Isotopes of protactinium

Isotopes of protactinium (₉₁Pa)
β−	230U
α	226Ac
Standard atomic weight Ar°(Pa)
	231.03588±0.00001; 231.04±0.01 (abridged);
	view; talk; edit;

Protactinium (₉₁Pa) has no stable isotopes. The four naturally occurring isotopes allow a standard atomic weight to be given.

Twenty-nine radioisotopes of protactinium have been characterized, ranging from ²¹¹Pa to ²³⁹Pa. The most stable isotope is ²³¹Pa with a half-life of 32,760 years, ²³³Pa with a half-life of 26.967 days, and ²³⁰Pa with a half-life of 17.4 days. All of the remaining radioactive isotopes have half-lives less than 1.6 days, and the majority of these have half-lives less than 1.8 seconds. This element also has five meta states, ^217mPa (t_1/2 1.15 milliseconds), ^220m1Pa (t_1/2 = 308 nanoseconds), ^220m2Pa (t_1/2 = 69 nanoseconds), ^229mPa (t_1/2 = 420 nanoseconds), and ^234mPa (t_1/2 = 1.17 minutes).

The only naturally occurring isotopes are ²³¹Pa, which occurs as an intermediate decay product of ²³⁵U, ²³⁴Pa and ^234mPa, both of which occur as intermediate decay products of ²³⁸U. ²³¹Pa makes up nearly all natural protactinium.

The primary decay mode for isotopes of Pa lighter than (and including) the most stable isotope ²³¹Pa is alpha decay, except for ²²⁸Pa to ²³⁰Pa, which primarily decay by electron capture to isotopes of thorium. The primary mode for the heavier isotopes is beta minus (β⁻) decay. The primary decay products of ²³¹Pa and isotopes of protactinium lighter than and including ²²⁷Pa are isotopes of actinium and the primary decay products for the heavier isotopes of protactinium are isotopes of uranium.

List of isotopes

Nuclide ^{[n 1]}	Historic name	Z	N	Isotopic mass (Da) ^{[n 2]}^{[n 3]}	Half-life ^{[n 4]}	Decay mode ^{[n 5]}	Daughter isotope ^{[n 6]}	Spin and parity ^{[n 7]}^{[n 4]}	Isotopic abundance
Nuclide ^{[n 1]}	Historic name	Excitation energy			Half-life ^{[n 4]}	Decay mode ^{[n 5]}	Daughter isotope ^{[n 6]}	Spin and parity ^{[n 7]}^{[n 4]}	Isotopic abundance
²¹¹Pa^[4]		91	120		3.8(+4.6−1.4) ms	α	²⁰⁷Ac	9/2−#
²¹²Pa		91	121	212.02320(8)	8(5) ms [5.1(+61−19) ms]	α	²⁰⁸Ac	7+#
²¹³Pa		91	122	213.02111(8)	7(3) ms [5.3(+40−16) ms]	α	²⁰⁹Ac	9/2−#
²¹⁴Pa		91	123	214.02092(8)	17(3) ms	α	²¹⁰Ac
²¹⁵Pa		91	124	215.01919(9)	14(2) ms	α	²¹¹Ac	9/2−#
²¹⁶Pa		91	125	216.01911(8)	105(12) ms	α (80%)	²¹²Ac
²¹⁶Pa		91	125	216.01911(8)	105(12) ms	β⁺ (20%)	²¹⁶Th
²¹⁷Pa		91	126	217.01832(6)	3.48(9) ms	α	²¹³Ac	9/2−#
^217mPa		1860(7) keV			1.08(3) ms	α	²¹³Ac	29/2+#
^217mPa		1860(7) keV			1.08(3) ms	IT (rare)	²¹⁷Pa	29/2+#
²¹⁸Pa		91	127	218.020042(26)	0.113(1) ms	α	²¹⁴Ac
²¹⁹Pa		91	128	219.01988(6)	53(10) ns	α^{[n 8]}	²¹⁵Ac	9/2−
²²⁰Pa		91	129	220.02188(6)	780(160) ns	α	²¹⁶Ac	1−#
^220m1Pa^[6]		34(26) keV			308(+250-99) ns	α	²¹⁶Ac
^220m2Pa^[6]		297(65) keV			69(+330-30) ns	α	²¹⁶Ac
²²¹Pa		91	130	221.02188(6)	4.9(8) μs	α	²¹⁷Ac	9/2−
²²²Pa		91	131	222.02374(8)#	3.2(3) ms	α	²¹⁸Ac
²²³Pa		91	132	223.02396(8)	5.1(6) ms	α	²¹⁹Ac
²²³Pa		91	132	223.02396(8)	5.1(6) ms	β⁺ (.001%)	²²³Th
²²⁴Pa		91	133	224.025626(17)	844(19) ms	α (99.9%)	²²⁰Ac	5−#
²²⁴Pa		91	133	224.025626(17)	844(19) ms	β⁺ (.1%)	²²⁴Th	5−#
²²⁵Pa		91	134	225.02613(8)	1.7(2) s	α	²²¹Ac	5/2−#
²²⁶Pa		91	135	226.027948(12)	1.8(2) min	α (74%)	²²²Ac
²²⁶Pa		91	135	226.027948(12)	1.8(2) min	β⁺ (26%)	²²⁶Th
²²⁷Pa		91	136	227.028805(8)	38.3(3) min	α (85%)	²²³Ac	(5/2−)
²²⁷Pa		91	136	227.028805(8)	38.3(3) min	EC (15%)	²²⁷Th	(5/2−)
²²⁸Pa		91	137	228.031051(5)	22(1) h	β⁺ (98.15%)	²²⁸Th	3+
²²⁸Pa		91	137	228.031051(5)	22(1) h	α (1.85%)	²²⁴Ac	3+
²²⁹Pa		91	138	229.0320968(30)	1.50(5) d	EC (99.52%)	²²⁹Th	(5/2+)
²²⁹Pa		91	138	229.0320968(30)	1.50(5) d	α (.48%)	²²⁵Ac	(5/2+)
^229mPa		11.6(3) keV			420(30) ns			3/2−
²³⁰Pa		91	139	230.034541(4)	17.4(5) d	β⁺ (91.6%)	²³⁰Th	(2−)
						β⁻ (8.4%)	²³⁰U
						α (.00319%)	²²⁶Ac
²³¹Pa	Protoactinium	91	140	231.0358840(24)	3.276(11)×10⁴ y	α	²²⁷Ac	3/2−	1.0000^{[n 9]}
						CD (1.34×10⁻⁹%)	²⁰⁷Tl ²⁴Ne
						SF (3×10⁻¹⁰%)	(various)
						CD (10⁻¹²%)	²⁰⁸Pb ²³F
²³²Pa		91	141	232.038592(8)	1.31(2) d	β⁻	²³²U	(2−)
²³²Pa		91	141	232.038592(8)	1.31(2) d	EC (.003%)	²³²Th	(2−)
²³³Pa		91	142	233.0402473(23)	26.975(13) d	β⁻	²³³U	3/2−	Trace^{[n 10]}
²³⁴Pa	Uranium Z	91	143	234.043308(5)	6.70(5) h	β⁻	²³⁴U	4+	Trace^{[n 11]}
²³⁴Pa	Uranium Z	91	143	234.043308(5)	6.70(5) h	SF (3×10⁻¹⁰%)	(various)	4+	Trace^{[n 11]}
^234mPa	Uranium X₂ Brevium	78(3) keV			1.17(3) min	β⁻ (99.83%)	²³⁴U	(0−)	Trace^{[n 11]}
						IT (.16%)	²³⁴Pa
						SF (10⁻¹⁰%)	(various)
²³⁵Pa		91	144	235.04544(5)	24.44(11) min	β⁻	²³⁵U	(3/2−)
²³⁶Pa		91	145	236.04868(21)	9.1(1) min	β⁻	²³⁶U	1(−)
²³⁶Pa		91	145	236.04868(21)	9.1(1) min	β⁻, SF (6×10⁻⁸%)	(various)	1(−)
²³⁷Pa		91	146	237.05115(11)	8.7(2) min	β⁻	²³⁷U	(1/2+)
²³⁸Pa		91	147	238.05450(6)	2.27(9) min	β⁻	²³⁸U	(3−)#
²³⁸Pa		91	147	238.05450(6)	2.27(9) min	β⁻, SF (2.6×10⁻⁶%)	(various)	(3−)#
²³⁹Pa		91	148	239.05726(21)#	1.8(5) h	β⁻	²³⁹U	(3/2)(−#)
This table header & footer: view

^ ^mPa – 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).
^ ^a ^b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
^ Modes of decay:
CD: Cluster decay
EC: Electron capture
IT: Isomeric transition
SF: Spontaneous fission
^ Bold italics symbol as daughter – Daughter product is nearly stable.
^ ( ) spin value – Indicates spin with weak assignment arguments.
^ Theoretically capable of β⁺ decay to ²¹⁹Th^[1]^[5]
^ Intermediate decay product of ²³⁵U
^ Intermediate decay product of ²³⁷Np
^ ^a ^b Intermediate decay product of ²³⁸U

Actinides and fission products

Actinides and fission products by half-life v t e
Actinides^[7] by decay chain				Half-life range (a)	Fission products of ²³⁵U by yield^[8]
4n	4n + 1	4n + 2	4n + 3	Half-life range (a)	4.5–7%	0.04–1.25%	<0.001%
²²⁸Ra^№				4–6 a		¹⁵⁵Eu^þ
²⁴⁴Cm^ƒ	²⁴¹Pu^ƒ	²⁵⁰Cf	²²⁷Ac^№	10–29 a	⁹⁰Sr	⁸⁵Kr	^113mCd^þ
²³²U^ƒ		²³⁸Pu^ƒ	²⁴³Cm^ƒ	29–97 a	¹³⁷Cs	¹⁵¹Sm^þ	^121mSn
²⁴⁸Bk^[9]	²⁴⁹Cf^ƒ	^242mAm^ƒ		141–351 a	No fission products have a half-life in the range of 100 a–210 ka ...
	²⁴¹Am^ƒ		²⁵¹Cf^ƒ^[10]	430–900 a
		²²⁶Ra^№	²⁴⁷Bk	1.3–1.6 ka
²⁴⁰Pu	²²⁹Th	²⁴⁶Cm^ƒ	²⁴³Am^ƒ	4.7–7.4 ka
	²⁴⁵Cm^ƒ	²⁵⁰Cm		8.3–8.5 ka
			²³⁹Pu^ƒ	24.1 ka
		²³⁰Th^№	²³¹Pa^№	32–76 ka
²³⁶Np^ƒ	²³³U^ƒ	²³⁴U^№		150–250 ka	⁹⁹Tc^₡	¹²⁶Sn
²⁴⁸Cm		²⁴²Pu		327–375 ka		⁷⁹Se^₡
				1.53 Ma	⁹³Zr
	²³⁷Np^ƒ			2.1–6.5 Ma	¹³⁵Cs^₡	¹⁰⁷Pd
²³⁶U			²⁴⁷Cm^ƒ	15–24 Ma		¹²⁹I^₡
²⁴⁴Pu				80 Ma	... nor beyond 15.7 Ma^[11]
²³²Th^№		²³⁸U^№	²³⁵U^ƒ№	0.7–14.1 Ga	... nor beyond 15.7 Ma^[11]
₡, has thermal neutron capture cross section in the range of 8–50 barns ƒ, fissile №, primarily a naturally occurring radioactive material (NORM) þ, neutron poison (thermal neutron capture cross section greater than 3k barns)

Protactinium-230

Protactinium-230 has 139 neutrons and a half-life of 17.4 days. Most of the time (92%), it undergoes beta plus decay to ²³⁰Th, with a minor (8%) beta-minus decay branch leading to ²³⁰U. It also has a very rare (.003%) alpha decay mode leading to ²²⁶Ac.^[12] It is not found in nature because its half-life is short and it is not found in the decay chains of ²³⁵U, ²³⁸U, or ²³²Th. It has a mass of 230.034541 u.

Protactinium-230 is of interest as a progenitor of uranium-230, an isotope that has been considered for use in targeted alpha-particle therapy (TAT). It can be produced through proton or deuteron irradiation of nautral thorium.^[13]

Protactinium-231


Transmutations in the thorium fuel cycle v t e
														²³⁷Np
														↑
		²³¹U	←	²³²U	↔	²³³U	↔	²³⁴U	↔	²³⁵U	↔	²³⁶U	→	²³⁷U
		↓		↑		↑		↑
		²³¹Pa	→	²³²Pa	←	²³³Pa	→	²³⁴Pa
		↑				↑
²³⁰Th	→	²³¹Th	←	²³²Th	→	²³³Th
Nuclides with a yellow background in italic have half-lives under 30 days Nuclides in bold have half-lives over 1,000,000 years Nuclides in red frames are fissile

Protactinium-231 is the longest-lived isotope of protactinium, with a half-life of 32,760 years. In nature, it is found in trace amounts as part of the actinium series, which starts with the primordial isotope uranium-235; the equilibrium concentration in uranium ore is 46.55 ²³¹Pa per million ²³⁵U. In nuclear reactors, it is one of the few long-lived radioactive actinides produced as a byproduct of the projected thorium fuel cycle, as a result of (n,2n) reactions where a fast neutron removes a neutron from ²³²Th or ²³²U, and can also be destroyed by neutron capture, though the cross section for this reaction is also low.

binding energy: 1759860 keV
beta decay energy: −382 keV

spin: 3/2−
mode of decay: alpha to ²²⁷Ac, also others

possible parent nuclides: beta from ²³¹Th, EC from ²³¹U, alpha from ²³⁵Np.

Protactinium-233

Protactinium-233 is also part of the thorium fuel cycle. It is an intermediate beta decay product between thorium-233 (produced from natural thorium-232 by neutron capture) and uranium-233 (the fissile fuel of the thorium cycle). Some thorium-cycle reactor designs try to protect Pa-233 from further neutron capture producing Pa-234 and U-234, which are not useful as fuel.

Protactinium-234

Protactinium-234 is a member of the uranium series with a half-life of 6.70 hours. It was discovered by Otto Hahn in 1921.^[14]

Protactinium-234m

Protactinium-234m is a member of the uranium series with a half-life of 1.17 minutes. It was discovered in 1913 by Kazimierz Fajans and Oswald Helmuth Göhring, who named it brevium for its short half-life.^[15] About 99.8% of decays of ²³⁴Th produce this isomer instead of the ground state (t_1/2 = 6.70 hours).^[15]

References

^ ^a ^b 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: Protactinium". 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.
^ Auranen, K (3 September 2020). "Exploring the boundaries of the nuclear landscape: α-decay properties of 211Pa". Physical Review C. 102 (34305): 034305. Bibcode:2020PhRvC.102c4305A. doi:10.1103/PhysRevC.102.034305. S2CID 225343089. Retrieved 17 September 2020.
^ https://www.nndc.bnl.gov/ensnds/219/Pa/adopted.pdf, NNDC Chart of Nuclides, Adopted Levels for ²¹⁹Pa.
^ ^a ^b Huang, T.H.; et al. (2018). "Identification of the new isotope ²²⁴Np" (pdf). Physical Review C. 98 (4): 044302. Bibcode:2018PhRvC..98d4302H. doi:10.1103/PhysRevC.98.044302. S2CID 125251822.
^ Plus radium (element 88). While actually a sub-actinide, it immediately precedes actinium (89) and follows a three-element gap of instability after polonium (84) where no nuclides have half-lives of at least four years (the longest-lived nuclide in the gap is radon-222 with a half life of less than four days). Radium's longest lived isotope, at 1,600 years, thus merits the element's inclusion here.
^ Specifically from thermal neutron fission of uranium-235, e.g. in a typical nuclear reactor.
^ Milsted, J.; Friedman, A. M.; Stevens, C. M. (1965). "The alpha half-life of berkelium-247; a new long-lived isomer of berkelium-248". Nuclear Physics. 71 (2): 299. Bibcode:1965NucPh..71..299M. doi:10.1016/0029-5582(65)90719-4.
"The isotopic analyses disclosed a species of mass 248 in constant abundance in three samples analysed over a period of about 10 months. This was ascribed to an isomer of Bk²⁴⁸ with a half-life greater than 9 [years]. No growth of Cf²⁴⁸ was detected, and a lower limit for the β⁻ half-life can be set at about 10⁴ [years]. No alpha activity attributable to the new isomer has been detected; the alpha half-life is probably greater than 300 [years]."
^ This is the heaviest nuclide with a half-life of at least four years before the "sea of instability".
^ Excluding those "classically stable" nuclides with half-lives significantly in excess of ²³²Th; e.g., while ^113mCd has a half-life of only fourteen years, that of ¹¹³Cd is eight quadrillion years.
^ 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.
^ Mastren, T.; Stein, B.W.; Parker, T.G.; Radchenko, V.; Copping, R.; Owens, A.; Wyant, L.E.; Brugh, M.; Kozimor, S.A.; Noriter, F.M.; Birnbaum, E.R.; John, K.D.; Fassbender, M.E. (2018). "Separation of protactinium employing sulfur-based extraction chromatographic resins". Analytical Chemistry. 90 (11): 7012–7017. doi:10.1021/acs.analchem.8b01380. ISSN 0003-2700. OSTI 1440455. PMID 29757620.
^ Fry, C., and M. Thoennessen. "Discovery of the Actinium, Thorium, Protactinium, and Uranium Isotopes." January 14, 2012. Accessed May 20, 2018. https://people.nscl.msu.edu/~thoennes/2009/ac-th-pa-u-adndt.pdf.
^ ^a ^b "Human Health Fact Sheet - Protactinium" (PDF). Argonne National Laboratory (ANL). November 2001. Retrieved 17 October 2023.

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.

[4] Pa – Excited nuclear isomer.

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

[TMS-6] # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).

[TNN-7] # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

[8] Modes of decay:
CD: Cluster decay
EC: Electron capture
IT: Isomeric transition
SF: Spontaneous fission

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

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

[5-13] Theoretically capable of β⁺ decay to ²¹⁹Th^[1]^[5]

[15] Intermediate decay product of ²³⁵U

[16] Intermediate decay product of ²³⁷Np

[us-17] Intermediate decay product of ²³⁸U

[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: Protactinium". 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.

[11] Auranen, K (3 September 2020). "Exploring the boundaries of the nuclear landscape: α-decay properties of 211Pa". Physical Review C. 102 (34305): 034305. Bibcode:2020PhRvC.102c4305A. doi:10.1103/PhysRevC.102.034305. S2CID 225343089. Retrieved 17 September 2020.

[12] ttps://www.nndc.bnl.gov/ensnds/219/Pa/adopted.pdf, NNDC Chart of Nuclides, Adopted Levels for ²¹⁹Pa.

[Np224-14] Huang, T.H.; et al. (2018). "Identification of the new isotope ²²⁴Np" (pdf). Physical Review C. 98 (4): 044302. Bibcode:2018PhRvC..98d4302H. doi:10.1103/PhysRevC.98.044302. S2CID 125251822.

[18] Plus radium (element 88). While actually a sub-actinide, it immediately precedes actinium (89) and follows a three-element gap of instability after polonium (84) where no nuclides have half-lives of at least four years (the longest-lived nuclide in the gap is radon-222 with a half life of less than four days). Radium's longest lived isotope, at 1,600 years, thus merits the element's inclusion here.

[19] Specifically from thermal neutron fission of uranium-235, e.g. in a typical nuclear reactor.

[20] Milsted, J.; Friedman, A. M.; Stevens, C. M. (1965). "The alpha half-life of berkelium-247; a new long-lived isomer of berkelium-248". Nuclear Physics. 71 (2): 299. Bibcode:1965NucPh..71..299M. doi:10.1016/0029-5582(65)90719-4.
"The isotopic analyses disclosed a species of mass 248 in constant abundance in three samples analysed over a period of about 10 months. This was ascribed to an isomer of Bk²⁴⁸ with a half-life greater than 9 [years]. No growth of Cf²⁴⁸ was detected, and a lower limit for the β⁻ half-life can be set at about 10⁴ [years]. No alpha activity attributable to the new isomer has been detected; the alpha half-life is probably greater than 300 [years]."

[21] This is the heaviest nuclide with a half-life of at least four years before the "sea of instability".

[22] Excluding those "classically stable" nuclides with half-lives significantly in excess of ²³²Th; e.g., while ^113mCd has a half-life of only fourteen years, that of ¹¹³Cd is eight quadrillion years.

[NUBASE2016-23] 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.

[230Pa-24] Mastren, T.; Stein, B.W.; Parker, T.G.; Radchenko, V.; Copping, R.; Owens, A.; Wyant, L.E.; Brugh, M.; Kozimor, S.A.; Noriter, F.M.; Birnbaum, E.R.; John, K.D.; Fassbender, M.E. (2018). "Separation of protactinium employing sulfur-based extraction chromatographic resins". Analytical Chemistry. 90 (11): 7012–7017. doi:10.1021/acs.analchem.8b01380. ISSN 0003-2700. OSTI 1440455. PMID 29757620.

[25] Fry, C., and M. Thoennessen. "Discovery of the Actinium, Thorium, Protactinium, and Uranium Isotopes." January 14, 2012. Accessed May 20, 2018. https://people.nscl.msu.edu/~thoennes/2009/ac-th-pa-u-adndt.pdf.

[hps-26] "Human Health Fact Sheet - Protactinium" (PDF). Argonne National Laboratory (ANL). November 2001. Retrieved 17 October 2023.

[1]

[2]

[3]

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[n 2]

[n 3]

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[4]

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[n 11]

[5]

[7]

[8]

[9]

[10]

[11]

[12]

[13]

[14]

[15]

CD:	Cluster decay
EC:	Electron capture
IT:	Isomeric transition
SF:	Spontaneous fission