT | <sup>83</sup>Zr | (7/2+) | | |-id=Zirconium-84 | <sup>84</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 44 | 83.9233257(59) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/84.pdf 1977] | 25.8(5) min | β<sup>+</sup> | <sup>84</sup>Y | 0+ | | |-id=Zirconium-85 | <sup>85</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 45 | 84.9214432(69) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/85.pdf 1963] | 7.86(4) min | β<sup>+</sup> | <sup>85</sup>Y | (7/2+) | | |-id=Zirconium-85m | rowspan=2 style="text-indent:1em" | <sup>85m</sup>Zr | rowspan=2 colspan="3" style="text-indent:2em" | 292.2(3) keV | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/85Zr-1.pdf 1976] | rowspan=2|10.9(3) s | IT (?%) | <sup>85</sup>Zr | rowspan=2|1/2−# | rowspan=2| | rowspan=2| |- | β<sup>+</sup> (?%) | <sup>85</sup>Y |-id=Zirconium-86 | <sup>86</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 46 | 85.9162968(38) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/86.pdf 1951] | 16.5(1) h | β<sup>+</sup> | <sup>86</sup>Y | 0+ | | |-id=Zirconium-87 | <sup>87</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 47 | 86.9148173(45) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/87.pdf 1949] | 1.68(1) h | β<sup>+</sup> | <sup>87</sup>Y | 9/2+ | | |-id=Zirconium-87m | style="text-indent:1em" | <sup>87m</sup>Zr | colspan="3" style="text-indent:2em" | 335.84(19) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/87Zr-1.pdf 1972] | 14.0(2) s | IT | <sup>87</sup>Zr | 1/2− | | |- | <sup>88</sup>Zr<ref group="n">Second most powerful known neutron absorber</ref> | style="text-align:right" | 40 | style="text-align:right" | 48 | 87.9102207(58) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/88.pdf 1951] | 83.4(3) d | EC | <sup>88</sup>Y | 0+ | | |-id=Zirconium-88m | style="text-indent:1em" | <sup>88m</sup>Zr | colspan="3" style="text-indent:2em" | 2887.79(6) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/88Zr-1.pdf 1971] | 1.320(25) μs | IT | <sup>88</sup>Zr | 8+ | | |- | <sup>89</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 49 | 88.9088798(30) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/89.pdf 1938] | 78.360(23) h | β<sup>+</sup> | '''<sup>89</sup>Y''' | 9/2+ | | |-id=Zirconium-89m | rowspan=2 style="text-indent:1em" | <sup>89m</sup>Zr | rowspan=2 colspan="3" style="text-indent:2em" | 587.82(10) keV | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/89Zr-1.pdf 1940] | rowspan=2|4.161(10) min | IT (93.77%) | <sup>89</sup>Zr | rowspan=2|1/2− | rowspan=2| | rowspan=2| |- | β<sup>+</sup> (6.23%) | '''<sup>89</sup>Y''' |-id=Zirconium-90 | <sup>90</sup>Zr<ref group="n" name="FP">Fission product</ref> | style="text-align:right" | 40 | style="text-align:right" | 50 | 89.90469876(13) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/90.pdf 1924] | colspan=3 align=center|'''Stable''' | 0+ | 0.5145(4) | |-id=Zirconium-90m1 | style="text-indent:1em" | <sup>90m1</sup>Zr | colspan="3" style="text-indent:2em" | 2319.000(9) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/90Zr-2.pdf 1963] | 809.2(20) ms | IT | '''<sup>90</sup>Zr''' | 5- | | |-id=Zirconium-90m2 | style="text-indent:1em" | <sup>90m2</sup>Zr | colspan="3" style="text-indent:2em" | 3589.418(15) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/90Zr-1.pdf 1959] | 131(4) ns | IT | '''<sup>90</sup>Zr''' | 8+ | | |-id=Zirconium-91 | <sup>91</sup>Zr<ref group="n" name="FP" /> | style="text-align:right" | 40 | style="text-align:right" | 51 | 90.90564021(10) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/91.pdf 1934] | colspan=3 align=center|'''Stable''' | 5/2+ | 0.1122(5) | |-id=Zirconium-91m | style="text-indent:1em" | <sup>91m</sup>Zr | colspan="3" style="text-indent:2em" | 3167.3(4) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/91Zr-1.pdf 1975] | 4.35(14) μs | IT | '''<sup>91</sup>Zr''' | (21/2+) | | |-id=Zirconium-92 | <sup>92</sup>Zr<ref group="n" name="FP" /> | style="text-align:right" | 40 | style="text-align:right" | 52 | 91.90503534(10) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/92.pdf 1924] | colspan=3 align=center|'''Stable''' | 0+ | 0.1715(3) | |- | rowspan=2 | <sup>93</sup>Zr<ref group="n">Long-lived fission product</ref> | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 53 | rowspan=2 | 92.90647066(49) | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/93.pdf 1950] | rowspan=2 | 1.61(5)×10<sup>6</sup> y | β<sup>−</sup> (73%)<ref name="Zr93"/> | <sup>93m1</sup>Nb | rowspan=2 | 5/2+ | rowspan=2 | | rowspan=2 | |- | β<sup>−</sup> (27%)<ref name="Zr93"/> | '''<sup>93</sup>Nb''' |-id=Zirconium-94 | <sup>94</sup>Zr<ref group="n" name="FP" /> | style="text-align:right" | 40 | style="text-align:right" | 54 | 93.90631252(18) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/94.pdf 1924] | colspan=3 align=center|'''Observationally stable'''<ref group="n">Believed to decay by β<sup>−</sup>β<sup>−</sup> to '''<sup>94</sup>Mo''' with a half-life over 1.1×10<sup>17</sup> years</ref> | 0+ | 0.1738(4) | |-id=Zirconium-95 | <sup>95</sup>Zr<ref group="n" name="FP" /> | style="text-align:right" | 40 | style="text-align:right" | 55 | 94.90804028(93) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/95.pdf 1946] | 64.032(6) d | β<sup>−</sup> | <sup>95</sup>Nb | 5/2+ | | |-id=Zirconium-96 | rowspan=2 | <sup>96</sup>Zr<ref group="n" name="FP" /><ref group="n">Primordial radionuclide</ref> | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 56 | rowspan=2 | 95.90827762(12) | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/96.pdf 1934] | rowspan=2 |'''2.34(17)×10<sup>19</sup> y''' | β<sup>−</sup>β<sup>−</sup> | '''<sup>96</sup>Mo''' | rowspan=2 |0+ | rowspan=2 |0.0280(2) | rowspan=2 | |- | β<sup>−</sup> | <sup>96</sup>Nb |-id=Zirconium-97 | <sup>97</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 57 | 96.91096380(13) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/97.pdf 1951] | 16.749(8) h | β<sup>−</sup> | <sup>97m</sup>Nb | 1/2+ | | |-id=Zirconium-97m | style="text-indent:1em" | <sup>97m</sup>Zr | colspan="3" style="text-indent:2em" | 1264.35(16) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/97Zr-1.pdf 1985] | 104.8(17) ns | IT | <sup>97</sup>Zr | 7/2+ | | |-id=Zirconium-98 | <sup>98</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 58 | 97.9127404(91) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/98.pdf 1967] | 30.7(4) s | β<sup>−</sup> | <sup>98</sup>Nb | 0+ | | |-id=Zirconium-98m | style="text-indent:1em" | <sup>98m</sup>Zr | colspan="3" style="text-indent:2em" | 6601.9(11) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/98Zr-1.pdf 2006] | 1.9(2) μs | IT | <sup>98</sup>Zr | (17−) | | |-id=Zirconium-99 | <sup>99</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 59 | 98.916675(11) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/99.pdf 1970] | 2.1(1) s | β<sup>−</sup> | <sup>99m</sup>Nb | 1/2+ | | |-id=Zirconium-99m | style="text-indent:1em" | <sup>99m</sup>Zr | colspan="3" style="text-indent:2em" | 251.96(9) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/99Zr-1.pdf 1970] | 336(5) ns | IT | <sup>99</sup>Zr | 7/2+ | | |-id=Zirconium-100 | <sup>100</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 60 | 99.9180105(87) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/100.pdf 1970] | 7.1(4) s | β<sup>−</sup> | <sup>100</sup>Nb | 0+ | | |-id=Zirconium-101 | <sup>101</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 61 | 100.9214585(89) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/101.pdf 1970] | 2.29(8) s | β<sup>−</sup> | <sup>101</sup>Nb | 3/2+ | | |-id=Zirconium-102 | <sup>102</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 62 | 101.9231542(94) | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/102.pdf 1970] | 2.01(8) s | β<sup>−</sup> | <sup>102</sup>Nb | 0+ | | |-id=Zirconium-103 | rowspan=2|<sup>103</sup>Zr | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 63 | rowspan=2|102.9272041(99) | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/103.pdf 1987] | rowspan=2|1.38(7) s | β<sup>−</sup> (>99%) | <sup>103</sup>Nb | rowspan=2|(5/2−) | rowspan=2| | rowspan=2| |- | β<sup>−</sup>, n (<1%) | <sup>102</sup>Nb |-id=Zirconium-104 | rowspan=2|<sup>104</sup>Zr | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 64 | rowspan=2|103.929449(10) | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/104.pdf 1990] | rowspan=2|920(28) ms | β<sup>−</sup> (>99%) | <sup>104</sup>Nb | rowspan=2|0+ | rowspan=2| | rowspan=2| |- | β<sup>−</sup>, n (<1%) | <sup>103</sup>Nb |-id=Zirconium-105 | rowspan=2|<sup>105</sup>Zr | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 65 | rowspan=2|104.934022(13) | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/105.pdf 1992] | rowspan=2|670(28) ms | β<sup>−</sup> (>98%) | <sup>105</sup>Nb | rowspan=2|1/2+# | rowspan=2| | rowspan=2| |- | β<sup>−</sup>, n (<2%) | <sup>104</sup>Nb |-id=Zirconium-106 | rowspan=2|<sup>106</sup>Zr | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 66 | rowspan=2|105.93693(22)# | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/106.pdf 1994] | rowspan=2|179(6) ms | β<sup>−</sup> (>98%) | <sup>106</sup>Nb | rowspan=2|0+ | rowspan=2| | rowspan=2| |- | β<sup>−</sup>, n (<2%) | <sup>105</sup>Nb |-id=Zirconium-107 | rowspan=2|<sup>107</sup>Zr | rowspan=2 style="text-align:right" | 40 | rowspan=2 style="text-align:right" | 67 | rowspan=2|106.94201(32)# | rowspan=2 style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/107.pdf 1994] | rowspan=2|145.7(24) ms | β<sup>−</sup> (>77%) | <sup>107</sup>Nb | rowspan=2|5/2+# | rowspan=2| | rowspan=2| |- | β<sup>−</sup>, n (<23%) | <sup>106</sup>Nb |-id=Zirconium-108 | <sup>108</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 68 | 107.94530(43)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/108.pdf 1997] | 78.5(20) ms | β<sup>−</sup> | <sup>108</sup>Nb | 0+ | | |-id=Zirconium-108m | style="text-indent:1em" | <sup>108m</sup>Zr | colspan="3" style="text-indent:2em" | 2074.5(8) keV | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/isomers/abstracts/40/108Zr-1.pdf 2011] | 540(30) ns | IT | <sup>108</sup>Zr | (6+) | | |-id=Zirconium-109 | <sup>109</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 69 | 108.95091(54)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/109.pdf 1997] | 56(3) ms | β<sup>−</sup> | <sup>109</sup>Nb | 5/2+# | | |-id=Zirconium-110 | <sup>110</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 70 | 109.95468(54)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/110.pdf 1997] | 37.5(20) ms | β<sup>−</sup> | <sup>110</sup>Nb | 0+ | | |-id=Zirconium-111 | <sup>111</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 71 | 110.96084(64)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/111.pdf 2010] | 24.0(5) ms | β<sup>−</sup> | <sup>111</sup>Nb | 5/2+# | | |-id=Zirconium-112 | <sup>112</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 72 | 111.96520(75)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/112.pdf 2010] | 43(21) ms | β<sup>−</sup> | <sup>112</sup>Nb | 0+ | | |-id=Zirconium-113 | <sup>113</sup>Zr | style="text-align:right" | 40 | style="text-align:right" | 73 | 112.97172(32)# | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/113.pdf 2018] | 15# ms<br />[>550 ns] | | | 3/2+ | | |-id=Zirconium-114 | <sup>114</sup>Zr<ref>{{Cite journal|url=https://journals.aps.org/prc/abstract/10.1103/PhysRevC.103.014614|doi = 10.1103/PhysRevC.103.014614|title = Observation of new neutron-rich isotopes in the vicinity of Zr110|year = 2021|last1 = Sumikama|first1 = T.|last2 = Fukuda|first2 = N.|last3 = Inabe|first3 = N.|last4 = Kameda|first4 = D.|last5 = Kubo|first5 = T.|last6 = Shimizu|first6 = Y.|last7 = Suzuki|first7 = H.|last8 = Takeda|first8 = H.|last9 = Yoshida|first9 = K.|last10 = Baba|first10 = H.|last11 = Browne|first11 = F.|last12 = Bruce|first12 = A. M.|last13 = Carroll|first13 = R.|last14 = Chiga|first14 = N.|last15 = Daido|first15 = R.|last16 = Didierjean|first16 = F.|last17 = Doornenbal|first17 = P.|last18 = Fang|first18 = Y.|last19 = Gey|first19 = G.|last20 = Ideguchi|first20 = E.|last21 = Isobe|first21 = T.|last22 = Lalkovski|first22 = S.|last23 = Li|first23 = Z.|last24 = Lorusso|first24 = G.|last25 = Lozeva|first25 = R.|last26 = Nishibata|first26 = H.|last27 = Nishimura|first27 = S.|last28 = Nishizuka|first28 = I.|last29 = Odahara|first29 = A.|last30 = Patel|first30 = Z.|journal = Physical Review C|volume = 103| issue=1 | article-number=014614 | bibcode=2021PhRvC.103a4614S |s2cid = 234019083|display-authors = 1|hdl = 10261/260248|hdl-access = free}}</ref> | style="text-align:right" | 40 | style="text-align:right" | 74 | | style="text-align:center" | [https://www.nndc.bnl.gov/discovery/abstracts/40/114.pdf 2021] | | | | 0+ | | {{Isotopes table/footer}}
==Zirconium-88== <sup>88</sup>Zr is a radioisotope of zirconium with a half-life of 83.4 days. In January 2019, this isotope was discovered to have a thermal neutron capture cross section of approximately 861,000 barns; this is several orders of magnitude greater than predicted, and greater than that of any other nuclide except xenon-135.<ref name="Zr88">{{cite journal |last1=Shusterman |first1=J.A. |last2=Scielzo |first2=N.D. |last3=Thomas |first3=K.J. |last4=Norman |first4=E.B. |last5=Lapi |first5=S.E. |last6=Loveless |first6=C.S. |last7=Peters |first7=N.J. |last8=Robertson |first8=J.D. |last9=Shaughnessy |first9=D.A. |last10=Tonchev |first10=A.P. |title=The surprisingly large neutron capture cross-section of <sup>88</sup>Zr |journal=Nature |date=2019 |volume=565 |issue=7739 |pages=328–330 |doi=10.1038/s41586-018-0838-z |pmid=30617314 |bibcode=2019Natur.565..328S |osti=1512575 |s2cid=57574387 |url=https://www.osti.gov/biblio/1512575 |url-access=subscription }}</ref>
==Zirconium-89== <sup>89</sup>Zr is a radioisotope of zirconium with a half-life of 78.36 hours, produced by proton irradiation of natural yttrium (<sup>89</sup>Y). Its most prominent gamma photon (99% of decays) has an energy of 909 keV and it emits a positron (as opposed to electron capture) about 23% of decays.<ref>{{NNDC}}</ref> Zirconium-89 is employed in specialized diagnostic applications using positron emission tomography<ref>{{cite journal |last1=Dilworth |first1=Jonathan R. |last2=Pascu |first2=Sofia I. |title=The chemistry of PET imaging with zirconium-89 |journal=Chemical Society Reviews |date=2018 |volume=47 |issue=8 |pages=2554–2571 |doi=10.1039/C7CS00014F|pmid=29557435 }}</ref> imaging, for example, with zirconium-89 labeled antibodies (immuno-PET).<ref>{{cite journal |last1=Van Dongen |first1=GA |last2=Vosjan |first2=MJ |title=Immuno-positron emission tomography: shedding light on clinical antibody therapy |journal= Cancer Biotherapy and Radiopharmaceuticals |date=August 2010 |volume=25 |issue=4 |pages=375–85|doi=10.1089/cbr.2010.0812 |pmid=20707716 }}</ref>
==Zirconium-93== {{Chain yield | 6.70 ± 0.40| 5.58 ± 0.16 | 6.979 ± 0.098| 6.94 ± 0.07| 5.38 ± 0.32 | 6.346 ± 0.044| 6.25 ± 0.04| 5.19 ± 0.31 | 4.913 ± 0.098| 4.53 ± 0.13 | 3.80 ± 0.03 | 3.82 ± 0.03| 3.0 ± 0.3 | 2.98 ± 0.04 | 2.98 ± 0.33| ? |data_ref=<ref>M. B. Chadwick et al, "ENDF/B-VII.1: Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data", Nucl. Data Sheets 112(2011)2887. (accessed at www-nds.iaea.org/exfor/endf.htm)</ref>}}{{Long-lived fission products}}<div style="float:right; margin-left:1em"></div>
'''<sup>93</sup>Zr''' is a radioisotope of zirconium with a half-life of 1.61 million years, decaying through emission of a low-energy beta particle. 73% of decays populate an excited state of niobium-93, which decays with a half-life of 13.9 years (almost entirely by internal conversion, emitting no gamma ray) to the stable ground state of <sup>93</sup>Nb, while the remaining 27% of decays directly populate the ground state.<ref name="Zr93">{{cite journal |last1=Cassette |first1=P. |last2=Chartier |first2=F. |last3=Isnard |first3=H. |last4=Fréchou |first4=C. |last5=Laszak |first5=I. |last6=Degros |first6=J.P. |last7=Bé |first7=M.M. |last8=Lépy |first8=M.C. |last9=Tartes |first9=I. |title=Determination of <sup>93</sup>Zr decay scheme and half-life |date=2010 |journal=Applied Radiation and Isotopes |volume=68 |issue=1 |pages=122–130 |doi=10.1016/j.apradiso.2009.08.011 |pmid=19734052 |bibcode=2010AppRI..68..122C |url=https://www.researchgate.net/publication/26793104}}</ref> It is one of the 7 long-lived fission products. The low specific activity and low energy of its radiation limit the radioactive hazards of this isotope, and its insolubility makes it unlikely to escape a waste repository; all these are shared with palladium-107.
Nuclear fission produces it at a fission yield of 6.3% (thermal neutron fission of <sup>235</sup>U), one of the most abundant fission products. Nuclear reactors usually contain large amounts of zirconium as fuel rod cladding (see zircalloy), and neutron irradiation of <sup>92</sup>Zr also produces some <sup>93</sup>Zr, though this is limited by <sup>92</sup>Zr's low neutron capture cross section of 0.22 barns. Indeed, one of the primary reasons for using zirconium in fuel rod cladding is its low cross section.
<sup>93</sup>Zr also has a low neutron capture cross section of 0.7 barns.<ref>{{cite web |date=2011-12-22 |url=http://www.nndc.bnl.gov/exfor/endf00.jsp |title=ENDF/B-VII.1 Zr-93(n,g) |publisher=National Nuclear Data Center, Brookhaven National Laboratory |access-date=2014-11-20 |archive-date=2009-07-20 |archive-url=https://web.archive.org/web/20090720032108/http://www.nndc.bnl.gov/exfor/endf00.jsp }}</ref><ref>{{cite journal |author=S. Nakamura |display-authors=etal |title=Thermal neutron capture cross-sections of Zirconium-91 and Zirconium-93 by prompt gamma-ray spectroscopy |journal=Journal of Nuclear Science and Technology |volume=44 |issue=1 |pages=21–28| year=2007 |doi=10.1080/18811248.2007.9711252|bibcode=2007JNST...44...21N |s2cid=96087661 }}</ref> Most fission zirconium consists of other isotopes; the other isotope with a significant neutron absorption cross section is <sup>91</sup>Zr with a cross section of 1.24 barns. <sup>93</sup>Zr is a less attractive candidate for disposal by nuclear transmutation than are <sup>99</sup>Tc and <sup>129</sup>I. The isotope could be recycled: if the effect on the neutron economy of {{chem|93|Zr}}'s higher cross section is deemed acceptable, irradiated cladding and fission product zirconium (which are mixed together in most current nuclear reprocessing methods) could be used to form new zircalloy cladding. Once the cladding is inside the reactor, the relatively low level radioactivity can be tolerated, but transport and manufacturing might require precautions not now taken. {{Clear}}
== See also == '''Daughter products other than zirconium''' * Isotopes of molybdenum * Isotopes of niobium * Isotopes of yttrium * Isotopes of strontium
== References == {{Reflist}}
{{Navbox element isotopes}} {{Authority control}}
Category:Isotopes of zirconium Zirconium