Isotopes of astatine: Difference between revisions

Isotopes of astatine (₈₅At)
α	205Bi
α	206Bi
α	207Bi
	view; talk; edit;

Browse history interactively

← Previous edit Next edit →

Content deleted Content added

VisualWikitext

Inline

Revision as of 15:51, 17 July 2023

Astatine (₈₅At) has 41 known isotopes, all of which are radioactive; their mass numbers range from 188 to 229 (though ¹⁸⁹At is undiscovered).^[2] There are also 24 known metastable excited states. The longest-lived isotope is ²¹⁰At, which has a half-life of 8.1 hours; the longest-lived isotope existing in naturally occurring decay chains is ²¹⁹At with a half-life of 56 seconds.

List of isotopes

Nuclide ^{[n 1]}	Z	N	Isotopic mass (Da) ^{[n 2]}^{[n 3]}	Half-life	Decay mode ^{[n 4]}	Daughter isotope ^{[n 5]}	Spin and parity ^{[n 6]}^{[n 7]}	Isotopic abundance
Nuclide ^{[n 1]}	Excitation energy^{[n 7]}			Half-life	Decay mode ^{[n 4]}	Daughter isotope ^{[n 5]}	Spin and parity ^{[n 6]}^{[n 7]}	Isotopic abundance
¹⁸⁸At^[2]	85	103		190+350 −80 μs	α (~50%)	¹⁸⁴Bi
¹⁸⁸At^[2]	85	103		190+350 −80 μs	p (~50%)	¹⁸⁷Po
¹⁹⁰At^[2]	85	105		1.0+14 −4 ms	α	¹⁸⁶Bi	(10−)
¹⁹¹At^[3]	85	106		1.7+11 −5 ms	α	¹⁸⁷Bi	(1/2+)
^191mAt	50(30) keV			2.1+4 −3 ms	α	¹⁸⁷Bi	(7/2−)
¹⁹²At^[1]	85	107	192.00314(28)	11.5(6) ms	α	¹⁸⁸Bi	3+#
					β⁺ (rare)	¹⁹²Po
					β⁺, SF (0.42%)	(various)
^192mAt	0(40) keV			88(6) ms	α	^188mBi	(9−, 10−)
					β⁺ (rare)	¹⁹²Po
					β⁺, SF (0.42%)	(various)
¹⁹³At^[1]	85	108	192.99984(6)	28+5 −4 ms	α	¹⁸⁹Bi	(1/2+)
^193m1At	8(9) keV			21(5) ms	α	^189m1Bi	(7/2−)
^193m2At	42(9) keV			27+4 −3 ms	IT (76%)	¹⁹³At	(13/2+)
^193m2At	42(9) keV			27+4 −3 ms	α (24%)	^189m2Bi	(13/2+)
¹⁹⁴At^[1]	85	109	193.99873(20)	286(7) ms	α (91.7%#)	¹⁹⁰Bi	(5-)
					β⁺ (8.3%#)	¹⁹⁴Po
					β⁺, SF (0.032%#)	(various)
^194mAt	-20(40) keV			323(7) ms	α (91.7%#)	¹⁹⁰Bi	(10-)
					β⁺ (8.3%#)	¹⁹⁴Po
					β⁺, SF (0.032%#)	(various)
¹⁹⁵At^[1]	85	110	194.996268(10)	290(20) ms	α	^191mBi	(1/2+)
¹⁹⁵At^[1]	85	110	194.996268(10)	290(20) ms	β⁺?	¹⁹⁵Po	(1/2+)
^195mAt	29(7) keV			143(3) ms	α (88%)	¹⁹¹Bi	(7/2-)
					IT (12%)	¹⁹⁵At
					β⁺?	¹⁹⁵Po
¹⁹⁶At^[1]	85	111	195.99579(6)	377(4) ms	α (97.5%)	¹⁹²Bi	(3+)
¹⁹⁶At^[1]	85	111	195.99579(6)	377(4) ms	β⁺ (2.5%)	¹⁹⁶Po	(3+)
^196m1At	−40(40) keV			20# ms	α	^192mBi	(10−)
^196m2At	157.9(1) keV			11(2) μs	IT	¹⁹⁶At	(5+)
¹⁹⁷At^[1]	85	112	196.99319(5)	388.2(5.6) ms	α (96.1%)	¹⁹³Bi	(9/2−)
¹⁹⁷At^[1]	85	112	196.99319(5)	388.2(5.6) ms	β⁺ (3.9%)	¹⁹⁷Po	(9/2−)
^197m1At	45(8) keV			2.0(2) s	α	^193m1Bi	(1/2+)
					IT (<0.004%)	¹⁹⁷At
					β⁺?	¹⁹⁷Po
^197m2At	310.7(2) keV			1.3(2) μs	IT	¹⁹⁷At	(13/2+)
¹⁹⁸At	85	113	197.99284(5)	4.2(3) s	α (94%)	¹⁹⁴Bi	(3+)
¹⁹⁸At	85	113	197.99284(5)	4.2(3) s	β⁺ (6%)	¹⁹⁸Po	(3+)
^198mAt	330(90)# keV			1.0(2) s			(10−)
¹⁹⁹At	85	114	198.99053(5)	6.92(13) s	α (89%)	¹⁹⁵Bi	(9/2−)
¹⁹⁹At	85	114	198.99053(5)	6.92(13) s	β⁺ (11%)	¹⁹⁹Po	(9/2−)
²⁰⁰At	85	115	199.990351(26)	43.2(9) s	α (57%)	¹⁹⁶Bi	(3+)
²⁰⁰At	85	115	199.990351(26)	43.2(9) s	β⁺ (43%)	²⁰⁰Po	(3+)
^200m1At	112.7(30) keV			47(1) s	α (43%)	¹⁹⁶Bi	(7+)
					IT	²⁰⁰At
					β⁺	²⁰⁰Po
^200m2At	344(3) keV			3.5(2) s			(10−)
²⁰¹At	85	116	200.988417(9)	85(3) s	α (71%)	¹⁹⁷Bi	(9/2−)
²⁰¹At	85	116	200.988417(9)	85(3) s	β⁺ (29%)	²⁰¹Po	(9/2−)
²⁰²At	85	117	201.98863(3)	184(1) s	β⁺ (88%)	²⁰²Po	(2, 3)+
²⁰²At	85	117	201.98863(3)	184(1) s	α (12%)	¹⁹⁸Bi	(2, 3)+
^202m1At	190(40) keV			182(2) s			(7+)
^202m2At	580(40) keV			460(50) ms			(10−)
²⁰³At	85	118	202.986942(13)	7.37(13) min	β⁺ (69%)	²⁰³Po	9/2−
²⁰³At	85	118	202.986942(13)	7.37(13) min	α (31%)	¹⁹⁹Bi	9/2−
²⁰⁴At	85	119	203.987251(26)	9.2(2) min	β⁺ (96%)	²⁰⁴Po	7+
²⁰⁴At	85	119	203.987251(26)	9.2(2) min	α (3.8%)	²⁰⁰Bi	7+
^204mAt	587.30(20) keV			108(10) ms	IT	²⁰⁴At	(10−)
²⁰⁵At	85	120	204.986074(16)	26.2(5) min	β⁺ (90%)	²⁰⁵Po	9/2−
²⁰⁵At	85	120	204.986074(16)	26.2(5) min	α (10%)	²⁰¹Bi	9/2−
^205mAt	2339.65(23) keV			7.76(14) μs			29/2+
²⁰⁶At	85	121	205.986667(22)	30.6(13) min	β⁺ (99.11%)	²⁰⁶Po	(5)+
²⁰⁶At	85	121	205.986667(22)	30.6(13) min	α (0.9%)	²⁰²Bi	(5)+
^206mAt	807(3) keV			410(80) ns			(10)−
²⁰⁷At	85	122	206.985784(23)	1.80(4) h	β⁺ (91%)	²⁰⁷Po	9/2−
²⁰⁷At	85	122	206.985784(23)	1.80(4) h	α (8.6%)	²⁰³Bi	9/2−
²⁰⁸At	85	123	207.986590(28)	1.63(3) h	β⁺ (99.5%)	²⁰⁸Po	6+
²⁰⁸At	85	123	207.986590(28)	1.63(3) h	α (0.55%)	²⁰⁴Bi	6+
²⁰⁹At	85	124	208.986173(8)	5.41(5) h	β⁺ (96%)	²⁰⁹Po	9/2−
²⁰⁹At	85	124	208.986173(8)	5.41(5) h	α (4.0%)	²⁰⁵Bi	9/2−
²¹⁰At	85	125	209.987148(8)	8.1(4) h	β⁺ (99.8%)	²¹⁰Po	(5)+
²¹⁰At	85	125	209.987148(8)	8.1(4) h	α (0.18%)	²⁰⁶Bi	(5)+
^210m1At	2549.6(2) keV			482(6) μs			(15)−
^210m2At	4027.7(2) keV			5.66(7) μs			(19)+
²¹¹At	85	126	210.9874963(30)	7.214(7) h	EC (58.2%)	²¹¹Po	9/2−
²¹¹At	85	126	210.9874963(30)	7.214(7) h	α (42%)	²⁰⁷Bi	9/2−
²¹²At	85	127	211.990745(8)	0.314(2) s	α (99.95%)	²⁰⁸Bi	(1−)
					β⁺ (0.05%)	²¹²Po
					β⁻ (2×10⁻⁶%)	²¹²Rn
^212m1At	223(7) keV			0.119(3) s	α (99%)	²⁰⁸Bi	(9−)
^212m1At	223(7) keV			0.119(3) s	IT (1%)	²¹²At	(9−)
^212m2At	4771.6(11) keV			152(5) μs			(25−)
²¹³At	85	128	212.992937(5)	125(6) ns	α	²⁰⁹Bi	9/2−
²¹⁴At	85	129	213.996372(5)	558(10) ns	α	²¹⁰Bi	1−
^214m1At	59(9) keV			265(30) ns
^214m2At	231(6) keV			760(15) ns			9−
²¹⁵At	85	130	214.998653(7)	0.10(2) ms	α	²¹¹Bi	9/2−	Trace^{[n 8]}
²¹⁶At	85	131	216.002423(4)	0.30(3) ms	α (99.99%)	²¹²Bi	1−
					β⁻ (.006%)	²¹⁶Rn
					EC (3×10⁻⁷%)	²¹⁶Po
^216mAt	413(5) keV			100# μs			(9−)
²¹⁷At	85	132	217.004719(5)	32.3(4) ms	α (99.98%)	²¹³Bi	9/2−	Trace^{[n 9]}
²¹⁷At	85	132	217.004719(5)	32.3(4) ms	β⁻ (.012%)	²¹⁷Rn	9/2−	Trace^{[n 9]}
²¹⁸At	85	133	218.008694(12)	1.27(6) s^[4]	α (99.9%)	²¹⁴Bi	1−#	Trace^{[n 10]}
²¹⁸At	85	133	218.008694(12)	1.27(6) s^[4]	β⁻ (0.10%)	²¹⁸Rn	1−#	Trace^{[n 10]}
²¹⁹At	85	134	219.011162(4)	56(3) s	α (97%)	²¹⁵Bi	(9/2−)	Trace^{[n 8]}
²¹⁹At	85	134	219.011162(4)	56(3) s	β⁻ (3.0%)	²¹⁹Rn	(9/2−)	Trace^{[n 8]}
²²⁰At	85	135	220.015433(15)	3.71(4) min	β⁻ (92%)	²²⁰Rn	3(−#)
²²⁰At	85	135	220.015433(15)	3.71(4) min	α (8.0%)	²¹⁶Bi	3(−#)
²²¹At	85	136	221.018017(15)	2.3(2) min	β⁻	²²¹Rn	3/2−#
²²²At	85	137	222.022494(17)	54(10) s	β⁻	²²²Rn
²²³At	85	138	223.025151(15)	50(7) s	β⁻	²²³Rn	3/2−#
²²⁴At	85	139	224.029749(24)	2.5(1.5) min	β⁻	²²⁴Rn	2+#
²²⁵At	85	140	225.03253(32)#	3# s	β⁻	²²⁵Rn	1/2+#
²²⁶At	85	141	226.03721(32)#	7# min	β⁻	²²⁶Rn	2+#
²²⁷At	85	142	227.04018(32)#	5# s	β⁻	²²⁷Rn	1/2+#
²²⁸At	85	143	228.04496(43)#	1# min	β⁻	²²⁸Rn	3+#
²²⁹At	85	144	229.04819(43)#	1# s	β⁻	²²⁹Rn	1/2+#
This table header & footer: view

^ ^mAt – Excited nuclear isomer.
^ ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
^ # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
^ Modes of decay:

EC: Electron capture

IT: Isomeric transition
^ Bold italics symbol as daughter – Daughter product is nearly stable.
^ ( ) spin value – Indicates spin with weak assignment arguments.
^ ^a ^b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
^ ^a ^b Intermediate decay product of ²³⁵U
^ Intermediate decay product of ²³⁷Np
^ Intermediate decay product of ²³⁸U

Alpha decay

Alpha decay characteristics for sample astatine isotopes^[a]
Mass number	Mass excess^[5]	Mass excess of daughter^[5]	Average energy of alpha decay	Half-life^[5]	Probability of alpha decay^[5]	Alpha decay half-life
207	−13.243 MeV	−19.116 MeV	5.873 MeV	1.80 h	8.6%	20.9 h
208	−12.491 MeV	−18.243 MeV	5.752 MeV	1.63 h	0.55%	12.3 d
209	−12.880 MeV	−18.638 MeV	5.758 MeV	5.41 h	4.1%	5.5 d
210	−11.972 MeV	−17.604 MeV	5.632 MeV	8.1 h	0.175%	193 d
211	−11.647 MeV	−17.630 MeV	5.983 MeV	7.21 h	41.8%	17.2 h
212	−8.621 MeV	−16.436 MeV	7.825 MeV	0.31 s	≈100%	0.31 s
213	−6.579 MeV	−15.834 MeV	9.255 MeV	125 ns	100%	125 ns
214	−3.380 MeV	−12.366 MeV	8.986 MeV	558 ns	100%	558 ns
219	10.397 MeV	4.073 MeV	6.324 MeV	56 s	97%	58 s
220	14.350 MeV	8.298 MeV	6.052 MeV	3.71 min	8%	46.4 min
221^[b]	16.810 MeV	11.244 MeV	5.566 MeV	2.3 min	experimentally alpha stable	∞

Astatine has 23 nuclear isomers (nuclei with one or more nucleons – protons or neutrons – in an excited state). A nuclear isomer may also be called a "meta-state"; this means the system has more internal energy than the "ground state" (the state with the lowest possible internal energy), making the former likely to decay into the latter. There may be more than one isomer for each isotope. The most stable of them is astatine-202m1,^[c] which has a half-life of about 3 minutes; this is longer than those of all ground states except those of isotopes 203–211 and 220. The least stable one is astatine-214m1; its half-life of 265 ns is shorter than those of all ground states except that of astatine-213.^[5]

Alpha decay energy follows the same trend as for other heavy elements.^[6] Lighter astatine isotopes have quite high energies of alpha decay, which become lower as the nuclei become heavier. However, astatine-211 has a significantly higher energy than the previous isotope; it has a nucleus with 126 neutrons, and 126 is a magic number (corresponding to a filled neutron shell). Despite having a similar half-life time as the previous isotope (8.1 hours for astatine-210 and 7.2 hours for astatine-211), the alpha decay probability is much higher for the latter: 41.8 percent versus just 0.18 percent.^[5]^[d] The two following isotopes release even more energy, with astatine-213 releasing the highest amount of energy of all astatine isotopes. For this reason, it is the shortest-lived astatine isotope.^[6] Even though heavier astatine isotopes release less energy, no long-lived astatine isotope exists; this happens due to the increasing role of beta decay.^[6] This decay mode is especially important for astatine: as early as 1950, it was postulated that the element has no beta-stable isotopes (i.e. ones that do not undergo beta decay at all),^[7] though nuclear mass measurements reveal that ²¹⁵At is in fact beta-stable, as it has the lowest mass of all isobars with A = 215.^[8] A beta decay mode has been found for all other astatine isotopes except for astatine-213, astatine-214, and astatine-216m.^[5] Among other isotopes: astatine-210 and the lighter isotopes decay by positron emission; astatine-216 and the heavier isotopes undergo beta decay; astatine-212 can decay either way; and astatine-211 decays by electron capture instead.^[5]

The most stable isotope of astatine is astatine-210, which has a half-life of about 8.1 hours. This isotope's primary decay mode is positron emission to the relatively long-lived alpha emitter, polonium-210. In total, only five isotopes of astatine have half-lives exceeding one hour: those between 207 and 211. The least stable ground state isotope is astatine-213, with a half-life of about 125 nanoseconds. It undergoes alpha decay to the extremely long-lived (in practice, stable) isotope bismuth-209.^[5]

References

^ ^a ^b ^c ^d ^e ^f ^g Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae. Cite error: The named reference "NUBASE2020" was defined multiple times with different content (see the help page).
^ ^a ^b ^c Kokkonen, Henna. "Decay properties of the new isotopes 188At and 190At" (PDF). University of Jyväskylä. Retrieved 8 June 2023.
^ Kettunen, H.; Enqvist, T.; Grahn, T.; Greenlees, P.T.; Jones, P.; Julin, R.; Juutinen, S.; Keenan, A.; Kuusiniemi, P.; Leino, M.; Leppänen, A.-P.; Nieminen, P.; Pakarinen, J.; Rahkila, P.; Uusitalo, J. (1 August 2003). "Alpha-decay studies of the new isotopes 191At and 193At" (PDF). The European Physical Journal A - Hadrons and Nuclei. 17 (4): 537–558. doi:10.1140/epja/i2002-10162-1. ISSN 1434-601X. S2CID 122384851. Retrieved 23 June 2023.
^ Cubiss, J. G.; Andreyev, A. N.; Barzakh, A. E.; Andel, B.; Antalic, S.; Cocolios, T. E.; Goodacre, T. Day; Fedorov, D. V.; Fedosseev, V. N.; Ferrer, R.; Fink, D. A.; Gaffney, L. P.; Ghys, L.; Huyse, M.; Kalaninová, Z.; Köster, U.; Marsh, B. A.; Molkanov, P. L.; Rossel, R. E.; Rothe, S.; Seliverstov, M. D.; Sels, S.; Sjödin, A. M.; Stryjczyk, M.; L.Truesdale, V.; Van Beveren, C.; Van Duppen, P.; Wilson, G. L. (2019-06-14). "Fine structure in the α decay of At218". Physical Review C. 99 (6). American Physical Society (APS): 064317. doi:10.1103/physrevc.99.064317. ISSN 2469-9985. S2CID 197508141.
^ ^a ^b ^c ^d ^e ^f ^g ^h ⁱ Audi, Georges; Bersillon, Olivier; Blachot, Jean; Wapstra, Aaldert Hendrik (2003), "The NUBASE evaluation of nuclear and decay properties", Nuclear Physics A, 729: 3–128, Bibcode:2003NuPhA.729....3A, doi:10.1016/j.nuclphysa.2003.11.001
^ ^a ^b ^c Lavrukhina & Pozdnyakov 1966, p. 232.
^ Rankama, Kalervo (1956). Isotope geology (2nd ed.). Pergamon Press. p. 403. ISBN 978-0-470-70800-2.
^ Audi, G.; Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S. (2017). "The NUBASE2016 evaluation of nuclear properties" (PDF). Chinese Physics C. 41 (3): 030001. Bibcode:2017ChPhC..41c0001A. doi:10.1088/1674-1137/41/3/030001.

Lavrukhina, Avgusta Konstantinovna; Pozdnyakov, Aleksandr Aleksandrovich (1966). Аналитическая химия технеция, прометия, астатина и франция [Analytical Chemistry of Technetium, Promethium, Astatine, and Francium] (in Russian). Nauka.
Isotope masses from:
- Audi, Georges; Bersillon, Olivier; Blachot, Jean; Wapstra, Aaldert Hendrik (2003), "The NUBASE evaluation of nuclear and decay properties", Nuclear Physics A, 729: 3–128, Bibcode:2003NuPhA.729....3A, doi:10.1016/j.nuclphysa.2003.11.001
Isotopic compositions and standard atomic masses from:
- de Laeter, John Robert; Böhlke, John Karl; De Bièvre, Paul; Hidaka, Hiroshi; Peiser, H. Steffen; Rosman, Kevin J. R.; Taylor, Philip D. P. (2003). "Atomic weights of the elements. Review 2000 (IUPAC Technical Report)". Pure and Applied Chemistry. 75 (6): 683–800. doi:10.1351/pac200375060683.
- Wieser, Michael E. (2006). "Atomic weights of the elements 2005 (IUPAC Technical Report)". Pure and Applied Chemistry. 78 (11): 2051–2066. doi:10.1351/pac200678112051.
"News & Notices: Standard Atomic Weights Revised". International Union of Pure and Applied Chemistry. 19 October 2005.
Half-life, spin, and isomer data selected from the following sources.
- Audi, Georges; Bersillon, Olivier; Blachot, Jean; Wapstra, Aaldert Hendrik (2003), "The NUBASE evaluation of nuclear and decay properties", Nuclear Physics A, 729: 3–128, Bibcode:2003NuPhA.729....3A, doi:10.1016/j.nuclphysa.2003.11.001
- National Nuclear Data Center. "NuDat 2.x database". Brookhaven National Laboratory.
- Holden, Norman E. (2004). "11. Table of the Isotopes". In Lide, David R. (ed.). CRC Handbook of Chemistry and Physics (85th ed.). Boca Raton, Florida: CRC Press. ISBN 978-0-8493-0485-9.

[3] At – Excited nuclear isomer.

[4] ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.

[TMS-5] # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).

[6] Modes of decay:

EC: Electron capture

IT: Isomeric transition

[7] Bold italics symbol as daughter – Daughter product is nearly stable.

[8] ( ) spin value – Indicates spin with weak assignment arguments.

[TNN-9] # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

[as-11] Intermediate decay product of ²³⁵U

[12] Intermediate decay product of ²³⁷Np

[14] Intermediate decay product of ²³⁸U

[15] In the table, under the words "mass excess", the energy equivalents are given rather than the real mass excesses; "mass excess daughter" stands for the energy equivalent of the mass excess sum of the daughter of the isotope and the alpha particle; "alpha decay half-life" refers to the half-life if decay modes other than alpha are omitted.

[17] Since astatine-221 has not been shown to undergo alpha decay, the alpha decay energy is theoretical. The value for mass excess is calculated rather than measured.

[18] "m1" means that this state of the isotope is the next possible one above – energy greater than – the ground state. "m2" and similar designations refer to further higher energy states. The number may be dropped if there is only one well-established meta state, such as astatine-216m. Note that other designation techniques exist.

[20] This means that if decay modes other than alpha are omitted, then astatine-210 has an alpha half-life of 4,628.6 hours (128.9 days) and astatine-211 has one of 17.2 hours (0.9 days). Therefore, astatine-211 is less stable toward alpha decay than the lighter isotope, and is more likely to undergo alpha decay in the same time period.

[NUBASE2020-1] ^ ^a ^b ^c ^d ^e ^f ^g Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae. Cite error: The named reference "NUBASE2020" was defined multiple times with different content (see the help page).

[At188190-2] Kokkonen, Henna. "Decay properties of the new isotopes 188At and 190At" (PDF). University of Jyväskylä. Retrieved 8 June 2023.

[10] Kettunen, H.; Enqvist, T.; Grahn, T.; Greenlees, P.T.; Jones, P.; Julin, R.; Juutinen, S.; Keenan, A.; Kuusiniemi, P.; Leino, M.; Leppänen, A.-P.; Nieminen, P.; Pakarinen, J.; Rahkila, P.; Uusitalo, J. (1 August 2003). "Alpha-decay studies of the new isotopes 191At and 193At" (PDF). The European Physical Journal A - Hadrons and Nuclei. 17 (4): 537–558. doi:10.1140/epja/i2002-10162-1. ISSN 1434-601X. S2CID 122384851. Retrieved 23 June 2023.

[13] Cubiss, J. G.; Andreyev, A. N.; Barzakh, A. E.; Andel, B.; Antalic, S.; Cocolios, T. E.; Goodacre, T. Day; Fedorov, D. V.; Fedosseev, V. N.; Ferrer, R.; Fink, D. A.; Gaffney, L. P.; Ghys, L.; Huyse, M.; Kalaninová, Z.; Köster, U.; Marsh, B. A.; Molkanov, P. L.; Rossel, R. E.; Rothe, S.; Seliverstov, M. D.; Sels, S.; Sjödin, A. M.; Stryjczyk, M.; L.Truesdale, V.; Van Beveren, C.; Van Duppen, P.; Wilson, G. L. (2019-06-14). "Fine structure in the α decay of At218". Physical Review C. 99 (6). American Physical Society (APS): 064317. doi:10.1103/physrevc.99.064317. ISSN 2469-9985. S2CID 197508141.

[NUBASE_2003-16] ^ ^a ^b ^c ^d ^e ^f ^g ^h ⁱ Audi, Georges; Bersillon, Olivier; Blachot, Jean; Wapstra, Aaldert Hendrik (2003), "The NUBASE evaluation of nuclear and decay properties", Nuclear Physics A, 729: 3–128, Bibcode:2003NuPhA.729....3A, doi:10.1016/j.nuclphysa.2003.11.001

[FOOTNOTELavrukhinaPozdnyakov1966232-19] Lavrukhina & Pozdnyakov 1966, p. 232.

[At-Kalervo-21] Rankama, Kalervo (1956). Isotope geology (2nd ed.). Pergamon Press. p. 403. ISBN 978-0-470-70800-2.

[NUBASE2016-22] Audi, G.; Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S. (2017). "The NUBASE2016 evaluation of nuclear properties" (PDF). Chinese Physics C. 41 (3): 030001. Bibcode:2017ChPhC..41c0001A. doi:10.1088/1674-1137/41/3/030001.

[1]

[2]

[n 1]

[n 2]

[n 3]

[n 4]

[n 5]

[n 6]

[n 7]

[3]

[n 8]

[n 9]

[4]

[n 10]

[a]

[5]

[b]

[c]

[6]

[d]

[7]

[8]

@@ Line 33: / Line 33: @@
 |
 |-
-| <sup>191</sup>At<ref>{{cite journal |last1=Kettunen |first1=H. |last2=Enqvist |first2=T. |last3=Grahn |first3=T. |last4=Greenlees |first4=P.T. |last5=Jones |first5=P. |last6=Julin |first6=R. |last7=Juutinen |first7=S. |last8=Keenan |first8=A. |last9=Kuusiniemi |first9=P. |last10=Leino |first10=M. |last11=Leppänen |first11=A.-P. |last12=Nieminen |first12=P. |last13=Pakarinen |first13=J. |last14=Rahkila |first14=P. |last15=Uusitalo |first15=J. |title=Alpha-decay studies of the new isotopes 191At and 193At |journal=The European Physical Journal A - Hadrons and Nuclei |date=1 August 2003 |volume=17 |issue=4 |pages=537–558 |doi=10.1140/epja/i2002-10162-1 |url=https://link.springer.com/content/pdf/10.1140/epja/i2002-10162-1.pdf |access-date=23 June 2023 |language=en |issn=1434-601X}}</ref>
+| <sup>191</sup>At<ref>{{cite journal |last1=Kettunen |first1=H. |last2=Enqvist |first2=T. |last3=Grahn |first3=T. |last4=Greenlees |first4=P.T. |last5=Jones |first5=P. |last6=Julin |first6=R. |last7=Juutinen |first7=S. |last8=Keenan |first8=A. |last9=Kuusiniemi |first9=P. |last10=Leino |first10=M. |last11=Leppänen |first11=A.-P. |last12=Nieminen |first12=P. |last13=Pakarinen |first13=J. |last14=Rahkila |first14=P. |last15=Uusitalo |first15=J. |title=Alpha-decay studies of the new isotopes 191At and 193At |journal=The European Physical Journal A - Hadrons and Nuclei |date=1 August 2003 |volume=17 |issue=4 |pages=537–558 |doi=10.1140/epja/i2002-10162-1 |s2cid=122384851 |url=https://link.springer.com/content/pdf/10.1140/epja/i2002-10162-1.pdf |access-date=23 June 2023 |language=en |issn=1434-601X}}</ref>
 | style="text-align:right" | 85
 | style="text-align:right" | 106
@@ Line 51: / Line 51: @@
 |
 |-
-| rowspan=3|<sup>192</sup>At<ref name="NUBASE2020">{{cite journal |last1=Kondev |first1=F. G. |last2=Wang |first2=M. |last3=Huang |first3=W. J. |last4=Naimi |first4=S. |last5=Audi |first5=G. |title=The NUBASE2020 evaluation of nuclear physics properties * |journal=Chinese Physics C, High Energy Physics and Nuclear Physics |date=1 March 2021 |volume=45 |issue=3 |doi=10.1088/1674-1137/abddae |url=https://www.osti.gov/biblio/1774641 |access-date=4 July 2023 |language=English |issn=1674-1137}}</ref>
+| rowspan=3|<sup>192</sup>At<ref name="NUBASE2020">{{cite journal |last1=Kondev |first1=F. G. |last2=Wang |first2=M. |last3=Huang |first3=W. J. |last4=Naimi |first4=S. |last5=Audi |first5=G. |title=The NUBASE2020 evaluation of nuclear physics properties * |journal=Chinese Physics C, High Energy Physics and Nuclear Physics |date=1 March 2021 |volume=45 |issue=3 |page=030001 |doi=10.1088/1674-1137/abddae |osti=1774641 |s2cid=233794940 |url=https://www.osti.gov/biblio/1774641 |access-date=4 July 2023 |language=English |issn=1674-1137}}</ref>
 | rowspan=3 style="text-align:right" | 85
 | rowspan=3 style="text-align:right" | 107
@@ Line 621: / Line 621: @@
 | rowspan=2 style="text-align:right" | 133
 | rowspan=2|218.008694(12)
-| rowspan=2|1.27(6)&nbsp;s<ref>{{cite journal | last=Cubiss | first=J. G. | last2=Andreyev | first2=A. N. | last3=Barzakh | first3=A. E. | last4=Andel | first4=B. | last5=Antalic | first5=S. | last6=Cocolios | first6=T. E. | last7=Goodacre | first7=T. Day | last8=Fedorov | first8=D. V. | last9=Fedosseev | first9=V. N. | last10=Ferrer | first10=R. | last11=Fink | first11=D. A. | last12=Gaffney | first12=L. P. | last13=Ghys | first13=L. | last14=Huyse | first14=M. | last15=Kalaninová | first15=Z. | last16=Köster | first16=U. | last17=Marsh | first17=B. A. | last18=Molkanov | first18=P. L. | last19=Rossel | first19=R. E. | last20=Rothe | first20=S. | last21=Seliverstov | first21=M. D. | last22=Sels | first22=S. | last23=Sjödin | first23=A. M. | last24=Stryjczyk | first24=M. | last25=L.Truesdale | first25=V. | last26=Van Beveren | first26=C. | last27=Van Duppen | first27=P. | last28=Wilson | first28=G. L. | title=Fine structure in the α decay of At218 | journal=Physical Review C | publisher=American Physical Society (APS) | volume=99 | issue=6 | date=2019-06-14 | issn=2469-9985 | doi=10.1103/physrevc.99.064317}}</ref>
+| rowspan=2|1.27(6)&nbsp;s<ref>{{cite journal | last1=Cubiss | first1=J. G. | last2=Andreyev | first2=A. N. | last3=Barzakh | first3=A. E. | last4=Andel | first4=B. | last5=Antalic | first5=S. | last6=Cocolios | first6=T. E. | last7=Goodacre | first7=T. Day | last8=Fedorov | first8=D. V. | last9=Fedosseev | first9=V. N. | last10=Ferrer | first10=R. | last11=Fink | first11=D. A. | last12=Gaffney | first12=L. P. | last13=Ghys | first13=L. | last14=Huyse | first14=M. | last15=Kalaninová | first15=Z. | last16=Köster | first16=U. | last17=Marsh | first17=B. A. | last18=Molkanov | first18=P. L. | last19=Rossel | first19=R. E. | last20=Rothe | first20=S. | last21=Seliverstov | first21=M. D. | last22=Sels | first22=S. | last23=Sjödin | first23=A. M. | last24=Stryjczyk | first24=M. | last25=L.Truesdale | first25=V. | last26=Van Beveren | first26=C. | last27=Van Duppen | first27=P. | last28=Wilson | first28=G. L. | title=Fine structure in the α decay of At218 | journal=Physical Review C | publisher=American Physical Society (APS) | volume=99 | issue=6 | date=2019-06-14 | page=064317 | issn=2469-9985 | doi=10.1103/physrevc.99.064317| s2cid=197508141 }}</ref>
 | α (99.9%)
 | <sup>214</sup>Bi

Revision as of 15:51, 17 July 2023

List of isotopes

Alpha decay

See also

References