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Americium (95Am) is anartificial element, and thus astandard atomic weight cannot be given. Like all artificial elements, it has no knownstable isotopes. The firstisotope to be synthesized was241Am in 1944. The artificial element decays by ejectingalpha particles. Americium has an atomic number of 95 (the number of protons in the nucleus of the americium atom). Despite243
Am being an order of magnitude longer lived than241
Am, the former is harder to obtain than the latter as more of it is present inspent nuclear fuel.
Eighteenradioisotopes of americium, ranging from229Am to247Am with the exception of231Am, have been characterized; another isotope,223Am, has also been reported but is unconfirmed. The most stable isotopes are243Am with ahalf-life of 7,350 years and241Am with a half-life of 432.6 years. All of the remainingradioactive isotopes have half-lives that are less than seven days, the majority of which are shorter than two hours. This element also has fourteenmeta states, with the most stable being242m1Am (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.
| 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: | |||||||||||||||||||
| EC: | Electron capture |
| CD: | Cluster decay |
| IT: | Isomeric transition |
| SF: | Spontaneous fission |
| Actinides[4] bydecay chain | Half-life range (a) | Fission products of235U byyield[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 ahalf-life | |||||
| 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 | |||||
| ||||||||

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 normalionization smoke detectors, which work as anionization chamber. It is a potential fuel for long-lifetimeradioisotope thermoelectric generators, with a half-life longer than that of the standardplutonium-238 (87.7 years) or the alternativestrontium-90 (28.91 years). Itsdecay heat is 0.114 W/g; its rate ofspontaneous fission 1.2/g/s.
The alpha decay of241Am is accompanied by a significant emission ofgamma rays. Its presence in plutonium is determined by the original concentration of241Pu (which decays to it) and the sample age. Older samples of plutonium containing plutonium-241 build up241Am, and chemical separation of americium from such plutonium (e.g. during reworking ofplutonium pits) may be required.

Americium-242m (half-life 141 years) is one of the rare cases, like108mAg,166mHo,180mTa,186mRe,192mIr,210mBi,212mPo and others, where a higher-energynuclear isomer is more stable than its ground state. While that ground state,242Am, decays with half-life 16.02 hours bybeta emission orelectron 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 analpha particle (0.45%, partial half-life 31 ky).
242mAm isfissile with a lowcritical mass, comparable to that of239Pu.[11] It has a very high fissioncross 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 ofnuclear rocket.[12][13]

Americium-243, an alpha emitter, has ahalf-life of 7350 years[1], the longest of all americium isotopes. It is formed in thenuclear fuel cycle mainly byneutron capture onplutonium-242 followed bybeta decay.[14] Production increases exponentially with increasingburnup as a total of 5 neutron captures on238U are required. IfMOX-fuel is used, particularly MOX-fuel high in241
Pu and242
Pu, more americium overall and more243
Am will be produced.
It decays by either emitting analpha particle (decay energy 5.439 MeV)[15] to become239Np, which then quickly goes to239Pu, 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 iscarcinogenic 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 product239Np. The external irradiation risk for the other two americium isotopes (241Am and242mAm) is less than 10% of that for americium-243.[9]