Isotopes of thallium

Isotopes of thallium (₈₁Tl)
ε	204Hg
Standard atomic weight Ar°(Tl)
	[204.382, 204.385]; 204.38±0.01 (abridged);
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Thallium (₈₁Tl) has 41 isotopes with atomic masses that range from 176 to 216. ²⁰³Tl and ²⁰⁵Tl are the only stable isotopes and ²⁰⁴Tl is the most stable radioisotope with a half-life of 3.78 years. ²⁰⁷Tl, with a half-life of 4.77 minutes, has the longest half-life of naturally occurring Tl radioisotopes. All isotopes of thallium are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.

Thallium-202 (half-life 12.23 days) can be made in a cyclotron^[4] while thallium-204 (half-life 3.78 years) is made by the neutron activation of stable thallium in a nuclear reactor.^[5]

In the fully ionized state, the isotope ²⁰⁵Tl⁸¹⁺ becomes beta-radioactive, undergoing bound-state β⁻ decay to ²⁰⁵Pb⁸¹⁺ with a half-life of 291+33
−27 days,^[6]^[7] but ²⁰³Tl remains stable.

²⁰⁵Tl is the decay product of bismuth-209, an isotope that was once thought to be stable but is now known to undergo alpha decay with an extremely long half-life of 2.01×10¹⁹ y.^[8] ²⁰⁵Tl is at the end of the neptunium series decay chain.

List of isotopes

Nuclide^[9] ^{[n 1]}	Historic name	Z	N	Isotopic mass (Da)^[10] ^{[n 2]}^{[n 3]}	Half-life ^{[n 4]}	Decay mode ^{[n 5]}	Daughter isotope ^{[n 6]}	Spin and parity ^{[n 7]}^{[n 4]}	Natural abundance (mole fraction)
Nuclide^[9] ^{[n 1]}	Historic name	Excitation energy^{[n 4]}			Half-life ^{[n 4]}	Decay mode ^{[n 5]}	Daughter isotope ^{[n 6]}	Spin and parity ^{[n 7]}^{[n 4]}	Normal proportion	Range of variation
¹⁷⁶Tl^[11]		81	95	176.00059(21)#	2.4+1.6 −0.7 ms	p (~63%)	¹⁷⁵Hg	(3−, 4−, 5−)
¹⁷⁶Tl^[11]		81	95	176.00059(21)#	2.4+1.6 −0.7 ms	α (~37%)	¹⁷²Au	(3−, 4−, 5−)
^176mTl		~671 keV			290+200 −80 μs	p (~50%)	¹⁷⁵Hg
^176mTl		~671 keV			290+200 −80 μs	α (~50%)	^172mAu
¹⁷⁷Tl^[12]		81	96	176.996427(27)	18(5) ms	α (73%)	¹⁷³Au	(1/2+)
¹⁷⁷Tl^[12]		81	96	176.996427(27)	18(5) ms	p (27%)	¹⁷⁶Hg	(1/2+)
^177mTl		807(18) keV			230(40) μs	p (51%)	¹⁷⁶Hg	(11/2−)
^177mTl		807(18) keV			230(40) μs	α (49%)	¹⁷³Au	(11/2−)
¹⁷⁸Tl^[13]		81	97	177.99490(12)#	255(9) ms	α (62%)	¹⁷⁴Au	(4-,5-)
						β⁺ (38%)	¹⁷⁸Hg
						β⁺, SF (0.15%)	(various)
¹⁷⁹Tl^[14]		81	98	178.99109(5)	437(9) ms	α (60%)	¹⁷⁵Au	(1/2+)
¹⁷⁹Tl^[14]		81	98	178.99109(5)	437(9) ms	β⁺ (40%)	¹⁷⁹Hg	(1/2+)
^179m1Tl		825(10)# keV			1.41(2) ms	α	¹⁷⁵Au	(11/2−)
						IT (rare)	¹⁷⁹Tl
						β⁺ (rare)	¹⁷⁹Hg
^179m2Tl		904.5(9) keV			119(14) ns	IT	¹⁷⁹Tl	(9/2−)
¹⁸⁰Tl^[15]		81	99	179.98991(13)#	1.09(1) s	β⁺ (93%)	¹⁸⁰Hg	4-#
						α (7%)	¹⁷⁶Au
						β⁺, SF (0.0032%)	¹⁰⁰Ru, ⁸⁰Kr^[16]
¹⁸¹Tl^[17]		81	100	180.986257(10)	2.9(1) s	β⁺ (91.4%)	¹⁸¹Hg	1/2+#
¹⁸¹Tl^[17]		81	100	180.986257(10)	2.9(1) s	α (8.6%)	¹⁷⁷Au	1/2+#
^181mTl		834.9(4) keV			1.40(3) ms	IT (99.60%)	¹⁸¹Tl	(9/2−)
^181mTl		834.9(4) keV			1.40(3) ms	α (0.40%)	¹⁷⁷Au	(9/2−)
¹⁸²Tl		81	101	181.98567(8)	2.0(3) s	β⁺ (96%)	¹⁸²Hg	2−#
¹⁸²Tl		81	101	181.98567(8)	2.0(3) s	α (4%)	¹⁷⁸Au	2−#
^182m1Tl		100(100)# keV			2.9(5) s	α	¹⁷⁸Au	(7+)
^182m1Tl		100(100)# keV			2.9(5) s	β⁺ (rare)	¹⁸²Hg	(7+)
^182m2Tl		600(140)# keV						10−
¹⁸³Tl		81	102	182.982193(10)	6.9(7) s	β⁺ (98%)	¹⁸³Hg	1/2+#
¹⁸³Tl		81	102	182.982193(10)	6.9(7) s	α (2%)	¹⁷⁹Au	1/2+#
^183m1Tl		630(17) keV			53.3(3) ms	IT (99.99%)	¹⁸³Tl	9/2−#
^183m1Tl		630(17) keV			53.3(3) ms	α (.01%)	¹⁷⁹Au	9/2−#
^183m2Tl		976.8(3) keV			1.48(10) μs			(13/2+)
¹⁸⁴Tl		81	103	183.98187(5)	9.7(6) s	β⁺	¹⁸⁴Hg	2−#
^184m1Tl		100(100)# keV			10# s	β⁺ (97.9%)	¹⁸⁴Hg	7+#
^184m1Tl		100(100)# keV			10# s	α (2.1%)	¹⁸⁰Au	7+#
^184m2Tl		500(140)# keV			47.1 ms	IT (99.911%)		(10−)
^184m2Tl		500(140)# keV			47.1 ms	α (.089%)	¹⁸⁰Au	(10−)
¹⁸⁵Tl		81	104	184.97879(6)	19.5(5) s	α	¹⁸¹Au	1/2+#
¹⁸⁵Tl		81	104	184.97879(6)	19.5(5) s	β⁺	¹⁸⁵Hg	1/2+#
^185mTl		452.8(20) keV			1.93(8) s	IT (99.99%)	¹⁸⁵Tl	9/2−#
						α (.01%)	¹⁸¹Au
						β⁺	¹⁸⁵Hg
¹⁸⁶Tl		81	105	185.97833(20)	40# s	β⁺	¹⁸⁶Hg	(2−)
¹⁸⁶Tl		81	105	185.97833(20)	40# s	α (.006%)	¹⁸²Au	(2−)
^186m1Tl		320(180) keV			27.5(10) s	β⁺	¹⁸⁶Hg	(7+)
^186m2Tl		690(180) keV			2.9(2) s			(10−)
¹⁸⁷Tl		81	106	186.975906(9)	~51 s	β⁺	¹⁸⁷Hg	(1/2+)
¹⁸⁷Tl		81	106	186.975906(9)	~51 s	α (rare)	¹⁸³Au	(1/2+)
^187mTl		335(3) keV			15.60(12) s	α	¹⁸³Au	(9/2−)
						IT	¹⁸⁷Tl
						β⁺	¹⁸⁷Hg
¹⁸⁸Tl		81	107	187.97601(4)	71(2) s	β⁺	¹⁸⁸Hg	(2−)
^188m1Tl		40(30) keV			71(1) s	β⁺	¹⁸⁸Hg	(7+)
^188m2Tl		310(30) keV			41(4) ms			(9−)
¹⁸⁹Tl		81	108	188.973588(12)	2.3(2) min	β⁺	¹⁸⁹Hg	(1/2+)
^189mTl		257.6(13) keV			1.4(1) min	β⁺ (96%)	¹⁸⁹Hg	(9/2−)
^189mTl		257.6(13) keV			1.4(1) min	IT (4%)	¹⁸⁹Tl	(9/2−)
¹⁹⁰Tl		81	109	189.97388(5)	2.6(3) min	β⁺	¹⁹⁰Hg	2(−)
^190m1Tl		130(90)# keV			3.7(3) min	β⁺	¹⁹⁰Hg	7(+#)
^190m2Tl		290(70)# keV			750(40) μs			(8−)
^190m3Tl		410(70)# keV			>1 μs			9−
¹⁹¹Tl		81	110	190.971786(8)	20# min	β⁺	¹⁹¹Hg	(1/2+)
^191mTl		297(7) keV			5.22(16) min	β⁺	¹⁹¹Hg	9/2(−)
¹⁹²Tl		81	111	191.97223(3)	9.6(4) min	β⁺	¹⁹²Hg	(2−)
^192m1Tl		160(50) keV			10.8(2) min	β⁺	¹⁹²Hg	(7+)
^192m2Tl		407(54) keV			296(5) ns			(8−)
¹⁹³Tl		81	112	192.97067(12)	21.6(8) min	β⁺	¹⁹³Hg	1/2(+#)
^193mTl		369(4) keV			2.11(15) min	IT (75%)	¹⁹³Tl	9/2−
^193mTl		369(4) keV			2.11(15) min	β⁺ (25%)	¹⁹³Hg	9/2−
¹⁹⁴Tl		81	113	193.97120(15)	33.0(5) min	β⁺	¹⁹⁴Hg	2−
¹⁹⁴Tl		81	113	193.97120(15)	33.0(5) min	α (10⁻⁷%)	¹⁹⁰Au	2−
^194mTl		300(200)# keV			32.8(2) min	β⁺	¹⁹⁴Hg	(7+)
¹⁹⁵Tl		81	114	194.969774(15)	1.16(5) h	β⁺	¹⁹⁵Hg	1/2+
^195mTl		482.63(17) keV			3.6(4) s	IT	¹⁹⁵Tl	9/2−
¹⁹⁶Tl		81	115	195.970481(13)	1.84(3) h	β⁺	¹⁹⁶Hg	2−
^196mTl		394.2(5) keV			1.41(2) h	β⁺ (95.5%)	¹⁹⁶Hg	(7+)
^196mTl		394.2(5) keV			1.41(2) h	IT (4.5%)	¹⁹⁶Tl	(7+)
¹⁹⁷Tl		81	116	196.969575(18)	2.84(4) h	β⁺	¹⁹⁷Hg	1/2+
^197mTl		608.22(8) keV			540(10) ms	IT	¹⁹⁷Tl	9/2−
¹⁹⁸Tl		81	117	197.97048(9)	5.3(5) h	β⁺	¹⁹⁸Hg	2−
^198m1Tl		543.5(4) keV			1.87(3) h	β⁺ (54%)	¹⁹⁸Hg	7+
^198m1Tl		543.5(4) keV			1.87(3) h	IT (46%)	¹⁹⁸Tl	7+
^198m2Tl		687.2(5) keV			150(40) ns			(5+)
^198m3Tl		742.3(4) keV			32.1(10) ms			(10−)#
¹⁹⁹Tl		81	118	198.96988(3)	7.42(8) h	β⁺	¹⁹⁹Hg	1/2+
^199mTl		749.7(3) keV			28.4(2) ms	IT	¹⁹⁹Tl	9/2−
²⁰⁰Tl		81	119	199.970963(6)	26.1(1) h	β⁺	²⁰⁰Hg	2−
^200m1Tl		753.6(2) keV			34.3(10) ms	IT	²⁰⁰Tl	7+
^200m2Tl		762.0(2) keV			0.33(5) μs			5+
²⁰¹Tl^{[n 8]}		81	120	200.970819(16)	72.912(17) h	EC	²⁰¹Hg	1/2+
^201mTl		919.50(9) keV			2.035(7) ms	IT	²⁰¹Tl	(9/2−)
²⁰²Tl		81	121	201.972106(16)	12.23(2) d	β⁺	²⁰²Hg	2−
^202mTl		950.19(10) keV			572(7) μs			7+
²⁰³Tl		81	122	202.9723442(14)	Observationally Stable^{[n 9]}			1/2+	0.2952(1)	0.29494–0.29528
^203mTl		3400(300) keV			7.7(5) μs			(25/2+)
²⁰⁴Tl		81	123	203.9738635(13)	3.78(2) y	β⁻ (97.1%)	²⁰⁴Pb	2−
²⁰⁴Tl		81	123	203.9738635(13)	3.78(2) y	EC (2.9%)	²⁰⁴Hg	2−
^204m1Tl		1104.0(4) keV			63(2) μs			(7)+
^204m2Tl		2500(500) keV			2.6(2) μs			(12−)
^204m3Tl		3500(500) keV			1.6(2) μs			(20+)
²⁰⁵Tl^{[n 10]}		81	124	204.9744275(14)	Observationally Stable^{[n 11]}^{[n 12]}			1/2+	0.7048(1)	0.70472–0.70506
^205m1Tl		3290.63(17) keV			2.6(2) μs			25/2+
^205m2Tl		4835.6(15) keV			235(10) ns			(35/2–)
²⁰⁶Tl	Radium E	81	125	205.9761103(15)	4.200(17) min	β⁻	²⁰⁶Pb	0−	Trace^{[n 13]}
^206mTl		2643.11(19) keV			3.74(3) min	IT	²⁰⁶Tl	(12–)
²⁰⁷Tl	Actinium C	81	126	206.977419(6)	4.77(2) min	β⁻	²⁰⁷Pb	1/2+	Trace^{[n 14]}
^207mTl		1348.1(3) keV			1.33(11) s	IT (99.9%)	²⁰⁷Tl	11/2–
^207mTl		1348.1(3) keV			1.33(11) s	β⁻ (.1%)	²⁰⁷Pb	11/2–
²⁰⁸Tl	Thorium C"	81	127	207.9820187(21)	3.053(4) min	β⁻	²⁰⁸Pb	5+	Trace^{[n 15]}
²⁰⁹Tl		81	128	208.985359(8)	2.161(7) min	β⁻	²⁰⁹Pb	1/2+	Trace^{[n 16]}
²¹⁰Tl	Radium C″	81	129	209.990074(12)	1.30(3) min	β⁻ (99.991%)	²¹⁰Pb	(5+)#	Trace^{[n 13]}
²¹⁰Tl	Radium C″	81	129	209.990074(12)	1.30(3) min	β⁻, n (.009%)	²⁰⁹Pb	(5+)#	Trace^{[n 13]}
²¹¹Tl		81	130	210.993480(50)	80(16) s	β⁻ (97.8%)	²¹¹Pb	1/2+
²¹¹Tl		81	130	210.993480(50)	80(16) s	β⁻, n (2.2%)	²¹⁰Pb	1/2+
²¹²Tl		81	131	211.998340(220)#	31(8) s	β⁻ (98.2%)	²¹²Pb	(5+)
²¹²Tl		81	131	211.998340(220)#	31(8) s	β⁻, n (1.8%)	²¹¹Pb	(5+)
²¹³Tl		81	132	213.001915(29)	24(4) s	β⁻ (92.4%)	²¹³Pb	1/2+
²¹³Tl		81	132	213.001915(29)	24(4) s	β⁻, n (7.6%)	²¹²Pb	1/2+
²¹⁴Tl		81	133	214.006940(210)#	11(2) s	β⁻ (66%)	²¹⁴Pb	5+#
²¹⁴Tl		81	133	214.006940(210)#	11(2) s	β⁻, n (34%)	²¹³Pb	5+#
²¹⁵Tl		81	134	215.010640(320)#	10(4) s	β⁻ (95.4%)	²¹⁵Pb	1/2+#
²¹⁵Tl		81	134	215.010640(320)#	10(4) s	β⁻, n (4.6%)	²¹⁴Pb	1/2+#
²¹⁶Tl		81	135	216.015800(320)#	6(3) s	β⁻	²¹⁶Pb	5+#
²¹⁶Tl		81	135	216.015800(320)#	6(3) s	β⁻, n (<11.5%)	²¹⁵Pb	5+#
This table header & footer: view

^ ^mTl – 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 ^c # – 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

n: Neutron emission

p: Proton emission
^ Bold symbol as daughter – Daughter product is stable.
^ ( ) spin value – Indicates spin with weak assignment arguments.
^ Main isotope used in scintigraphy
^ Believed to undergo α decay to ¹⁹⁹Au
^ Final decay product of 4n+1 decay chain (the Neptunium series)
^ Believed to undergo α decay to ²⁰¹Au
^ Can undergo bound-state β⁻ decay to ²⁰⁵Pb⁸¹⁺ with a half-life of 291+33
−27 days when fully ionized^[7]
^ ^a ^b Intermediate decay product of ²³⁸U
^ Intermediate decay product of ²³⁵U
^ Intermediate decay product of ²³²Th
^ Intermediate decay product of ²³⁷Np

Thallium-201

Thallium-201 (²⁰¹Tl) is a synthetic radioisotope of thallium. It has a half-life of 73 hours and decays by electron capture, emitting X-rays (~70–80 keV), and photons of 135 and 167 keV in 10% total abundance.^[18] Thallium-201 is synthesized by the neutron activation of stable thallium in a nuclear reactor,^[18]^[19] or by the ²⁰³Tl(p, 3n)²⁰¹Pb nuclear reaction in cyclotrons, as ²⁰¹Pb naturally decays to ²⁰¹Tl afterwards.^[20] It is a radiopharmaceutical, as it has good imaging characteristics without excessive patient radiation dose. It is the most popular isotope used for thallium nuclear cardiac stress tests.^[21]

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: Thallium". CIAAW. 2009.
^ 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.
^ "Thallium Research". doe.gov. Department of Energy. Archived from the original on 2006-12-09. Retrieved 23 March 2018.
^ Manual for reactor produced radioisotopes from the International Atomic Energy Agency
^ "Bound-state beta decay of highly ionized atoms" (PDF). Archived from the original (PDF) on October 29, 2013. Retrieved June 9, 2013.
^ ^a ^b Bai, M.; Blaum, K.; Boev, B.; Bosch, F.; Brandau, C.; Cvetković, V.; Dickel, T.; Dillmann, I.; Dmytriiev, D.; Faestermann, T.; Forstner, O.; Franczak, B.; Geissel, H.; Gernhäuser, R.; Glorius, J.; Griffin, C. J.; Gumberidze, A.; Haettner, E.; Hillenbrand, P.-M.; Kienle, P.; Korten, W.; Kozhuharov, Ch.; Kuzminchuk, N.; Langanke, K.; Litvinov, S.; Menz, E.; Morgenroth, T.; Nociforo, C.; Nolden, F.; Pavićević, M. K.; Petridis, N.; Popp, U.; Purushothaman, S.; Reifarth, R.; Sanjari, M. S.; Scheidenberger, C.; Spillmann, U.; Steck, M.; Stöhlker, Th.; Tanaka, Y. K.; Trassinelli, M.; Trotsenko, S.; Varga, L.; Wang, M.; Weick, H.; Woods, P. J.; Yamaguchi, T.; Zhang, Y. H.; Zhao, J.; Zuber, K.; et al. (E121 Collaboration and LOREX Collaboration) (2 December 2024). "Bound-State Beta Decay of ²⁰⁵Tl⁸¹⁺ Ions and the LOREX Project". Physical Review Letters. 133 (23). American Physical Society: 232701. doi:10.1103/PhysRevLett.133.232701.
^ Marcillac, P.; Coron, N.; Dambier, G.; et al. (2003). "Experimental detection of α-particles from the radioactive decay of natural bismuth". Nature. 422 (6934): 876–878. Bibcode:2003Natur.422..876D. doi:10.1038/nature01541. PMID 12712201. S2CID 4415582.
^ 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.
^ Al-Aqeel, Muneerah Abdullah M. "Decay Spectroscopy of the Thallium Isotopes 176,177Tl". University of Liverpool. ProQuest 2447566201. Retrieved 21 June 2023.
^ Poli, G. L.; Davids, C. N.; Woods, P. J.; Seweryniak, D.; Batchelder, J. C.; Brown, L. T.; Bingham, C. R.; Carpenter, M. P.; Conticchio, L. F.; Davinson, T.; DeBoer, J.; Hamada, S.; Henderson, D. J.; Irvine, R. J.; Janssens, R. V. F.; Maier, H. J.; Müller, L.; Soramel, F.; Toth, K. S.; Walters, W. B.; Wauters, J. (1 June 1999). "Proton and $\ensuremath{\alpha}$ radioactivity below the $Z=82$ shell closure". Physical Review C. 59 (6): R2979–R2983. doi:10.1103/PhysRevC.59.R2979. Retrieved 21 June 2023.
^ Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.
^ Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.
^ Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.
^ Reich, E. S. (2010). "Mercury serves up a nuclear surprise: a new type of fission". Scientific American. Retrieved 12 May 2011.
^ Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.
^ ^a ^b 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
^ "Manual for reactor produced radioisotopes" (PDF). International Atomic Energy Agency. 2003. Archived (PDF) from the original on 2011-05-21. Retrieved 2010-05-13.
^ Cyclotron Produced Radionuclides: Principles and Practice (PDF). International Atomic Energy Agency. 2008. ISBN 9789201002082. Retrieved 2022-07-01.
^ Maddahi, Jamshid; Berman, Daniel (2001). "Detection, Evaluation, and Risk Stratification of Coronary Artery Disease by Thallium-201 Myocardial Perfusion Scintigraphy 155". Cardiac SPECT imaging (2nd ed.). Lippincott Williams & Wilkins. pp. 155–178. ISBN 978-0-7817-2007-6. Archived from the original on 2017-02-22. Retrieved 2016-09-26.

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.

[10] Tl – Excited nuclear isomer.

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

[TMS-13] # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).

[TNN-14] # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

[15] Modes of decay:

EC: Electron capture

IT: Isomeric transition

n: Neutron emission

p: Proton emission

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

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

[25] Main isotope used in scintigraphy

[26] Believed to undergo α decay to ¹⁹⁹Au

[27] Final decay product of 4n+1 decay chain (the Neptunium series)

[28] Believed to undergo α decay to ²⁰¹Au

[29] Can undergo bound-state β⁻ decay to ²⁰⁵Pb⁸¹⁺ with a half-life of 291+33
−27 days when fully ionized^[7]

[Th-30] Intermediate decay product of ²³⁸U

[31] Intermediate decay product of ²³⁵U

[32] Intermediate decay product of ²³²Th

[33] Intermediate decay product of ²³⁷Np

[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: Thallium". CIAAW. 2009.

[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.

[4] "Thallium Research". doe.gov. Department of Energy. Archived from the original on 2006-12-09. Retrieved 23 March 2018.

[5] Manual for reactor produced radioisotopes from the International Atomic Energy Agency

[6] "Bound-state beta decay of highly ionized atoms" (PDF). Archived from the original (PDF) on October 29, 2013. Retrieved June 9, 2013.

[Tl-205-7] Bai, M.; Blaum, K.; Boev, B.; Bosch, F.; Brandau, C.; Cvetković, V.; Dickel, T.; Dillmann, I.; Dmytriiev, D.; Faestermann, T.; Forstner, O.; Franczak, B.; Geissel, H.; Gernhäuser, R.; Glorius, J.; Griffin, C. J.; Gumberidze, A.; Haettner, E.; Hillenbrand, P.-M.; Kienle, P.; Korten, W.; Kozhuharov, Ch.; Kuzminchuk, N.; Langanke, K.; Litvinov, S.; Menz, E.; Morgenroth, T.; Nociforo, C.; Nolden, F.; Pavićević, M. K.; Petridis, N.; Popp, U.; Purushothaman, S.; Reifarth, R.; Sanjari, M. S.; Scheidenberger, C.; Spillmann, U.; Steck, M.; Stöhlker, Th.; Tanaka, Y. K.; Trassinelli, M.; Trotsenko, S.; Varga, L.; Wang, M.; Weick, H.; Woods, P. J.; Yamaguchi, T.; Zhang, Y. H.; Zhao, J.; Zuber, K.; et al. (E121 Collaboration and LOREX Collaboration) (2 December 2024). "Bound-State Beta Decay of ²⁰⁵Tl⁸¹⁺ Ions and the LOREX Project". Physical Review Letters. 133 (23). American Physical Society: 232701. doi:10.1103/PhysRevLett.133.232701.

[8] Marcillac, P.; Coron, N.; Dambier, G.; et al. (2003). "Experimental detection of α-particles from the radioactive decay of natural bismuth". Nature. 422 (6934): 876–878. Bibcode:2003Natur.422..876D. doi:10.1038/nature01541. PMID 12712201. S2CID 4415582.

[NUBASE2016-9] 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-11] 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.

[18] Al-Aqeel, Muneerah Abdullah M. "Decay Spectroscopy of the Thallium Isotopes 176,177Tl". University of Liverpool. ProQuest 2447566201. Retrieved 21 June 2023.

[19] Poli, G. L.; Davids, C. N.; Woods, P. J.; Seweryniak, D.; Batchelder, J. C.; Brown, L. T.; Bingham, C. R.; Carpenter, M. P.; Conticchio, L. F.; Davinson, T.; DeBoer, J.; Hamada, S.; Henderson, D. J.; Irvine, R. J.; Janssens, R. V. F.; Maier, H. J.; Müller, L.; Soramel, F.; Toth, K. S.; Walters, W. B.; Wauters, J. (1 June 1999). "Proton and $\ensuremath{\alpha}$ radioactivity below the $Z=82$ shell closure". Physical Review C. 59 (6): R2979–R2983. doi:10.1103/PhysRevC.59.R2979. Retrieved 21 June 2023.

[20] Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.

[21] Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.

[22] Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.

[23] Reich, E. S. (2010). "Mercury serves up a nuclear surprise: a new type of fission". Scientific American. Retrieved 12 May 2011.

[24] Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641.

[Audi-34] 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

[35] "Manual for reactor produced radioisotopes" (PDF). International Atomic Energy Agency. 2003. Archived (PDF) from the original on 2011-05-21. Retrieved 2010-05-13.

[36] Cyclotron Produced Radionuclides: Principles and Practice (PDF). International Atomic Energy Agency. 2008. ISBN 9789201002082. Retrieved 2022-07-01.

[37] Maddahi, Jamshid; Berman, Daniel (2001). "Detection, Evaluation, and Risk Stratification of Coronary Artery Disease by Thallium-201 Myocardial Perfusion Scintigraphy 155". Cardiac SPECT imaging (2nd ed.). Lippincott Williams & Wilkins. pp. 155–178. ISBN 978-0-7817-2007-6. Archived from the original on 2017-02-22. Retrieved 2016-09-26.

[1]

[2]

[3]

[4]

[5]

[6]

[7]

[8]

[9]

[n 1]

[10]

[n 2]

[n 3]

[n 4]

[n 5]

[n 6]

[n 7]

[11]

[12]

[13]

[14]

[15]

[16]

[17]

[n 8]

[n 9]

[n 10]

[n 11]

[n 12]

[n 13]

[n 14]

[n 15]

[n 16]

[18]

[19]

[20]

[21]

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