Isotopes of xenon

(Redirected from Xenon-126)

Naturally occurring xenon (54Xe) consists of seven stable isotopes and two very long-lived isotopes. Double electron capture has been observed in 124Xe (half-life 1.8 ± 0.5(stat) ± 0.1(sys) ×1022 years)[2] and double beta decay in 136Xe (half-life 2.165 ± 0.016(stat) ± 0.059(sys) ×1021 years),[7] which are among the longest measured half-lives of all nuclides. The isotopes 126Xe and 134Xe are also predicted to undergo double beta decay,[8] but this process has never been observed in these isotopes, so they are considered to be stable.[9][10][11] Beyond these stable forms, 32 artificial unstable isotopes and various isomers have been studied, the longest-lived of which is 127Xe with a half-life of 36.345 days. All other isotopes have half-lives less than 12 days, most less than 20 hours. The shortest-lived isotope, 108Xe,[12] has a half-life of 58 μs, and is the heaviest known nuclide with equal numbers of protons and neutrons. Of known isomers, the longest-lived is 131mXe with a half-life of 11.934 days. 129Xe is produced by beta decay of 129I (half-life: 16 million years); 131mXe, 133Xe, 133mXe, and 135Xe are some of the fission products of both 235U and 239Pu, so are used as indicators of nuclear explosions.

Isotopes of xenon (54Xe)
Main isotopes[1]Decay
abun­dancehalf-life (t1/2)modepro­duct
124Xe0.095%1.8×1022 y[2]εε124Te
125Xesynth16.9 hβ+125I
126Xe0.0890%stable
127Xesynth36.345 dε127I
128Xe1.91%stable
129Xe26.4%stable
130Xe4.07%stable
131Xe21.2%stable
132Xe26.9%stable
133Xesynth5.247 dβ133Cs
134Xe10.4%stable
135Xesynth9.14 hβ135Cs
136Xe8.86%2.165×1021 y[3][4]ββ136Ba
Standard atomic weight Ar°(Xe)

The artificial isotope 135Xe is of considerable significance in the operation of nuclear fission reactors. 135Xe has a huge cross section for thermal neutrons, 2.65×106 barns, so it acts as a neutron absorber or "poison" that can slow or stop the chain reaction after a period of operation. This was discovered in the earliest nuclear reactors built by the American Manhattan Project for plutonium production. Because of this effect, designers must make provisions to increase the reactor's reactivity (the number of neutrons per fission that go on to fission other atoms of nuclear fuel) over the initial value needed to start the chain reaction. For the same reason, the fission products produced in a nuclear explosion and a power plant differ significantly as a large share of 135
Xe
will absorb neutrons in a steady state reactor, while basically none of the 135
I
will have had time to decay to xenon before the explosion of the bomb removes it from the neutron radiation.

Relatively high concentrations of radioactive xenon isotopes are also found emanating from nuclear reactors due to the release of this fission gas from cracked fuel rods or fissioning of uranium in cooling water.[citation needed] The concentrations of these isotopes are still usually low compared to the naturally occurring radioactive noble gas 222Rn.

Because xenon is a tracer for two parent isotopes, Xe isotope ratios in meteorites are a powerful tool for studying the formation of the Solar System. The I-Xe method of dating gives the time elapsed between nucleosynthesis and the condensation of a solid object from the solar nebula (xenon being a gas, only that part of it that formed after condensation will be present inside the object). Xenon isotopes are also a powerful tool for understanding terrestrial differentiation. Excess 129Xe found in carbon dioxide well gases from New Mexico was believed to be from the decay of mantle-derived gases soon after Earth's formation.[13] It has been suggested that the isotopic composition of atmospheric xenon fluctuated prior to the GOE before stabilizing, perhaps as a result of the rise in atmospheric O2.[14]

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]
Spin and
parity
[n 7][n 8]
Natural abundance (mole fraction)
Excitation energyNormal proportionRange of variation
108Xe[12]545458+106
−23
 μs
α104Te0+
109Xe545513(2) msα105Te
110Xe5456109.94428(14)310(190) ms
[105+35
−25
 ms
]
β+110I0+
α106Te
111Xe5457110.94160(33)#740(200) msβ+ (90%)111I5/2+#
α (10%)107Te
112Xe5458111.93562(11)2.7(8) sβ+ (99.1%)112I0+
α (.9%)108Te
113Xe5459112.93334(9)2.74(8) sβ+ (92.98%)113I(5/2+)#
β+, p (7%)112Te
α (.011%)109Te
β+, α (.007%)109Sb
114Xe5460113.927980(12)10.0(4) sβ+114I0+
115Xe5461114.926294(13)18(4) sβ+ (99.65%)115I(5/2+)
β+, p (.34%)114Te
β+, α (3×10−4%)111Sb
116Xe5462115.921581(14)59(2) sβ+116I0+
117Xe5463116.920359(11)61(2) sβ+ (99.99%)117I5/2(+)
β+, p (.0029%)116Te
118Xe5464117.916179(11)3.8(9) minβ+118I0+
119Xe5465118.915411(11)5.8(3) minβ+119I5/2(+)
120Xe5466119.911784(13)40(1) minβ+120I0+
121Xe5467120.911462(12)40.1(20) minβ+121I(5/2+)
122Xe5468121.908368(12)20.1(1) hEC122I0+
123Xe5469122.908482(10)2.08(2) hβ+123I1/2+
123mXe185.18(22) keV5.49(26) μs7/2(−)
124Xe[n 9]5470123.905893(2)1.8(5 (stat), 1 (sys))×1022 y[2]Double EC124Te0+9.52(3)×10−4
125Xe5471124.9063955(20)16.9(2) hβ+125I1/2(+)
125m1Xe252.60(14) keV56.9(9) sIT125Xe9/2(−)
125m2Xe295.86(15) keV0.14(3) μs7/2(+)
126Xe5472125.904274(7)Observationally Stable[n 10]0+8.90(2)×10−4
127Xe5473126.905184(4)36.345(3) dEC127I1/2+
127mXe297.10(8) keV69.2(9) sIT127Xe9/2−
128Xe5474127.9035313(15)Stable0+0.019102(8)
129Xe[n 11]5475128.9047794(8)Stable1/2+0.264006(82)
129mXe236.14(3) keV8.88(2) dIT129Xe11/2−
130Xe5476129.9035080(8)Stable0+0.040710(13)
131Xe[n 12]5477130.9050824(10)Stable3/2+0.212324(30)
131mXe163.930(8) keV11.934(21) dIT131Xe11/2−
132Xe[n 12]5478131.9041535(10)Stable0+0.269086(33)
132mXe2752.27(17) keV8.39(11) msIT132Xe(10+)
133Xe[n 12][n 13]5479132.9059107(26)5.2475(5) dβ133Cs3/2+
133mXe233.221(18) keV2.19(1) dIT133Xe11/2−
134Xe[n 12]5480133.9053945(9)Observationally Stable[n 14]0+0.104357(21)
134m1Xe1965.5(5) keV290(17) msIT134Xe7−
134m2Xe3025.2(15) keV5(1) μs(10+)
135Xe[n 15]5481134.907227(5)9.14(2) hβ135Cs3/2+
135mXe526.551(13) keV15.29(5) minIT (99.99%)135Xe11/2−
β (.004%)135Cs
136Xe[n 9]5482135.907219(8)2.165(16 (stat), 59 (sys))×1021 y[7]ββ136Ba0+0.088573(44)
136mXe1891.703(14) keV2.95(9) μs6+
137Xe5483136.911562(8)3.818(13) minβ137Cs7/2−
138Xe5484137.91395(5)14.08(8) minβ138Cs0+
139Xe5485138.918793(22)39.68(14) sβ139Cs3/2−
140Xe5486139.92164(7)13.60(10) sβ140Cs0+
141Xe5487140.92665(10)1.73(1) sβ (99.45%)141Cs5/2(−#)
β, n (.043%)140Cs
142Xe5488141.92971(11)1.22(2) sβ (99.59%)142Cs0+
β, n (.41%)141Cs
143Xe5489142.93511(21)#0.511(6) sβ143Cs5/2−
144Xe5490143.93851(32)#0.388(7) sβ144Cs0+
β, n143Cs
145Xe5491144.94407(32)#188(4) msβ145Cs(3/2−)#
146Xe5492145.94775(43)#146(6) msβ146Cs0+
147Xe5493146.95356(43)#130(80) ms
[0.10(+10−5) s]
β147Cs3/2−#
β, n146Cs
148Xe549485(15) msβ148Cs0+
149Xe549550 ms#3/2−#
150Xe549640 ms#0+
This table header & footer:
  • The isotopic composition refers to that in air.

Xenon-124

Xenon-124 is an isotope of xenon that undergoes double electron capture to tellurium-124 with a very long half-life of 1.8×1022 years, more than 12 orders of magnitude longer than the age of the universe ((13.799±0.021)×109 years). Such decays have been observed in the XENON1T detector in 2019, and are the rarest processes ever directly observed.[15] (Even slower decays of other nuclei have been measured, but by detecting decay products that have accumulated over billions of years rather than observing them directly.[16])

Xenon-133

xenon-133, 133Xe
General
Symbol133Xe
Namesxenon-133, 133Xe, Xe-133
Protons (Z)54
Neutrons (N)79
Nuclide data
Natural abundancesyn
Half-life (t1/2)5.243(1) d
Isotope mass132.9059107 Da
Spin3/2+
Decay products133Cs
Decay modes
Decay modeDecay energy (MeV)
Beta0.427
Isotopes of xenon
Complete table of nuclides

Xenon-133 (sold as a drug under the brand name Xeneisol, ATC code V09EX03 (WHO)) is an isotope of xenon. It is a radionuclide that is inhaled to assess pulmonary function, and to image the lungs.[17] It is also used to image blood flow, particularly in the brain.[18] 133Xe is also an important fission product.[citation needed] It is discharged to the atmosphere in small quantities by some nuclear power plants.[19]

Xenon-135

Xenon-135 is a radioactive isotope of xenon, produced as a fission product of uranium. It has a half-life of about 9.2 hours and is the most powerful known neutron-absorbing nuclear poison (having a neutron absorption cross-section of 2 million barns[20]). The overall yield of xenon-135 from fission is 6.3%, though most of this results from the radioactive decay of fission-produced tellurium-135 and iodine-135. Xe-135 exerts a significant effect on nuclear reactor operation (xenon pit). It is discharged to the atmosphere in small quantities by some nuclear power plants.[19]

Xenon-136

Xenon-136 is an isotope of xenon that undergoes double beta decay to barium-136 with a very long half-life of 2.11×1021 years, more than 10 orders of magnitude longer than the age of the universe ((13.799±0.021)×109 years). It is being used in the Enriched Xenon Observatory experiment to search for neutrinoless double beta decay.

See also

References