Isotopes of americium

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Americium (95Am) is an artificial element, and thus a standard atomic weight cannot be given. Like all artificial elements, it has no known stable isotopes. The first isotope to be synthesized was 241Am in 1944. The artificial element decays by ejecting alpha particles. Americium has an atomic number of 95 (the number of protons in the nucleus of the americium atom). Despite 243
Am
being an order of magnitude longer lived than 241
Am
, the former is harder to obtain than the latter as more of it is present in spent nuclear fuel.

Quick facts Main isotopes, Decay ...
Isotopes of americium (95Am)
Main isotopes[1] Decay
Isotope abun­dance half-life (t1/2) mode pro­duct
241Am synth 432.6 y α 237Np
SF
242Am synth 16.02 h β 242Cm
ε 242Pu
242m1Am synth 141 y IT 242Am
α 238Np
243Am synth 7350 y α 239Np
SF
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Eighteen radioisotopes of americium, ranging from 229Am to 247Am with the exception of 231Am, have been characterized; another isotope, 223Am, has also been reported but is unconfirmed. The most stable isotopes are 243Am with a half-life of 7,350 years and 241Am with a half-life of 432.6 years. All of the remaining radioactive isotopes have half-lives that are less than seven days, the majority of which are shorter than two hours. This element also has fourteen meta states, with the most stable being 242m1Am (half-life 141 years). This isomer is unusual in that its half-life is far longer than that of the ground state of the same isotope.

List of isotopes

More information Nuclide, Z ...
Nuclide
[n 1]
Z N Isotopic mass (Da)[2]
[n 2][n 3]
Half-life[1]
Decay
mode
[1]
[n 4]
Daughter
isotope

Spin and
parity[1]
[n 5][n 6]
Excitation energy[n 6]
223Am[n 7] 95 128 223.04584(32)# 10(9) ms α 219Np 9/2–#
229Am 95 134 229.04528(11) 1.8(15) s α 225Np 5/2–#
230Am 95 135 230.04603(15)# 40(9) s β+ (<70%) 230Pu 1–#
β+, SF (>30%) (various)
232Am 95 137 232.04661(32)# 1.31(4) min β+ (97%) 232Pu 1–#
α? (3%) 228Np
β+, SF (0.069%) (various)
233Am 95 138 233.04647(12)# 3.2(8) min β+? (95.5%) 233Pu 5/2–#
α (4.5%) 229Np
234Am 95 139 234.04773(17)# 2.32(8) min β+ (99.95%) 234Pu 0–#
α (0.039%) 230Np
β+, SF (0.0066%) (various)
235Am 95 140 235.04791(6) 10.3(6) min β+ (99.60%) 235Pu 5/2−#
α (0.40%) 231Np
236Am 95 141 236.04943(13)# 3.6(1) min β+ 236Pu 5−
α (4×10−3%) 232Np
236mAm 50(50)# keV 2.9(2) min β+ 236Pu (1−)
237Am 95 142 237.05000(6)# 73.6(8) min β+ (99.975%) 237Pu 5/2−
α (0.025%) 233Np
238Am 95 143 238.05198(6) 98(3) min β+ 238Pu 1+
α (1.0×10−4%) 234Np
238mAm 2500(200)# keV 35(18) μs SF (various)
239Am 95 144 239.0530227(21) 11.9(1) h EC (99.990%) 239Pu 5/2−
α (0.010%) 235Np
239mAm 2500(200) keV 163(12) ns SF (various) (7/2+)
240Am 95 145 240.055298(15) 50.8(3) h β+ 240Pu (3−)
α (1.9×10−4%) 236Np
240mAm 3000(200) keV 940(40) μs SF (various)
241Am 95 146 241.0568273(12) 432.6(6) y α 237Np 5/2−
SF (3.6×10−10%) (various)
241mAm 2200(200) keV 1.2(3) μs SF (various)
242Am 95 147 242.0595474(12) 16.02(2) h β (82.7%) 242Cm 1−
EC (17.3%) 242Pu
242m1Am 48.60(5) keV 141(2) y IT (99.55%) 242Am 5−
α (0.45%) 238Np
SF (<4.7×10−9%) (various)
242m2Am 2200(80) keV 14.0(10) ms SF (various) (2+, 3−)
IT 242Am
243Am 95 148 243.0613799(15) 7350(9) y α 239Np 5/2−
SF (3.7×10−9%) (various)
243mAm 2300(200) keV 5.5(5) μs SF (various)
244Am 95 149 244.0642829(16) 10.01(3) h β 244Cm (6−)
244m1Am 89.3(16) keV 26.13(43) min β (99.96%) 244Cm 1+
EC (0.0364%) 244Pu
244m2Am 2000(200)# keV 0.90(15) ms SF (various)
244m3Am 2200(200)# keV ~6.5 μs SF (various)
245Am 95 150 245.0664528(20) 2.05(1) h β 245Cm 5/2+
245mAm 2400(400)# keV 0.64(6) μs SF (various)
246Am 95 151 246.069774(19)# 39(3) min β 246Cm 7−
246m1Am 30(10)# keV 25.0(2) min β 246Cm 2(−)
246m2Am 2000(800)# keV 73(10) μs SF (various)
247Am 95 152 247.07209(11)# 23.0(13) min β 247Cm 5/2#
This table header & footer:
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  1. mAm  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. () spin value  Indicates spin with weak assignment arguments.
  5. #  Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  6. The discovery of this isotope is uncertain due to disagreements between theoretical predictions and reported experimental data.[3]

Actinides vs fission products

More information Half-life range (a), 4n (Thorium) ...
Actinides[4] by decay chain Half-life
range (a)
Fission products of 235U by yield[5]
4n
(Thorium)
4n + 1
(Neptunium)
4n + 2
(Radium)
4n + 3
(Actinium)
4.5–7% 0.04–1.25% <0.001%
228Ra 4–6 a 155Euþ
248Bk[6] > 9 a
244Cmƒ 241Puƒ 250Cf 227Ac 10–29 a 90Sr 85Kr 113mCdþ
232Uƒ 238Puƒ 243Cmƒ 29–97 a 137Cs 151Smþ 121mSn
249Cfƒ 242mAmƒ 141–351 a

No fission products have a half-life
in the range of 100 a–210 ka ...

241Amƒ 251Cfƒ[7] 430–900 a
226Ra 247Bk 1.3–1.6 ka
240Pu 229Th 246Cmƒ 243Amƒ 4.7–7.4 ka
245Cmƒ 250Cm 8.3–8.5 ka
239Puƒ 24.1 ka
230Th 231Pa 32–76 ka
236Npƒ 233Uƒ 234U 150–250 ka 99Tc 126Sn
248Cm 242Pu 327–375 ka 79Se
1.33 Ma 135Cs
237Npƒ 1.61–6.5 Ma 93Zr 107Pd
236U 247Cmƒ 15–24 Ma 129I
244Pu 80 Ma

... nor beyond 15.7 Ma[8]

232Th 238U 235Uƒ№ 0.7–14.1 Ga
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Americium-241

Americium-241, as used in ionization smoke detectors.

Americium-241 (alpha emitter, half-life 432.6 years) is the most common isotope of americium in nuclear waste.[9] It is the isotope used in normal ionization smoke detectors, which work as an ionization chamber. It is a potential fuel for long-lifetime radioisotope thermoelectric generators, with a half-life longer than that of the standard plutonium-238 (87.7 years) or the alternative strontium-90 (28.91 years). Its decay heat is 0.114 W/g; its rate of spontaneous fission 1.2/g/s.

The alpha decay of 241Am is accompanied by a significant emission of gamma rays. Its presence in plutonium is determined by the original concentration of 241Pu (which decays to it) and the sample age. Older samples of plutonium containing plutonium-241 build up 241Am, and chemical separation of americium from such plutonium (e.g. during reworking of plutonium pits) may be required.

Americium-242m

Transmutation flow between 238Pu and 244Cm in LWR.[10]
Fission percentage is 100 minus shown percentages.
Total rate of transmutation varies greatly by nuclide.
245Cm–248Cm are long-lived with negligible decay.

Americium-242m (half-life 141 years) is one of the rare cases, like 108mAg, 166mHo, 180mTa, 186mRe, 192mIr, 210mBi, 212mPo and others, where a higher-energy nuclear isomer is more stable than its ground state. While that ground state, 242Am, decays with half-life 16.02 hours by beta emission or electron capture, in a typical example of spin-forbiddenness the isomer does not decay by those modes, but falls to the ground state very slowly (99.55% of decays) or emits an alpha particle (0.45%, partial half-life 31 ky).

242mAm is fissile with a low critical mass, comparable to that of 239Pu.[11] It has a very high fission cross section, and is quickly destroyed if it is produced in a nuclear reactor. It has been investigated whether this isotope could be used for a novel type of nuclear rocket.[12][13]

Americium-243

A sample of Am-243

Americium-243, an alpha emitter, has a half-life of 7350 years[1], the longest of all americium isotopes. It is formed in the nuclear fuel cycle mainly by neutron capture on plutonium-242 followed by beta decay.[14] Production increases exponentially with increasing burnup as a total of 5 neutron captures on 238U are required. If MOX-fuel is used, particularly MOX-fuel high in 241
Pu
and 242
Pu
, more americium overall and more 243
Am
will be produced.

It decays by either emitting an alpha particle (decay energy 5.439 MeV)[15] to become 239Np, which then quickly goes to 239Pu, or, very rarely, spontaneous fission. The fission rate is about 60% that of americium-241 or about 0.7/g/s.[16]

As for the other americium isotopes, and more generally for all alpha emitters, 243Am is carcinogenic in case of internal contamination after being inhaled or ingested. 243Am also presents a risk of external irradiation associated with the gamma ray emitted by its short-lived decay product 239Np. The external irradiation risk for the other two americium isotopes (241Am and 242mAm) is less than 10% of that for americium-243.[9]

References

Sources

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