Template:Isotopes table/testcases2

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This list:

#List of isotopes

① Z=1 H
He
② 3 Li
Be
B
C
N
O
F
Ne
③ 11 Na
Mg
Al
Si
P
S
Cl
Ar
④ 19 K
Ca
Sc
Ti
V
Cr
Mn
Fe
Co
Ni
Cu
Zn
Ga
Ge
As
Se
Br
Kr
⑤ 37 Rb
Sr
Y
Zr
Nb
Mo
Tc
Ru
Rh
Pd
Ag
Cd
In
Sn
Sb
Te
I
Xe
⑥ 55 Cs
Ba
La
Ce
Pr
Nd
Pm
Sm
Eu
Gd
Tb
Dy
Ho
Er
Tm
Yb
Lu
Hf
Ta
W
Re
Os
Ir
Pt
Au
Hg
Tl
Pb
Bi
Po
At
Rn
⑦ 87 Fr
Ra
Ac
Th
Pa
U
Np
Pu
Am
Cm
Bk
Cf
Es
Fm
Md
No
Lr
Rf
Db
Sg
Bh
Hs
Mt
Ds
Rg
Cn
Nh
Fl
Mc
Lv
Ts
Og
⑧ 119 Uue
Ubn
Ubu R
Ubb R
Category:Lists of isotopes by element (122)
Category:Isotope content page (65)
{{Isotopes table}}

H[edit]

H old[edit]

nuclide symbol	Z(p)	N(n)	isotopic mass (u)^[1]	half-life [resonance width]	decay mode(s)^[2]	daughter isotope(s)^{[n 1]}	nuclear spin and parity	representative isotopic composition (mole fraction)^{[n 2]}	range of natural variation (mole fraction)
¹H	1	0	1.00782503224(9)	Stable^{[n 3]}^{[n 4]}			1⁄2⁺	0.999885(70)	0.999816–0.999974
²H (D)^{[n 5]}	1	1	2.01410177811(12)	Stable			1⁺	0.000115(70)^{[n 6]}	0.000026–0.000184
³H (T)^{[n 7]}	1	2	3.01604928199(23)	12.32(2) y	β⁻	³ He	1⁄2⁺	Trace^{[n 8]}
⁴ H	1	3	4.02643(11)	1.39(10)×10⁻²² s [3.28(23) MeV]	n	³ H	2⁻
⁵ H	1	4	5.03531(10)	> 9.1×10⁻²² s [< 0.5 MeV]	2n	³ H	(1⁄2⁺)
⁶ H	1	5	6.04496(27)	2.90(70)×10⁻²² s [1.6(4) MeV]	3n	³ H	2⁻#
⁶ H	1	5	6.04496(27)	2.90(70)×10⁻²² s [1.6(4) MeV]	4n	² H	2⁻#
⁷ H	1	6	7.05275(108)#	5×10⁻²² s#	4n	³ H	1⁄2⁺#

^ Bold for stable isotopes.
^ Refers to that in water.
^ Unless proton decay occurs.
^ This and ³He are the only stable nuclides with more protons than neutrons.
^ Produced during Big Bang nucleosynthesis.
^ Tank hydrogen has a ²
H
abundance as low as 3.2×10⁻⁵ (mole fraction).
^ Produced during Big Bang nucleosynthesis, but not primordial, as all such atoms have since decayed to ³He.
^ Cosmogenic

Notes

Commercially available materials may have been subjected to an undisclosed or inadvertent isotopic fractionation. Substantial deviations from the given mass and composition can occur.
Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.
Isotope abundances are given by IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)

H new[edit]

Testing: H, isotopes of hydrogen (notes:mass#, unc(), var[], resonance, daughter-st; refs:NUBASE2016, AME2016)
rows=2 +HistName=no +TracesOnly=no +AbuNaturalVar_2cols=yes +ExEn=no

Nuclide^[2]	Z	N	Isotopic mass (Da)^[1] ^{[n 1]}	Half-life [resonance width]	Decay mode	Daughter isotope ^{[n 2]}	Spin and parity	Natural abundance (mole fraction)
Nuclide^[2]	Z	N	Isotopic mass (Da)^[1] ^{[n 1]}	Half-life [resonance width]	Decay mode	Daughter isotope ^{[n 2]}	Spin and parity	Normal proportion	Range of variation
¹H	1	0	1.00782503224(9)	Stable^{[n 3]}^{[n 4]}			1⁄2⁺	0.999885(70)	0.999816–0.999974
²H (D)^{[n 5]}	1	1	2.01410177811(12)	Stable			1⁺	0.000115(70)^{[n 6]}	0.000026–0.000184
³H (T)^{[n 7]}	1	2	3.01604928199(23)	12.32(2) y	β⁻	³ He	1⁄2⁺	Trace^{[n 8]}
⁴ H	1	3	4.02643(11)	1.39(10)×10⁻²² s [3.28(23) MeV]	n	³ H	2⁻
⁵ H	1	4	5.03531(10)	> 9.1×10⁻²² s [< 0.5 MeV]	2n	³ H	(1⁄2⁺)
⁶ H	1	5	6.04496(27)	2.90(70)×10⁻²² s [1.6(4) MeV]	3n	³ H	2⁻#
⁶ H	1	5	6.04496(27)	2.90(70)×10⁻²² s [1.6(4) MeV]	4n	² H	2⁻#
⁷ H	1	6	7.05275(108)#	5×10⁻²² s#	4n	³ H	1⁄2⁺#
This table header & footer: view

^ ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
^ Bold symbol as daughter – Daughter product is stable.
^ Unless proton decay occurs.
^ This and ³He are the only stable nuclides with more protons than neutrons.
^ Produced during Big Bang nucleosynthesis.
^ Tank hydrogen has a ²
H
abundance as low as 3.2×10⁻⁵ (mole fraction).
^ Produced during Big Bang nucleosynthesis, but not primordial, as all such atoms have since decayed to ³He.
^ Cosmogenic

Notes

Commercially available materials may have been subjected to an undisclosed or inadvertent isotopic fractionation. Substantial deviations from the given mass and composition can occur.
Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.
Isotope abundances are given by IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)

Tc[edit]

Tc old[edit]

nuclide symbol	Z(p)	N(n)	isotopic mass (u)	half-life	decay mode(s)^{[n 1]}	daughter isotope(s)^{[n 2]}	nuclear spin and parity	representative isotopic composition (mole fraction)
nuclide symbol	excitation energy			half-life	decay mode(s)^{[n 1]}	daughter isotope(s)^{[n 2]}	nuclear spin and parity	representative isotopic composition (mole fraction)
⁸⁵Tc	43	42	84.94883(43)#	<110 ns	β⁺	⁸⁵Mo	1/2−#
					p	⁸⁴Mo
					β⁺, p	⁸⁴Nb
⁸⁶Tc	43	43	85.94288(32)#	55(6) ms	β⁺	⁸⁶Mo	(0+)
^86mTc	1500(150) keV			1.11(21) µs			(5+,5−)
⁸⁷Tc	43	44	86.93653(32)#	2.18(16) s	β⁺	⁸⁷Mo	1/2−#
^87mTc	20(60)# keV			2# s			9/2+#
⁸⁸Tc	43	45	87.93268(22)#	5.8(2) s	β⁺	⁸⁸Mo	(2,3)
^88mTc	0(300)# keV			6.4(8) s	β⁺	⁸⁸Mo	(6,7,8)
⁸⁹Tc	43	46	88.92717(22)#	12.8(9) s	β⁺	⁸⁹Mo	(9/2+)
^89mTc	62.6(5) keV			12.9(8) s	β⁺	⁸⁹Mo	(1/2−)
⁹⁰Tc	43	47	89.92356(26)	8.7(2) s	β⁺	⁹⁰Mo	1+
^90mTc	310(390) keV			49.2(4) s	β⁺	⁹⁰Mo	(8+)
⁹¹Tc	43	48	90.91843(22)	3.14(2) min	β⁺	⁹¹Mo	(9/2)+
^91mTc	139.3(3) keV			3.3(1) min	β⁺ (99%)	⁹¹Mo	(1/2)−
^91mTc	139.3(3) keV			3.3(1) min	IT (1%)	⁹¹Tc	(1/2)−
⁹²Tc	43	49	91.915260(28)	4.25(15) min	β⁺	⁹²Mo	(8)+
^92mTc	270.15(11) keV			1.03(7) µs			(4+)
⁹³Tc	43	50	92.910249(4)	2.75(5) h	β⁺	⁹³Mo	9/2+
^93m1Tc	391.84(8) keV			43.5(10) min	IT (76.6%)	⁹³Tc	1/2−
^93m1Tc	391.84(8) keV			43.5(10) min	β⁺ (23.4%)	⁹³Mo	1/2−
^93m2Tc	2185.16(15) keV			10.2(3) µs			(17/2)−
⁹⁴Tc	43	51	93.909657(5)	293(1) min	β⁺	⁹⁴Mo	7+
^94mTc	75.5(19) keV			52.0(10) min	β⁺ (99.9%)	⁹⁴Mo	(2)+
^94mTc	75.5(19) keV			52.0(10) min	IT (.1%)	⁹⁴Tc	(2)+
⁹⁵Tc	43	52	94.907657(6)	20.0(1) h	β⁺	⁹⁵Mo	9/2+
^95mTc	38.89(5) keV			61(2) d	β⁺ (96.12%)	⁹⁵Mo	1/2−
^95mTc	38.89(5) keV			61(2) d	IT (3.88%)	⁹⁵Tc	1/2−
⁹⁶Tc	43	53	95.907871(6)	4.28(7) d	β⁺	⁹⁶Mo	7+
^96mTc	34.28(7) keV			51.5(10) min	IT (98%)	⁹⁶Tc	4+
^96mTc	34.28(7) keV			51.5(10) min	β⁺ (2%)	⁹⁶Mo	4+
⁹⁷Tc	43	54	96.906365(5)	4.21×10⁶ a	EC	⁹⁷Mo	9/2+
^97mTc	96.56(6) keV			91.0(6) d	IT (99.66%)	⁹⁷Tc	1/2−
^97mTc	96.56(6) keV			91.0(6) d	EC (.34%)	⁹⁷Mo	1/2−
⁹⁸Tc	43	55	97.907216(4)	4.2×10⁶ a	β⁻	⁹⁸Ru	(6)+
^98mTc	90.76(16) keV			14.7(3) µs			(2)−
⁹⁹Tc^{[n 3]}	43	56	98.9062547(21)	2.111(12)×10⁵ a	β⁻	⁹⁹Ru	9/2+
^99mTc^{[n 4]}	142.6832(11) keV			6.0067(5) h	IT (99.99%)	⁹⁹Tc	1/2−
^99mTc^{[n 4]}	142.6832(11) keV			6.0067(5) h	β⁻ (.0037%)	⁹⁹Ru	1/2−
¹⁰⁰Tc	43	57	99.9076578(24)	15.8(1) s	β⁻ (99.99%)	¹⁰⁰Ru	1+
¹⁰⁰Tc	43	57	99.9076578(24)	15.8(1) s	EC (.0018%)	¹⁰⁰Mo	1+
^100m1Tc	200.67(4) keV			8.32(14) µs			(4)+
^100m2Tc	243.96(4) keV			3.2(2) µs			(6)+
¹⁰¹Tc	43	58	100.907315(26)	14.22(1) min	β⁻	¹⁰¹Ru	9/2+
^101mTc	207.53(4) keV			636(8) µs			1/2−
¹⁰²Tc	43	59	101.909215(10)	5.28(15) s	β⁻	¹⁰²Ru	1+
^102mTc	20(10) keV			4.35(7) min	β⁻ (98%)	¹⁰²Ru	(4,5)
^102mTc	20(10) keV			4.35(7) min	IT (2%)	¹⁰²Tc	(4,5)
¹⁰³Tc	43	60	102.909181(11)	54.2(8) s	β⁻	¹⁰³Ru	5/2+
¹⁰⁴Tc	43	61	103.91145(5)	18.3(3) min	β⁻	¹⁰⁴Ru	(3+)#
^104m1Tc	69.7(2) keV			3.5(3) µs			2(+)
^104m2Tc	106.1(3) keV			0.40(2) µs			(+)
¹⁰⁵Tc	43	62	104.91166(6)	7.6(1) min	β⁻	¹⁰⁵Ru	(3/2−)
¹⁰⁶Tc	43	63	105.914358(14)	35.6(6) s	β⁻	¹⁰⁶Ru	(1,2)
¹⁰⁷Tc	43	64	106.91508(16)	21.2(2) s	β⁻	¹⁰⁷Ru	(3/2−)
^107mTc	65.7(10) keV			184(3) ns			(5/2−)
¹⁰⁸Tc	43	65	107.91846(14)	5.17(7) s	β⁻	¹⁰⁸Ru	(2)+
¹⁰⁹Tc	43	66	108.91998(10)	860(40) ms	β⁻ (99.92%)	¹⁰⁹Ru	3/2−#
¹⁰⁹Tc	43	66	108.91998(10)	860(40) ms	β⁻, n (.08%)	¹⁰⁸Ru	3/2−#
¹¹⁰Tc	43	67	109.92382(8)	0.92(3) s	β⁻ (99.96%)	¹¹⁰Ru	(2+)
¹¹⁰Tc	43	67	109.92382(8)	0.92(3) s	β⁻, n (.04%)	¹⁰⁹Ru	(2+)
¹¹¹Tc	43	68	110.92569(12)	290(20) ms	β⁻ (99.15%)	¹¹¹Ru	3/2−#
¹¹¹Tc	43	68	110.92569(12)	290(20) ms	β⁻, n (.85%)	¹¹⁰Ru	3/2−#
¹¹²Tc	43	69	111.92915(13)	290(20) ms	β⁻ (97.4%)	¹¹²Ru	2+#
¹¹²Tc	43	69	111.92915(13)	290(20) ms	β⁻, n (2.6%)	¹¹¹Ru	2+#
¹¹³Tc	43	70	112.93159(32)#	170(20) ms	β⁻	¹¹³Ru	3/2−#
¹¹⁴Tc	43	71	113.93588(64)#	150(30) ms	β⁻	¹¹⁴Ru	2+#
¹¹⁵Tc	43	72	114.93869(75)#	100# ms [>300 ns]	β⁻	¹¹⁵Ru	3/2−#
¹¹⁶Tc	43	73	115.94337(75)#	90# ms [>300 ns]			2+#
¹¹⁷Tc	43	74	116.94648(75)#	40# ms [>300 ns]			3/2−#
¹¹⁸Tc	43	75	117.95148(97)#	30# ms [>300 ns]			2+#

^ Abbreviations:
EC: Electron capture
IT: Isomeric transition
^ Bold for stable isotopes, bold italics for nearly-stable isotopes (half-life longer than the age of the universe)
^ Long-lived fission product
^ Used in medicine

Notes

Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.

Tc new[edit]

Testing: Tc, isotopes of technetium (notes:m, daughter-nst, daughter-st, EC, IT, n, p, exen#, spin#, spin(), unc(); refs:)
rows=2 +HistName=no +TracesOnly=yes +AbuNaturalVar_2cols=no +ExEn=yes

Nuclide ^{[n 1]}	Z	N	Isotopic mass (Da) ^{[n 2]}	Half-life	Decay mode ^{[n 3]}	Daughter isotope ^{[n 4]}^{[n 5]}	Spin and parity ^{[n 6]}^{[n 7]}	Isotopic abundance
Nuclide ^{[n 1]}	Excitation energy^{[n 7]}			Half-life	Decay mode ^{[n 3]}	Daughter isotope ^{[n 4]}^{[n 5]}	Spin and parity ^{[n 6]}^{[n 7]}	Isotopic abundance
⁸⁵Tc	43	42	84.94883(43)#	<110 ns	β⁺	⁸⁵Mo	1/2−#
					p	⁸⁴Mo
					β⁺, p	⁸⁴Nb
⁸⁶Tc	43	43	85.94288(32)#	55(6) ms	β⁺	⁸⁶Mo	(0+)
^86mTc	1500(150) keV			1.11(21) µs			(5+,5−)
⁸⁷Tc	43	44	86.93653(32)#	2.18(16) s	β⁺	⁸⁷Mo	1/2−#
^87mTc	20(60)# keV			2# s			9/2+#
⁸⁸Tc	43	45	87.93268(22)#	5.8(2) s	β⁺	⁸⁸Mo	(2,3)
^88mTc	0(300)# keV			6.4(8) s	β⁺	⁸⁸Mo	(6,7,8)
⁸⁹Tc	43	46	88.92717(22)#	12.8(9) s	β⁺	⁸⁹Mo	(9/2+)
^89mTc	62.6(5) keV			12.9(8) s	β⁺	⁸⁹Mo	(1/2−)
⁹⁰Tc	43	47	89.92356(26)	8.7(2) s	β⁺	⁹⁰Mo	1+
^90mTc	310(390) keV			49.2(4) s	β⁺	⁹⁰Mo	(8+)
⁹¹Tc	43	48	90.91843(22)	3.14(2) min	β⁺	⁹¹Mo	(9/2)+
^91mTc	139.3(3) keV			3.3(1) min	β⁺ (99%)	⁹¹Mo	(1/2)−
^91mTc	139.3(3) keV			3.3(1) min	IT (1%)	⁹¹Tc	(1/2)−
⁹²Tc	43	49	91.915260(28)	4.25(15) min	β⁺	⁹²Mo	(8)+
^92mTc	270.15(11) keV			1.03(7) µs			(4+)
⁹³Tc	43	50	92.910249(4)	2.75(5) h	β⁺	⁹³Mo	9/2+
^93m1Tc	391.84(8) keV			43.5(10) min	IT (76.6%)	⁹³Tc	1/2−
^93m1Tc	391.84(8) keV			43.5(10) min	β⁺ (23.4%)	⁹³Mo	1/2−
^93m2Tc	2185.16(15) keV			10.2(3) µs			(17/2)−
⁹⁴Tc	43	51	93.909657(5)	293(1) min	β⁺	⁹⁴Mo	7+
^94mTc	75.5(19) keV			52.0(10) min	β⁺ (99.9%)	⁹⁴Mo	(2)+
^94mTc	75.5(19) keV			52.0(10) min	IT (.1%)	⁹⁴Tc	(2)+
⁹⁵Tc	43	52	94.907657(6)	20.0(1) h	β⁺	⁹⁵Mo	9/2+
^95mTc	38.89(5) keV			61(2) d	β⁺ (96.12%)	⁹⁵Mo	1/2−
^95mTc	38.89(5) keV			61(2) d	IT (3.88%)	⁹⁵Tc	1/2−
⁹⁶Tc	43	53	95.907871(6)	4.28(7) d	β⁺	⁹⁶Mo	7+
^96mTc	34.28(7) keV			51.5(10) min	IT (98%)	⁹⁶Tc	4+
^96mTc	34.28(7) keV			51.5(10) min	β⁺ (2%)	⁹⁶Mo	4+
⁹⁷Tc	43	54	96.906365(5)	4.21×10⁶ a	EC	⁹⁷Mo	9/2+
^97mTc	96.56(6) keV			91.0(6) d	IT (99.66%)	⁹⁷Tc	1/2−
^97mTc	96.56(6) keV			91.0(6) d	EC (.34%)	⁹⁷Mo	1/2−
⁹⁸Tc	43	55	97.907216(4)	4.2×10⁶ a	β⁻	⁹⁸Ru	(6)+
^98mTc	90.76(16) keV			14.7(3) µs			(2)−
⁹⁹Tc^{[n 8]}	43	56	98.9062547(21)	2.111(12)×10⁵ a	β⁻	⁹⁹Ru	9/2+
^99mTc^{[n 9]}	142.6832(11) keV			6.0067(5) h	IT (99.99%)	⁹⁹Tc	1/2−
^99mTc^{[n 9]}	142.6832(11) keV			6.0067(5) h	β⁻ (.0037%)	⁹⁹Ru	1/2−
¹⁰⁰Tc	43	57	99.9076578(24)	15.8(1) s	β⁻ (99.99%)	¹⁰⁰Ru	1+
¹⁰⁰Tc	43	57	99.9076578(24)	15.8(1) s	EC (.0018%)	¹⁰⁰Mo	1+
^100m1Tc	200.67(4) keV			8.32(14) µs			(4)+
^100m2Tc	243.96(4) keV			3.2(2) µs			(6)+
¹⁰¹Tc	43	58	100.907315(26)	14.22(1) min	β⁻	¹⁰¹Ru	9/2+
^101mTc	207.53(4) keV			636(8) µs			1/2−
¹⁰²Tc	43	59	101.909215(10)	5.28(15) s	β⁻	¹⁰²Ru	1+
^102mTc	20(10) keV			4.35(7) min	β⁻ (98%)	¹⁰²Ru	(4,5)
^102mTc	20(10) keV			4.35(7) min	IT (2%)	¹⁰²Tc	(4,5)
¹⁰³Tc	43	60	102.909181(11)	54.2(8) s	β⁻	¹⁰³Ru	5/2+
¹⁰⁴Tc	43	61	103.91145(5)	18.3(3) min	β⁻	¹⁰⁴Ru	(3+)#
^104m1Tc	69.7(2) keV			3.5(3) µs			2(+)
^104m2Tc	106.1(3) keV			0.40(2) µs			(+)
¹⁰⁵Tc	43	62	104.91166(6)	7.6(1) min	β⁻	¹⁰⁵Ru	(3/2−)
¹⁰⁶Tc	43	63	105.914358(14)	35.6(6) s	β⁻	¹⁰⁶Ru	(1,2)
¹⁰⁷Tc	43	64	106.91508(16)	21.2(2) s	β⁻	¹⁰⁷Ru	(3/2−)
^107mTc	65.7(10) keV			184(3) ns			(5/2−)
¹⁰⁸Tc	43	65	107.91846(14)	5.17(7) s	β⁻	¹⁰⁸Ru	(2)+
¹⁰⁹Tc	43	66	108.91998(10)	860(40) ms	β⁻ (99.92%)	¹⁰⁹Ru	3/2−#
¹⁰⁹Tc	43	66	108.91998(10)	860(40) ms	β⁻, n (.08%)	¹⁰⁸Ru	3/2−#
¹¹⁰Tc	43	67	109.92382(8)	0.92(3) s	β⁻ (99.96%)	¹¹⁰Ru	(2+)
¹¹⁰Tc	43	67	109.92382(8)	0.92(3) s	β⁻, n (.04%)	¹⁰⁹Ru	(2+)
¹¹¹Tc	43	68	110.92569(12)	290(20) ms	β⁻ (99.15%)	¹¹¹Ru	3/2−#
¹¹¹Tc	43	68	110.92569(12)	290(20) ms	β⁻, n (.85%)	¹¹⁰Ru	3/2−#
¹¹²Tc	43	69	111.92915(13)	290(20) ms	β⁻ (97.4%)	¹¹²Ru	2+#
¹¹²Tc	43	69	111.92915(13)	290(20) ms	β⁻, n (2.6%)	¹¹¹Ru	2+#
¹¹³Tc	43	70	112.93159(32)#	170(20) ms	β⁻	¹¹³Ru	3/2−#
¹¹⁴Tc	43	71	113.93588(64)#	150(30) ms	β⁻	¹¹⁴Ru	2+#
¹¹⁵Tc	43	72	114.93869(75)#	100# ms [>300 ns]	β⁻	¹¹⁵Ru	3/2−#
¹¹⁶Tc	43	73	115.94337(75)#	90# ms [>300 ns]			2+#
¹¹⁷Tc	43	74	116.94648(75)#	40# ms [>300 ns]			3/2−#
¹¹⁸Tc	43	75	117.95148(97)#	30# ms [>300 ns]			2+#

^ ^mTc – Excited nuclear isomer.
^ ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
^ Modes of decay:

EC: Electron capture

IT: Isomeric transition

n: Neutron emission

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.
^ ^a ^b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
^ Long-lived fission product
^ Used in medicine

Notes

Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.

U[edit]

U old[edit]

nuclide symbol	historic name	Z(p)	N(n)	isotopic mass (u)^[3]	half-life^[4]	decay mode(s)^[5] ^{[n 1]}	daughter isotope(s)^{[n 2]}	nuclear spin and parity	representative isotopic composition (mole fraction)	range of natural variation (mole fraction)
nuclide symbol	historic name	excitation energy			half-life^[4]	decay mode(s)^[5] ^{[n 1]}	daughter isotope(s)^{[n 2]}	nuclear spin and parity	representative isotopic composition (mole fraction)	range of natural variation (mole fraction)
²³⁵U^{[n 3]}^{[n 4]}^{[n 5]}	Actin Uranium Actino-Uranium	92	143	235.0439299(20)	7.04(1)×10⁸ y	α	²³¹Th	7/2−	[0.007204(6)]	0.007198– 0.007207
						SF (7×10⁻⁹%)	(various)
						CD (8×10⁻¹⁰%)	¹⁸⁶Hf ²⁵Ne ²⁴Ne
^235mU		0.0765(4) keV			~26 min	IT	²³⁵U	1/2+
²³⁶U	Thoruranium^[6]	92	144	236.045568(2)	2.342(3)×10⁷ y	α	²³²Th	0+
²³⁶U	Thoruranium^[6]	92	144	236.045568(2)	2.342(3)×10⁷ y	SF (9.6×10⁻⁸%)	(various)	0+
^236m1U		1052.89(19) keV			100(4) ns			(4)−
^236m2U		2750(10) keV			120(2) ns			(0+)
²³⁷U		92	145	237.0487302(20)	6.75(1) d	β⁻	²³⁷Np	1/2+
²³⁸U^{[n 6]}^{[n 3]}^{[n 4]}	Uranium I	92	146	238.0507882(20)	4.468(3)×10⁹ y	α	²³⁴Th	0+	[0.992742(10)]	0.992739– 0.992752
						SF (5.45×10⁻⁵%)	(various)
						β⁻β⁻ (2.19×10⁻¹⁰%)	²³⁸Pu
^238mU		2557.9(5) keV			280(6) ns			0+

^ Abbreviations:
CD: Cluster decay
EC: Electron capture
IT: Isomeric transition
SF: Spontaneous fission
^ Bold for stable isotopes, bold italics for nearly-stable isotopes (half-life longer than the age of the universe)
^ ^a ^b Primordial radionuclide
^ ^a ^b Used in Uranium–lead dating
^ Important in nuclear reactors
^ Used in uranium–uranium dating

+ Notes

U new[edit]

Nuclide^[2] ^{[n 1]}	Historic name	Z	N	Isotopic mass (Da)^[1]	Half-life	Decay mode ^{[n 2]}	Daughter isotope ^{[n 3]}	Spin and parity	Natural abundance (mole fraction)
Nuclide^[2] ^{[n 1]}	Historic name	Excitation energy			Half-life	Decay mode ^{[n 2]}	Daughter isotope ^{[n 3]}	Spin and parity	Normal proportion	Range of variation
²³⁵U^{[n 4]}^{[n 5]}^{[n 6]}	Actin Uranium Actino-Uranium	92	143	235.0439299(20)	7.04(1)×10⁸ y	α	²³¹Th	7/2−	[0.007204(6)]	0.007198– 0.007207
						SF (7×10⁻⁹%)	(various)
						CD (8×10⁻¹⁰%)	¹⁸⁶Hf ²⁵Ne ²⁴Ne
^235mU		0.0765(4) keV			~26 min	IT	²³⁵U	1/2+
²³⁶U	Thoruranium^[6]	92	144	236.045568(2)	2.342(3)×10⁷ y	α	²³²Th	0+
²³⁶U	Thoruranium^[6]	92	144	236.045568(2)	2.342(3)×10⁷ y	SF (9.6×10⁻⁸%)	(various)	0+
^236m1U		1052.89(19) keV			100(4) ns			(4)−
^236m2U		2750(10) keV			120(2) ns			(0+)
²³⁷U		92	145	237.0487302(20)	6.75(1) d	β⁻	²³⁷Np	1/2+
²³⁸U^{[n 7]}^{[n 4]}^{[n 5]}	Uranium I	92	146	238.0507882(20)	4.468(3)×10⁹ y	α	²³⁴Th	0+	[0.992742(10)]	0.992739– 0.992752
						SF (5.45×10⁻⁵%)	(various)
						β⁻β⁻ (2.19×10⁻¹⁰%)	²³⁸Pu
^238mU		2557.9(5) keV			280(6) ns			0+
This table header & footer: view

^ ^mU – Excited nuclear isomer.
^ 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.
^ ^a ^b Primordial radionuclide
^ ^a ^b Used in Uranium–lead dating
^ Important in nuclear reactors
^ Used in uranium–uranium dating

Hs[edit]

Hs old[edit]

nuclide symbol	Z(p)	N(n)	Isotopic mass (u)	Half-life	Decay mode(s)	Daughter isotope(s)	Nuclear spin and parity
nuclide symbol	Excitation energy			Half-life	Decay mode(s)	Daughter isotope(s)	Nuclear spin and parity
²⁶³Hs	108	155	263.12856(37)#	760(40) µs	α	²⁵⁹Sg	7/2+#
²⁶⁴Hs	108	156	264.12836(3)	540(300) µs	α (50%)	²⁶⁰Sg	0+
²⁶⁴Hs	108	156	264.12836(3)	540(300) µs	SF (50%)	(various)	0+
²⁶⁵Hs	108	157	265.129793(26)	1.96(0.16) ms	α	²⁶¹Sg	9/2+#
^265mHs	300(70) keV			360(150) µs	α	²⁶¹Sg	3/2+#
²⁶⁶Hs^{[n 1]}	108	158	266.13005(4)	3.02(0.54) ms	α (68%)	²⁶²Sg	0+
²⁶⁶Hs^{[n 1]}	108	158	266.13005(4)	3.02(0.54) ms	SF (32%)^[7]	(various)	0+
^266mHs	1100(70) keV			280(220) ms	α	²⁶²Sg	9-#
²⁶⁷Hs	108	159	267.13167(10)#	55(11) ms	α	²⁶³Sg	5/2+#
^267mHs^{[n 2]}	39(24) keV			990(90) µs	α	²⁶³Sg
²⁶⁸Hs	108	160	268.13187(30)#	1.42(1.13) s	α	²⁶⁴Sg	0+
²⁶⁹Hs^{[n 3]}	108	161	269.13375(13)#	16 s	α	²⁶⁵Sg	9/2+#
²⁷⁰Hs	108	162	270.13429(27)#	10 s	α	²⁶⁶Sg	0+
²⁷¹Hs	108	163	271.13717(32)#	~4 s	α	²⁶⁷Sg
²⁷³Hs^{[n 4]}	108	165	273.14168(40)#	510 ms^[8]	α	²⁶⁹Sg	3/2+#
²⁷⁵Hs^{[n 5]}	108	167	275.14667(63)#	290(150) ms	α	²⁷¹Sg
²⁷⁷Hs^{[n 6]}	108	169	277.15190(58)#	11(9) ms	SF	(various)	3/2+#

^ Not directly synthesized, occurs as decay product of ²⁷⁰Ds
^ Existence of this isomer is unconfirmed
^ Not directly synthesized, occurs in decay chain of ²⁷⁷Cn
^ Not directly synthesized, occurs in decay chain of ²⁸⁵Fl
^ Not directly synthesized, occurs in decay chain of ²⁸⁷Fl
^ Not directly synthesized, occurs in decay chain of ²⁸⁹Fl

Notes

Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.
# = Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses, ( )

Hs new[edit]

Nuclide^[2] ^{[n 1]}	Z	N	Isotopic mass (Da)^[1] ^{[n 2]}	Half-life	Decay mode ^{[n 3]}	Daughter isotope	Spin and parity ^{[n 4]}
Nuclide^[2] ^{[n 1]}	Excitation energy			Half-life	Decay mode ^{[n 3]}	Daughter isotope	Spin and parity ^{[n 4]}
²⁶³Hs	108	155	263.12856(37)#	760(40) µs	α	²⁵⁹Sg	7/2+#
²⁶⁴Hs	108	156	264.12836(3)	540(300) µs	α (50%)	²⁶⁰Sg	0+
²⁶⁴Hs	108	156	264.12836(3)	540(300) µs	SF (50%)	(various)	0+
²⁶⁵Hs	108	157	265.129793(26)	1.96(0.16) ms	α	²⁶¹Sg	9/2+#
^265mHs	300(70) keV			360(150) µs	α	²⁶¹Sg	3/2+#
²⁶⁶Hs^{[n 5]}	108	158	266.13005(4)	3.02(0.54) ms	α (68%)	²⁶²Sg	0+
²⁶⁶Hs^{[n 5]}	108	158	266.13005(4)	3.02(0.54) ms	SF (32%)^[9]	(various)	0+
^266mHs	1100(70) keV			280(220) ms	α	²⁶²Sg	9-#
²⁶⁷Hs	108	159	267.13167(10)#	55(11) ms	α	²⁶³Sg	5/2+#
^267mHs^{[n 6]}	39(24) keV			990(90) µs	α	²⁶³Sg
²⁶⁸Hs	108	160	268.13187(30)#	1.42(1.13) s	α	²⁶⁴Sg	0+
²⁶⁹Hs^{[n 7]}	108	161	269.13375(13)#	16 s	α	²⁶⁵Sg	9/2+#
²⁷⁰Hs	108	162	270.13429(27)#	10 s	α	²⁶⁶Sg	0+
²⁷¹Hs	108	163	271.13717(32)#	~4 s	α	²⁶⁷Sg
²⁷³Hs^{[n 8]}	108	165	273.14168(40)#	510 ms^[8]	α	²⁶⁹Sg	3/2+#
²⁷⁵Hs^{[n 9]}	108	167	275.14667(63)#	290(150) ms	α	²⁷¹Sg
²⁷⁷Hs^{[n 10]}	108	169	277.15190(58)#	11(9) ms	SF	(various)	3/2+#
This table header & footer: view

^ ^mHs – Excited nuclear isomer.
^ # – 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:

SF: Spontaneous fission
^ # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
^ Not directly synthesized, occurs as decay product of ²⁷⁰Ds
^ Existence of this isomer is unconfirmed
^ Not directly synthesized, occurs in decay chain of ²⁷⁷Cn
^ Not directly synthesized, occurs in decay chain of ²⁸⁵Fl
^ Not directly synthesized, occurs in decay chain of ²⁸⁷Fl
^ Not directly synthesized, occurs in decay chain of ²⁸⁹Fl

References[edit]

^ ^a ^b ^c ^d 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. Cite error: The named reference "AME2016 II" was defined multiple times with different content (see the help page).
^ ^a ^b ^c ^d 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. Cite error: The named reference "NUBASE2016" was defined multiple times with different content (see the help page).
^ 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. doi:10.1088/1674-1137/41/3/030003.
^ 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. doi:10.1088/1674-1137/41/3/030001.
^ "Universal Nuclide Chart". nucleonica.
^ ^a ^b Trenn, Thaddeus J. (1978). "Thoruranium (U-236) as the extinct natural parent of thorium: The premature falsification of an essentially correct theory". Annals of Science. 35 (6): 581–97. doi:10.1080/00033797800200441.
^ Dieter Ackermann (September 8, 2011). "²⁷⁰Ds and Its Decay Products – Decay Properties and Experimental Masses" (PDF). The 4th International conference on the Chemistry and Physics of Transactinide Elements, 5–11 September, Sochi, Russia. {{cite journal}}: Cite journal requires |journal= (help)
^ ^a ^b Utyonkov, V. K.; Brewer, N. T.; Oganessian, Yu. Ts.; Rykaczewski, K. P.; Abdullin, F. Sh.; Dimitriev, S. N.; Grzywacz, R. K.; Itkis, M. G.; Miernik, K.; Polyakov, A. N.; Roberto, J. B.; Sagaidak, R. N.; Shirokovsky, I. V.; Shumeiko, M. V.; Tsyganov, Yu. S.; Voinov, A. A.; Subbotin, V. G.; Sukhov, A. M.; Karpov, A. V.; Popeko, A. G.; Sabel'nikov, A. V.; Svirikhin, A. I.; Vostokin, G. K.; Hamilton, J. H.; Kovrinzhykh, N. D.; Schlattauer, L.; Stoyer, M. A.; Gan, Z.; Huang, W. X.; Ma, L. (30 January 2018). "Neutron-deficient superheavy nuclei obtained in the ²⁴⁰Pu+⁴⁸Ca reaction". Physical Review C. 97 (14320): 1–10. Bibcode:2018PhRvC..97a4320U. doi:10.1103/PhysRevC.97.014320.
^ Dieter Ackermann (September 8, 2011). "²⁷⁰Ds and Its Decay Products – Decay Properties and Experimental Masses" (PDF). The 4th International conference on the Chemistry and Physics of Transactinide Elements, 5–11 September, Sochi, Russia. {{cite journal}}: Cite journal requires |journal= (help)

[3] Bold for stable isotopes.

[4] Refers to that in water.

[5] Unless proton decay occurs.

[6] This and ³He are the only stable nuclides with more protons than neutrons.

[7] Produced during Big Bang nucleosynthesis.

[8] Tank hydrogen has a ²
H
abundance as low as 3.2×10⁻⁵ (mole fraction).

[9] Produced during Big Bang nucleosynthesis, but not primordial, as all such atoms have since decayed to ³He.

[10] Cosmogenic

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

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

[13] Unless proton decay occurs.

[14] This and ³He are the only stable nuclides with more protons than neutrons.

[15] Produced during Big Bang nucleosynthesis.

[16] Tank hydrogen has a ²
H
abundance as low as 3.2×10⁻⁵ (mole fraction).

[17] Produced during Big Bang nucleosynthesis, but not primordial, as all such atoms have since decayed to ³He.

[18] Cosmogenic

[19] Abbreviations:
EC: Electron capture
IT: Isomeric transition

[20] Bold for stable isotopes, bold italics for nearly-stable isotopes (half-life longer than the age of the universe)

[21] Long-lived fission product

[22] Used in medicine

[23] Tc – Excited nuclear isomer.

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

[25] Modes of decay:

EC: Electron capture

IT: Isomeric transition

n: Neutron emission

p: Proton emission

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

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

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

[TNN-29] # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

[30] Long-lived fission product

[31] Used in medicine

[35] Abbreviations:
CD: Cluster decay
EC: Electron capture
IT: Isomeric transition
SF: Spontaneous fission

[36] Bold for stable isotopes, bold italics for nearly-stable isotopes (half-life longer than the age of the universe)

[pn-37] Primordial radionuclide

[ul-38] Used in Uranium–lead dating

[39] Important in nuclear reactors

[uu-41] Used in uranium–uranium dating

[42] U – Excited nuclear isomer.

[43] Modes of decay:

CD: Cluster decay

EC: Electron capture

IT: Isomeric transition

SF: Spontaneous fission

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

[pn-45] Primordial radionuclide

[ul-46] Used in Uranium–lead dating

[47] Important in nuclear reactors

[uu-48] Used in uranium–uranium dating

[49] Not directly synthesized, occurs as decay product of ²⁷⁰Ds

[ui-51] Existence of this isomer is unconfirmed

[52] Not directly synthesized, occurs in decay chain of ²⁷⁷Cn

[53] Not directly synthesized, occurs in decay chain of ²⁸⁵Fl

[55] Not directly synthesized, occurs in decay chain of ²⁸⁷Fl

[q-56] Not directly synthesized, occurs in decay chain of ²⁸⁹Fl

[57] Hs – Excited nuclear isomer.

[TMS-58] # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).

[59] Modes of decay:

SF: Spontaneous fission

[TNN-60] # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).

[61] Not directly synthesized, occurs as decay product of ²⁷⁰Ds

[ui-63] Existence of this isomer is unconfirmed

[64] Not directly synthesized, occurs in decay chain of ²⁷⁷Cn

[65] Not directly synthesized, occurs in decay chain of ²⁸⁵Fl

[66] Not directly synthesized, occurs in decay chain of ²⁸⁷Fl

[q-67] Not directly synthesized, occurs in decay chain of ²⁸⁹Fl

[AME2016_II-1] 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. Cite error: The named reference "AME2016 II" was defined multiple times with different content (see the help page).

[NUBASE2016-2] 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. Cite error: The named reference "NUBASE2016" was defined multiple times with different content (see the help page).

[32] 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. doi:10.1088/1674-1137/41/3/030003.

[33] 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. doi:10.1088/1674-1137/41/3/030001.

[34] "Universal Nuclide Chart". nucleonica.

[thoruranium-40] Trenn, Thaddeus J. (1978). "Thoruranium (U-236) as the extinct natural parent of thorium: The premature falsification of an essentially correct theory". Annals of Science. 35 (6): 581–97. doi:10.1080/00033797800200441.

[50] Dieter Ackermann (September 8, 2011). "²⁷⁰Ds and Its Decay Products – Decay Properties and Experimental Masses" (PDF). The 4th International conference on the Chemistry and Physics of Transactinide Elements, 5–11 September, Sochi, Russia. {{cite journal}}: Cite journal requires |journal= (help)

[PuCa2017-54] Utyonkov, V. K.; Brewer, N. T.; Oganessian, Yu. Ts.; Rykaczewski, K. P.; Abdullin, F. Sh.; Dimitriev, S. N.; Grzywacz, R. K.; Itkis, M. G.; Miernik, K.; Polyakov, A. N.; Roberto, J. B.; Sagaidak, R. N.; Shirokovsky, I. V.; Shumeiko, M. V.; Tsyganov, Yu. S.; Voinov, A. A.; Subbotin, V. G.; Sukhov, A. M.; Karpov, A. V.; Popeko, A. G.; Sabel'nikov, A. V.; Svirikhin, A. I.; Vostokin, G. K.; Hamilton, J. H.; Kovrinzhykh, N. D.; Schlattauer, L.; Stoyer, M. A.; Gan, Z.; Huang, W. X.; Ma, L. (30 January 2018). "Neutron-deficient superheavy nuclei obtained in the ²⁴⁰Pu+⁴⁸Ca reaction". Physical Review C. 97 (14320): 1–10. Bibcode:2018PhRvC..97a4320U. doi:10.1103/PhysRevC.97.014320.

[62] Dieter Ackermann (September 8, 2011). "²⁷⁰Ds and Its Decay Products – Decay Properties and Experimental Masses" (PDF). The 4th International conference on the Chemistry and Physics of Transactinide Elements, 5–11 September, Sochi, Russia. {{cite journal}}: Cite journal requires |journal= (help)

[1]

[2]

[n 1]

[n 2]

[n 3]

[n 4]

[n 5]

[n 6]

[n 7]

[n 8]

[n 1]

[n 2]

[n 3]

[n 4]

[n 5]

[n 6]

[n 7]

[n 8]

[n 1]

[n 2]

[n 3]

[n 4]

[n 1]

[n 2]

[n 3]

[n 4]

[n 5]

[n 6]

[n 7]

[n 8]

[n 9]

[3]

[4]

[5]

[n 1]

[n 2]

[n 3]

[n 4]

[n 5]

[6]

[n 6]

[n 1]

[n 2]

[n 3]

[n 4]

[n 5]

[n 6]

[n 7]

[n 1]

[7]

[n 2]

[n 3]

[n 4]

[8]

[n 5]

[n 6]

[n 1]

[n 2]

[n 3]

[n 4]

[n 5]

[9]

[n 6]

[n 7]

[n 8]

[n 9]

[n 10]