Isotopes of strontium

(Redirected from Strontium-86)

The alkaline earth metal strontium (38Sr) has four stable, naturally occurring isotopes: 84Sr (0.56%), 86Sr (9.86%), 87Sr (7.0%) and 88Sr (82.58%). Its standard atomic weight is 87.62(1).

Isotopes of strontium (38Sr)
Main isotopes[1]Decay
abun­dancehalf-life (t1/2)modepro­duct
82Srsynth25.36 dε82Rb
83Srsynth1.35 dε83Rb
β+83Rb
γ
84Sr0.56%stable
85Srsynth64.84 dε85Rb
γ
86Sr9.86%stable
87Sr7%stable
88Sr82.6%stable
89Srsynth50.52 dβ89Y
90Srtrace28.90 yβ90Y
Standard atomic weight Ar°(Sr)

Only 87Sr is radiogenic; it is produced by decay from the radioactive alkali metal 87Rb, which has a half-life of 4.88 × 1010 years (i.e. more than three times longer than the current age of the universe). Thus, there are two sources of 87Sr in any material: primordial, formed during nucleosynthesis along with 84Sr, 86Sr and 88Sr; and that formed by radioactive decay of 87Rb. The ratio 87Sr/86Sr is the parameter typically reported in geologic investigations;[4] ratios in minerals and rocks have values ranging from about 0.7 to greater than 4.0 (see rubidium–strontium dating). Because strontium has an electron configuration similar to that of calcium, it readily substitutes for calcium in minerals.

In addition to the four stable isotopes, thirty-two unstable isotopes of strontium are known to exist, ranging from 73Sr to 108Sr. Radioactive isotopes of strontium primarily decay into the neighbouring elements yttrium (89Sr and heavier isotopes, via beta minus decay) and rubidium (85Sr, 83Sr and lighter isotopes, via positron emission or electron capture). The longest-lived of these isotopes, and the most relevantly studied, are 90Sr with a half-life of 28.9 years, 85Sr with a half-life of 64.853 days, and 89Sr (89Sr) with a half-life of 50.57 days. All other strontium isotopes have half-lives shorter than 50 days, most under 100 minutes.

Strontium-89 is an artificial radioisotope used in treatment of bone cancer;[5] this application utilizes its chemical similarity to calcium, which allows it to substitute calcium in bone structures. In circumstances where cancer patients have widespread and painful bony metastases, the administration of 89Sr results in the delivery of beta particles directly to the cancerous portions of the bone, where calcium turnover is greatest. Strontium-90 is a by-product of nuclear fission, present in nuclear fallout. The 1986 Chernobyl nuclear accident contaminated a vast area with 90Sr.[6] It causes health problems, as it substitutes for calcium in bone, preventing expulsion from the body. Because it is a long-lived high-energy beta emitter, it is used in SNAP (Systems for Nuclear Auxiliary Power) devices. These devices hold promise for use in spacecraft, remote weather stations, navigational buoys, etc., where a lightweight, long-lived, nuclear-electric power source is required.

In 2020, researchers have found that mirror nuclides 73Sr and 73Br were found to not behave identically to each other as expected.[7]

List of isotopes

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

[n 5]
Daughter
isotope

[n 6][n 7]
Spin and
parity
[n 8][n 4]
Natural abundance (mole fraction)
Excitation energyNormal proportionRange of variation
73Sr383572.96597(64)#>25 msβ+ (>99.9%)73Rb1/2−#
β+, p (<.1%)72Kr
74Sr383673.95631(54)#50# ms [>1.5 μs]β+74Rb0+
75Sr383774.94995(24)88(3) msβ+ (93.5%)75Rb(3/2−)
β+, p (6.5%)74Kr
76Sr383875.94177(4)7.89(7) sβ+76Rb0+
77Sr383976.937945(10)9.0(2) sβ+ (99.75%)77Rb5/2+
β+, p (.25%)76Kr
78Sr384077.932180(8)159(8) sβ+78Rb0+
79Sr384178.929708(9)2.25(10) minβ+79Rb3/2(−)
80Sr384279.924521(7)106.3(15) minβ+80Rb0+
81Sr384380.923212(7)22.3(4) minβ+81Rb1/2−
82Sr384481.918402(6)25.36(3) dEC82Rb0+
83Sr384582.917557(11)32.41(3) hβ+83Rb7/2+
83mSr259.15(9) keV4.95(12) sIT83Sr1/2−
84Sr384683.913425(3)Observationally Stable[n 9]0+0.00560.0055–0.0058
85Sr384784.912933(3)64.853(8) dEC85Rb9/2+
85mSr238.66(6) keV67.63(4) minIT (86.6%)85Sr1/2−
β+ (13.4%)85Rb
86Sr384885.9092607309(91)Stable0+0.09860.0975–0.0999
86mSr2955.68(21) keV455(7) ns8+
87Sr[n 10]384986.9088774970(91)Stable9/2+0.07000.0694–0.0714
87mSr388.533(3) keV2.815(12) hIT (99.7%)87Sr1/2−
EC (.3%)87Rb
88Sr[n 11]385087.9056122571(97)Stable0+0.82580.8229–0.8275
89Sr[n 11]385188.9074507(12)50.57(3) dβ89Y5/2+
90Sr[n 11]385289.907738(3)28.90(3) yβ90Y0+
91Sr385390.910203(5)9.63(5) hβ91Y5/2+
92Sr385491.911038(4)2.66(4) hβ92Y0+
93Sr385592.914026(8)7.423(24) minβ93Y5/2+
94Sr385693.915361(8)75.3(2) sβ94Y0+
95Sr385794.919359(8)23.90(14) sβ95Y1/2+
96Sr385895.921697(29)1.07(1) sβ96Y0+
97Sr385996.926153(21)429(5) msβ (99.95%)97Y1/2+
β, n (.05%)96Y
97m1Sr308.13(11) keV170(10) ns(7/2)+
97m2Sr830.8(2) keV255(10) ns(11/2−)#
98Sr386097.928453(28)0.653(2) sβ (99.75%)98Y0+
β, n (.25%)97Y
99Sr386198.93324(9)0.269(1) sβ (99.9%)99Y3/2+
β, n (.1%)98Y
100Sr386299.93535(14)202(3) msβ (99.02%)100Y0+
β, n (.98%)99Y
101Sr3863100.94052(13)118(3) msβ (97.63%)101Y(5/2−)
β, n (2.37%)100Y
102Sr3864101.94302(12)69(6) msβ (94.5%)102Y0+
β, n (5.5%)101Y
103Sr3865102.94895(54)#50# ms [>300 ns]β103Y
104Sr3866103.95233(75)#30# ms [>300 ns]β104Y0+
105Sr3867104.95858(75)#20# ms [>300 ns]
106Sr[8]3868
107Sr[8]3869
108Sr[9]3870
This table header & footer:

References