Isotopes of iridium

Isotopes of iridium (₇₇Ir)
ε	192Os
Standard atomic weight Ar°(Ir)
	192.217±0.002[2]; 192.22±0.01 (abridged)[3];

There are two natural isotopes of iridium (₇₇Ir), and 37 radioisotopes, the most stable radioisotope being ¹⁹²Ir with a half-life of 73.83 days, and many nuclear isomers, the most stable of which is ^192m2Ir with a half-life of 241 years. All other isomers have half-lives under a year, most under a day. All isotopes of iridium are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.[4]

List of isotopes

Nuclide[5] [n 1]	Z	N	Isotopic mass (Da)[6] [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)
Nuclide[5] [n 1]	Excitation energy[n 4]			Half-life [n 4]	Decay mode [n 5]	Daughter isotope [n 6][n 7]	Spin and parity [n 8][n 4]	Normal proportion	Range of variation
¹⁶⁴Ir[7]	77	87	163.99220(44)#	<0.5 μs	p?	¹⁶³Os	2−#
^164mIr	270(110)# keV			70(10) μs	p (96%)	¹⁶³Os	9+#
^164mIr	270(110)# keV			70(10) μs	α (4%)	^160mRe	9+#
¹⁶⁵Ir	77	88	164.98752(23)#	1.20+0.82 −0.74 μs[8]	p	¹⁶⁴Os	(1/2+)
^165mIr[9]	~255 keV			340(40) μs	p (88%)	¹⁶⁴Os	(11/2−)
^165mIr[9]	~255 keV			340(40) μs	α (12%)	^161mRe	(11/2−)
¹⁶⁶Ir	77	89	165.98582(22)#	10.5(22) ms	α (93%)	¹⁶²Re	(2−)
¹⁶⁶Ir	77	89	165.98582(22)#	10.5(22) ms	p (7%)	¹⁶⁵Os	(2−)
^166mIr	172(6) keV			15.1(9) ms	α (98.2%)	¹⁶²Re	(9+)
^166mIr	172(6) keV			15.1(9) ms	p (1.8%)	¹⁶⁵Os	(9+)
¹⁶⁷Ir	77	90	166.981665(20)	35.2(20) ms	α (48%)	¹⁶³Re	1/2+
					p (32%)	¹⁶⁶Os
					β⁺ (20%)	¹⁶⁷Os
^167mIr	175.3(22) keV			30.0(6) ms	α (80%)	¹⁶³Re	11/2−
					β⁺ (20%)	¹⁶⁷Os
					p (.4%)	¹⁶⁶Os
¹⁶⁸Ir	77	91	167.97988(16)#	161(21) ms	α	¹⁶⁴Re	(2-)
¹⁶⁸Ir	77	91	167.97988(16)#	161(21) ms	β⁺ (rare)	¹⁶⁸Os	(2-)
^168mIr	50(100)# keV			125(40) ms	α	¹⁶⁴Re	(9+)
¹⁶⁹Ir	77	92	168.976295(28)	780(360) ms [0.64(+46−24) s]	α	¹⁶⁵Re	(1/2+)
¹⁶⁹Ir	77	92	168.976295(28)	780(360) ms [0.64(+46−24) s]	β⁺ (rare)	¹⁶⁹Os	(1/2+)
^169mIr	154(24) keV			308(22) ms	α (72%)	¹⁶⁵Re	(11/2−)
^169mIr	154(24) keV			308(22) ms	β⁺ (28%)	¹⁶⁹Os	(11/2−)
¹⁷⁰Ir	77	93	169.97497(11)#	910(150) ms [0.87(+18−12) s]	β⁺ (64%)	¹⁷⁰Os	low#
¹⁷⁰Ir	77	93	169.97497(11)#	910(150) ms [0.87(+18−12) s]	α (36%)	¹⁶⁶Re	low#
^170mIr	160(50)# keV			440(60) ms	α (36%)	¹⁶⁶Re	(8+)
					β⁺	¹⁷⁰Os
					IT	¹⁷⁰Ir
¹⁷¹Ir	77	94	170.97163(4)	3.6(10) s [3.2(+13−7) s]	α (58%)	¹⁶⁷Re	1/2+
¹⁷¹Ir	77	94	170.97163(4)	3.6(10) s [3.2(+13−7) s]	β⁺ (42%)	¹⁷¹Os	1/2+
^171mIr	180(30)# keV			1.40(10) s			(11/2−)
¹⁷²Ir	77	95	171.970610(30)	4.4(3) s	β⁺ (98%)	¹⁷²Os	(3+)
¹⁷²Ir	77	95	171.970610(30)	4.4(3) s	α (2%)	¹⁶⁸Re	(3+)
^172mIr	280(100)# keV			2.0(1) s	β⁺ (77%)	¹⁷²Os	(7+)
^172mIr	280(100)# keV			2.0(1) s	α (23%)	¹⁶⁸Re	(7+)
¹⁷³Ir	77	96	172.967502(15)	9.0(8) s	β⁺ (93%)	¹⁷³Os	(3/2+,5/2+)
¹⁷³Ir	77	96	172.967502(15)	9.0(8) s	α (7%)	¹⁶⁹Re	(3/2+,5/2+)
^173mIr	253(27) keV			2.20(5) s	β⁺ (88%)	¹⁷³Os	(11/2−)
^173mIr	253(27) keV			2.20(5) s	α (12%)	¹⁶⁹Re	(11/2−)
¹⁷⁴Ir	77	97	173.966861(30)	7.9(6) s	β⁺ (99.5%)	¹⁷⁴Os	(3+)
¹⁷⁴Ir	77	97	173.966861(30)	7.9(6) s	α (.5%)	¹⁷⁰Re	(3+)
^174mIr	193(11) keV			4.9(3) s	β⁺ (99.53%)	¹⁷⁴Os	(7+)
^174mIr	193(11) keV			4.9(3) s	α (.47%)	¹⁷⁰Re	(7+)
¹⁷⁵Ir	77	98	174.964113(21)	9(2) s	β⁺ (99.15%)	¹⁷⁵Os	(5/2−)
¹⁷⁵Ir	77	98	174.964113(21)	9(2) s	α (.85%)	¹⁷¹Re	(5/2−)
¹⁷⁶Ir	77	99	175.963649(22)	8.3(6) s	β⁺ (97.9%)	¹⁷⁶Os
¹⁷⁶Ir	77	99	175.963649(22)	8.3(6) s	α (2.1%)	¹⁷²Re
¹⁷⁷Ir	77	100	176.961302(21)	30(2) s	β⁺ (99.94%)	¹⁷⁷Os	5/2−
¹⁷⁷Ir	77	100	176.961302(21)	30(2) s	α (.06%)	¹⁷³Re	5/2−
¹⁷⁸Ir	77	101	177.961082(21)	12(2) s	β⁺	¹⁷⁸Os
¹⁷⁹Ir	77	102	178.959122(12)	79(1) s	β⁺	¹⁷⁹Os	(5/2)−
¹⁸⁰Ir	77	103	179.959229(23)	1.5(1) min	β⁺	¹⁸⁰Os	(4,5)(+#)
¹⁸¹Ir	77	104	180.957625(28)	4.90(15) min	β⁺	¹⁸¹Os	(5/2)−
¹⁸²Ir	77	105	181.958076(23)	15(1) min	β⁺	¹⁸²Os	(3+)
¹⁸³Ir	77	106	182.956846(27)	57(4) min	β⁺ ( 99.95%)	¹⁸³Os	5/2−
¹⁸³Ir	77	106	182.956846(27)	57(4) min	α (.05%)	¹⁷⁹Re	5/2−
¹⁸⁴Ir	77	107	183.95748(3)	3.09(3) h	β⁺	¹⁸⁴Os	5−
^184m1Ir	225.65(11) keV			470(30) μs			3+
^184m2Ir	328.40(24) keV			350(90) ns			(7)+
¹⁸⁵Ir	77	108	184.95670(3)	14.4(1) h	β⁺	¹⁸⁵Os	5/2−
¹⁸⁶Ir	77	109	185.957946(18)	16.64(3) h	β⁺	¹⁸⁶Os	5+
^186mIr	0.8(4) keV			1.92(5) h	β⁺	¹⁸⁶Os	2−
^186mIr	0.8(4) keV			1.92(5) h	IT (rare)	¹⁸⁶Ir	2−
¹⁸⁷Ir	77	110	186.957363(7)	10.5(3) h	β⁺	¹⁸⁷Os	3/2+
^187m1Ir	186.15(4) keV			30.3(6) ms	IT	¹⁸⁷Ir	9/2−
^187m2Ir	433.81(9) keV			152(12) ns			11/2−
¹⁸⁸Ir	77	111	187.958853(8)	41.5(5) h	β⁺	¹⁸⁸Os	1−
^188mIr	970(30) keV			4.2(2) ms	IT	¹⁸⁸Ir	7+#
^188mIr	970(30) keV			4.2(2) ms	β⁺ (rare)	¹⁸⁸Os	7+#
¹⁸⁹Ir	77	112	188.958719(14)	13.2(1) d	EC	¹⁸⁹Os	3/2+
^189m1Ir	372.18(4) keV			13.3(3) ms	IT	¹⁸⁹Ir	11/2−
^189m2Ir	2333.3(4) keV			3.7(2) ms			(25/2)+
¹⁹⁰Ir	77	113	189.9605460(18)	11.78(10) d	EC	¹⁹⁰Os	4−
¹⁹⁰Ir	77	113	189.9605460(18)	11.78(10) d	β⁺ (<0.002%)[1]	¹⁹⁰Os	4−
^190m1Ir	26.1(1) keV			1.120(3) h	IT	¹⁹⁰Ir	(1−)
^190m2Ir	36.154(25) keV			>2 μs			(4)+
^190m3Ir	376.4(1) keV			3.087(12) h			(11)−
¹⁹¹Ir	77	114	190.9605940(18)	Observationally Stable[n 9]			3/2+	0.373(2)
^191m1Ir	171.24(5) keV			4.94(3) s	IT	¹⁹¹Ir	11/2−
^191m2Ir	2120(40) keV			5.5(7) s
¹⁹²Ir	77	115	191.9626050(18)	73.827(13) d	β⁻ (95.24%)	¹⁹²Pt	4+
¹⁹²Ir	77	115	191.9626050(18)	73.827(13) d	EC (4.76%)	¹⁹²Os	4+
^192m1Ir	56.720(5) keV			1.45(5) min	IT (98.25%)	¹⁹²Ir	1−
^192m1Ir	56.720(5) keV			1.45(5) min	β⁻ (1.75%)	¹⁹²Pt	1−
^192m2Ir	168.14(12) keV			241(9) y	IT	¹⁹²Ir	(11−)
¹⁹³Ir	77	116	192.9629264(18)	Observationally Stable[n 10]			3/2+	0.627(2)
^193mIr	80.240(6) keV			10.53(4) d	IT	¹⁹³Ir	11/2−
¹⁹⁴Ir	77	117	193.9650784(18)	19.28(13) h	β⁻	¹⁹⁴Pt	1−
^194m1Ir	147.078(5) keV			31.85(24) ms	IT	¹⁹⁴Ir	(4+)
^194m2Ir	370(70) keV			171(11) d			(10,11)(−#)
¹⁹⁵Ir	77	118	194.9659796(18)	2.5(2) h	β⁻	¹⁹⁵Pt	3/2+
^195mIr	100(5) keV			3.8(2) h	β⁻ (95%)	¹⁹⁵Pt	11/2−
^195mIr	100(5) keV			3.8(2) h	IT (5%)	¹⁹⁵Ir	11/2−
¹⁹⁶Ir	77	119	195.96840(4)	52(1) s	β⁻	¹⁹⁶Pt	(0−)
^196mIr	210(40) keV			1.40(2) h	β⁻ (99.7%)	¹⁹⁶Pt	(10,11−)
^196mIr	210(40) keV			1.40(2) h	IT	¹⁹⁶Ir	(10,11−)
¹⁹⁷Ir	77	120	196.969653(22)	5.8(5) min	β⁻	¹⁹⁷Pt	3/2+
^197mIr	115(5) keV			8.9(3) min	β⁻ (99.75%)	¹⁹⁷Pt	11/2−
^197mIr	115(5) keV			8.9(3) min	IT (.25%)	¹⁹⁷Ir	11/2−
¹⁹⁸Ir	77	121	197.97228(21)#	8(1) s	β⁻	¹⁹⁸Pt
¹⁹⁹Ir	77	122	198.97380(4)	7(5) s	β⁻	¹⁹⁹Pt	3/2+#
^199mIr	130(40)# keV			235(90) ns	IT	¹⁹⁹Ir	11/2−#
²⁰⁰Ir	77	123	199.976800(210)#	43(6) s	β⁻	²⁰⁰Pt	(2-, 3-)
²⁰¹Ir	77	124	200.978640(210)#	21(5) s	β⁻	²⁰¹Pt	(3/2+)
²⁰²Ir	77	125	201.981990(320)#	11(3) s	β⁻	²⁰²Pt	(2-)
^202mIr	2000(1000)# keV			3.4(0.6) μs	IT	²⁰²Ir
This table header & footer:

^mIr – 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).
# – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
Modes of decay:

EC: Electron capture

IT: Isomeric transition

p: Proton emission
Bold italics symbol as daughter – Daughter product is nearly stable.
Bold symbol as daughter – Daughter product is stable.
( ) spin value – Indicates spin with weak assignment arguments.
Believed to undergo α decay to ¹⁸⁷Re
Believed to undergo α decay to ¹⁸⁹Re

Iridium-192

Iridium-192 (symbol ¹⁹²Ir) is a radioactive isotope of iridium, with a half-life of 73.83 days.[10] It decays by emitting beta (β) particles and gamma (γ) radiation. About 96% of ¹⁹²Ir decays occur via emission of β and γ radiation, leading to ¹⁹²Pt. Some of the β particles are captured by other ¹⁹²Ir nuclei, which are then converted to ¹⁹²Os. Electron capture is responsible for the remaining 4% of ¹⁹²Ir decays.[11] Iridium-192 is normally produced by neutron activation of natural-abundance iridium metal.[12]

Iridium-192 is a very strong gamma ray emitter, with a gamma dose-constant of approximately 1.54 μSv·h⁻¹·MBq⁻¹ at 30 cm, and a specific activity of 341 TBq·g⁻¹ (9.22 kCi·g⁻¹).[13][14] There are seven principal energy packets produced during its disintegration process ranging from just over 0.2 to about 0.6 MeV.

The ^192m2Ir isomer is unusual, both for its long half-life for an isomer, and that said half-life greatly exceeds that of the ground state of the same isotope.

References

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.
"Standard Atomic Weights: Iridium". CIAAW. 2017.
Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.
Belli, P.; Bernabei, R.; Danevich, F. A.; et al. (2019). "Experimental searches for rare alpha and beta decays". European Physical Journal A. 55 (8): 140–1–140–7. arXiv:1908.11458. Bibcode:2019EPJA...55..140B. doi:10.1140/epja/i2019-12823-2. ISSN 1434-601X. S2CID 201664098.
Half-life, decay mode, nuclear spin, and isotopic composition is sourced in:
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.
Wang, M.; Audi, G.; Kondev, F. G.; Huang, W. J.; Naimi, S.; Xu, X. (2017). "The AME2016 atomic mass evaluation (II). Tables, graphs, and references" (PDF). Chinese Physics C. 41 (3): 030003-1–030003-442. doi:10.1088/1674-1137/41/3/030003.
Drummond, M. C.; O'Donnell, D.; Page, R. D.; Joss, D. T.; Capponi, L.; Cox, D. M.; Darby, I. G.; Donosa, L.; Filmer, F.; Grahn, T.; Greenlees, P. T.; Hauschild, K.; Herzan, A.; Jakobsson, U.; Jones, P. M.; Julin, R.; Juutinen, S.; Ketelhut, S.; Leino, M.; Lopez-Martens, A.; Mistry, A. K.; Nieminen, P.; Peura, P.; Rahkila, P.; Rinta-Antila, S.; Ruotsalainen, P.; Sandzelius, M.; Sarén, J.; Sayğı, B.; Scholey, C.; Simpson, J.; Sorri, J.; Thornthwaite, A.; Uusitalo, J. (16 June 2014). "α decay of the π h 11 / 2 isomer in Ir 164". Physical Review C. 89 (6): 064309. Bibcode:2014PhRvC..89f4309D. doi:10.1103/PhysRevC.89.064309. ISSN 0556-2813. Retrieved 21 June 2023.
Hilton, Joshua Ben. "Decays of new nuclides 169Au, 170Hg, 165Pt and the ground state of 165Ir discovered using MARA". University of Liverpool. ProQuest 2448649087. Retrieved 21 June 2023.
Drummond, M. C.; O'Donnell, D.; Page, R. D.; Joss, D. T.; Capponi, L.; Cox, D. M.; Darby, I. G.; Donosa, L.; Filmer, F.; Grahn, T.; Greenlees, P. T.; Hauschild, K.; Herzan, A.; Jakobsson, U.; Jones, P. M.; Julin, R.; Juutinen, S.; Ketelhut, S.; Leino, M.; Lopez-Martens, A.; Mistry, A. K.; Nieminen, P.; Peura, P.; Rahkila, P.; Rinta-Antila, S.; Ruotsalainen, P.; Sandzelius, M.; Sarén, J.; Sayğı, B.; Scholey, C.; Simpson, J.; Sorri, J.; Thornthwaite, A.; Uusitalo, J. (16 June 2014). "α decay of the π h 11 / 2 isomer in Ir 164". Physical Review C. 89 (6): 064309. Bibcode:2014PhRvC..89f4309D. doi:10.1103/PhysRevC.89.064309. ISSN 0556-2813. Retrieved 21 June 2023.
"Radioisotope Brief: Iridium-192 (Ir-192)". Retrieved 20 March 2012.
Baggerly, Leo L. (1956). The radioactive decay of Iridium-192 (PDF) (Ph.D. thesis). Pasadena, Calif.: California Institute of Technology. pp. 1, 2, 7. doi:10.7907/26VA-RB25.
"Isotope Supplier: Stable Isotopes and Radioisotopes from ISOFLEX - Iridium-192". www.isoflex.com. Retrieved 2017-10-11.
Delacroix, D; Guerre, J P; Leblanc, P; Hickman, C (2002). Radionuclide and Radiation Protection Data Handbook (PDF). Radiation Protection Dosimetry. Vol. 98, no. 1 (2nd ed.). Ashford, Kent: Nuclear Technology Publishing. pp. 9–168. doi:10.1093/OXFORDJOURNALS.RPD.A006705. ISBN 1870965876. PMID 11916063. S2CID 123447679. Archived from the original (PDF) on 2019-08-22.
Unger, L M; Trubey, D K (May 1982). Specific Gamma-Ray Dose Constants for Nuclides Important to Dosimetry and Radiological Assessment (PDF) (Report). Oak Ridge National Laboratory. Archived from the original (PDF) on 22 March 2018.

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.

External links

NLM Hazardous Substances Databank – Iridium, Radioactive (referring to iridium-192)

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.

[6] Ir – Excited nuclear isomer.

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

[TMS-9] # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).

[TNN-10] # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

[11] Modes of decay:

EC: Electron capture

IT: Isomeric transition

p: Proton emission

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

[13] Bold symbol as daughter – Daughter product is stable.

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

[18] Believed to undergo α decay to ¹⁸⁷Re

[19] Believed to undergo α decay to ¹⁸⁹Re

[NUBASE2020-1] 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.

[2] "Standard Atomic Weights: Iridium". CIAAW. 2017.

[CIAAW2021-3] Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.

[bellidecay-4] Belli, P.; Bernabei, R.; Danevich, F. A.; et al. (2019). "Experimental searches for rare alpha and beta decays". European Physical Journal A. 55 (8): 140–1–140–7. arXiv:1908.11458. Bibcode:2019EPJA...55..140B. doi:10.1140/epja/i2019-12823-2. ISSN 1434-601X. S2CID 201664098.

[NUBASE2016-5] Half-life, decay mode, nuclear spin, and isotopic composition is sourced in:
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.

[AME2016_II-7] Wang, M.; Audi, G.; Kondev, F. G.; Huang, W. J.; Naimi, S.; Xu, X. (2017). "The AME2016 atomic mass evaluation (II). Tables, graphs, and references" (PDF). Chinese Physics C. 41 (3): 030003-1–030003-442. doi:10.1088/1674-1137/41/3/030003.

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EC:	Electron capture
IT:	Isomeric transition
p:	Proton emission