Natural tantalum (73Ta) consists of two isotopes: observationally stable 181Ta (99.988%) and 180mTa (0.012%).

There are also 35 known artificial radioisotopes, the longest-lived of which are 179Ta with a half-life of 1.82 years, 182Ta with a half-life of 114.74 days, 183Ta with a half-life of 5.1 days, and 177Ta with a half-life of 56.46 hours. All other isotopes have half-lives under a day, most under an hour. There are also numerous isomers, the most stable of which (other than 180mTa) is 182m2Ta with a half-life of 15.8 minutes. All isotopes and nuclear isomers of tantalum are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.

Tantalum has been proposed as a "salting" material for nuclear weapons (cobalt is another, better-known salting material). A jacket of tantalum, irradiated by the intense high-energy neutron flux of the weapon, would be transmuted into the radioactive isotope 182Ta, producing about 1.12MeV of gamma radiation per decay and significantly increasing the radioactivity of the weapon's fallout for months. Such a weapon is not known to have ever been built, tested, or used.

List of isotopes

NuclideZNIsotopic mass (Da)Discovery yearHalf-lifeDecay modeDaughter isotopeSpin and parityNatural abundance (molefraction)
Excitation energyNormal proportionRange of variation
154Ta7381
155Ta7382154.97425(32)#3.2(13)msp154Hf11/2−
156Ta7383155.97209(32)#106(4)msp (71%)155Hf(2−)
β+ (29%)156Hf
156mTa94(8)keV360(40)msβ+ (95.8%)156Hf(9+)
p (4.2%)155Hf
157Ta7384156.96823(16)10.1(4)msα (96.6%)153Lu1/2+
p (3.4%)156Hf
157m1Ta22(5)keV4.3(1)msα153Lu11/2−
157m2Ta1593(9)keV1.7(1)msα153Lu25/2−#
158Ta7385157.96659(22)#49(4)msα154Lu(2)−
158m1Ta141(11)keV36.0(8)msα (95%)154Lu(9)+
158m2Ta2808(16)keV6.1(1)μsIT (98.6%)158Ta(19−)
α (1.4%)154Lu
159Ta7386158.963028(21)1.04(9)sβ+ (66%)159Hf1/2+
α (34%)155Lu
159mTa64(5)keV560(60)msα (55%)155Lu11/2−
β+ (45%)159Hf
160Ta7387159.961542(58)1.70(20)sα156Lu(2)−
160mTa110(250)keV1.55(4)sα156Lu(9,10)+
161Ta7388160.958369(26)3#s(1/2+)
161mTa61(23)keV(2005)3.08(11)sβ+ (93%)161Hf(11/2−)
α (7%)157Lu
162Ta7389161.957293(68)3.57(12)sβ+ (99.93%)162Hf3−#
α (0.074%)158Lu
162mTa120(50)#keV(1974)5#s7+#
163Ta7390162.954337(41)10.6(18)sβ+ (99.8%)163Hf1/2+
163mTa138(18)#keV(1992)10#s9/2−
164Ta7391163.953534(30)14.2(3)sβ+164Hf(3+)
165Ta7392164.950780(15)31.0(15)sβ+165Hf(1/2+,3/2+)
165mTa24(18)keV(1992)30#s(9/2−)
166Ta7393165.950512(30)34.4(5)sβ+166Hf(2)+
167Ta7394166.948093(30)1.33(7)minβ+167Hf(3/2+)
168Ta7395167.948047(30)2.0(1)minβ+168Hf(3+)
169Ta7396168.946011(30)4.9(4)minβ+169Hf(5/2+)
170Ta7397169.946175(30)6.76(6)minβ+170Hf(3+)
171Ta7398170.944476(30)23.3(3)minβ+171Hf(5/2+)
172Ta7399171.944895(30)36.8(3)minβ+172Hf(3+)
173Ta73100172.943750(30)3.14(13)hβ+173Hf5/2−
173m1Ta173.10(21)keV205.2(56)nsIT173Ta9/2−
173m2Ta1717.2(4)keV132(3)nsIT173Ta21/2−
174Ta73101173.944454(30)1.14(8)hβ+174Hf3+
175Ta73102174.943737(30)10.5(2)hβ+175Hf7/2+
175m1Ta131.41(17)keV222(8)nsIT175Ta9/2−
175m2Ta339.2(13)keV(1969)170(20)nsIT175Ta(1/2+)
175m3Ta1567.6(3)keV1.95(15)μsIT175Ta21/2−
176Ta73103175.944857(33)8.09(5)hβ+176Hf(1)−
176m1Ta103.0(10)keV1.08(7)msIT176Ta7+
176m2Ta1474.0(14)keV3.8(4)μsIT176Ta14−
176m3Ta2874.0(14)keV0.97(7)msIT176Ta20−
177Ta73104176.9444819(36)56.36(13)hβ+177Hf7/2+
177m1Ta73.16(7)keV410(7)nsIT177Ta9/2−
177m2Ta186.16(6)keV3.62(10)μsIT177Ta5/2−
177m3Ta1354.8(3)keV5.30(11)μsIT177Ta21/2−
177m4Ta4656.3(8)keV133(4)μsIT177Ta49/2−
178Ta73105177.945680(56)#2.36(8)hβ+178Hf7−
178m1Ta100(50)#keV9.31(3)minβ+178Hf(1+)
178m2Ta1467.82(16)keV59(3)msIT178Ta15−
178m3Ta2901.9(7)keV290(12)msIT178Ta21−
179Ta73106178.9459391(16)1.82(3)yEC179Hf7/2+
179m1Ta30.7(1)keV1.42(8)μsIT179Ta9/2−
179m2Ta520.23(18)keV280(80)nsIT179Ta1/2+
179m3Ta1252.60(23)keV322(16)nsIT179Ta21/2−
179m4Ta1317.2(4)keV9.0(2)msIT179Ta25/2+
179m5Ta1328.0(4)keV1.6(4)μsIT179Ta23/2−
179m6Ta2639.3(5)keV54.1(17)msIT179Ta37/2+
180Ta73107179.9474676(22)8.154(6)hEC (85%)180Hf1+
β− (15%)180W
180m1Ta75.3(14)keVObservationally stable9−1.201(32)×10−4
180m2Ta1452.39(22)keV31.2(14)μsIT15−
180m3Ta3678.9(10)keV2.0(5)μsIT(22−)
180m4Ta4172.2(16)keV17(5)μsIT(24+)
181Ta73108180.9479985(17)Observationally stable7/2+0.9998799(32)
181m1Ta6.237(20)keV6.05(12)μsIT181Ta9/2−
181m2Ta615.19(3)keV18(1)μsIT181Ta1/2+
181m3Ta1428(14)keV140(36)nsIT181Ta19/2+#
181m4Ta1483.43(21)keV25.2(18)μsIT181Ta21/2−
181m5Ta2227.9(9)keV210(20)μsIT181Ta29/2−
182Ta73109181.9501546(17)114.74(12)dβ−182W3−
182m1Ta16.273(4)keV283(3)msIT182Ta5+
182m2Ta519.577(16)keV15.84(10)minIT182Ta10−
183Ta73110182.9513754(17)5.1(1)dβ−183W7/2+
183m1Ta73.164(14)keV106(10)nsIT183Ta9/2−
183m2Ta470(10)#keV42(5)μsIT183Ta(1/2+)
183m3Ta1335(14)keV0.9(3)μsIT183Ta(19/2+)
184Ta73111183.954010(28)8.7(1)hβ−184W(5−)
185Ta73112184.955561(15)49.4(15)minβ−185W(7/2+)
185m1Ta406(1)keV0.9(3)μsIT185Ta(3/2+)
185m2Ta1273.4(4)keV11.8(14)msIT185Ta21/2−
186Ta73113185.958553(64)10.5(3)minβ−186W3#
186m1Ta336(20)keV1.54(5)min9+#
186m2Ta347.9(3)keV17(2)s7+#
187Ta73114186.960391(60)2.3(6)minβ−187W(7/2+)
187m1Ta1778(1)keV7.3(9)sIT187Ta(25/2−)
187m2Ta2933(14)keV136(24)sβ−187mW41/2+# [≥35/2]
IT187m1Ta
188Ta73115187.96360(22)#19.6(20)sβ−188W(1−)
188m1Ta99(33)keV19.6(20)s(7−)
188m2Ta391(33)keV3.6(4)μsIT188Ta10+#
189Ta73116188.96569(22)#20#s [>300ns]β−189W7/2+#
189mTa1309keV1.20(7)μsIT189Ta(19/2+)
189m2Ta1444keV160(20)nsIT189Ta(21/2−)
190Ta73117189.96917(22)#5.3(7)sβ−190W(3)
191Ta73118190.97153(32)#460#ms [>300ns]7/2+#
192Ta73119191.97520(43)#2.2(7)sβ−192W(2)
193Ta73120192.97766(43)#220#ms [>300ns]7/2+#
194Ta73121193.98161(54)#2#s [>300ns]
195Ta73122
196Ta73123
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Tantalum-180m

The nuclide 180mTa (m denotes a metastable state) is one of a very few nuclear isomers which are more stable than their ground states. Although it is not unique in this regard (this property is shared by bismuth-210m (210mBi) and americium-242m (242mAm), among other nuclides), it is exceptional in that it is observationally stable: no decay has ever been observed. In contrast, the ground state nuclide 180Ta has a half-life of only 8 hours.

180mTa has sufficient energy to decay in three ways: isomeric transition to the ground state of 180Ta, beta decay to 180W, or electron capture to 180Hf. However, no radioactivity from any of these theoretically possible decay modes has ever been observed. As of 2023, the half-life of 180mTa is calculated from experimental observation to be at least 2.9×1017 (290 quadrillion) years. The very slow decay of 180mTa is attributed to its high spin (9 units) and the low spin of lower-lying states. Gamma or beta decay would require many units of angular momentum to be removed in a single step, so that the process would be very slow. Similar suppression of gamma or beta decay occurs for 210mBi, a rather short-lived alpha emitter.

Because of this stability, 180mTa is a primordial nuclide, the only naturally occurring nuclear isomer (excluding short-lived radiogenic and cosmogenic nuclides). It presents one of two apparent violations of the Mattauch isobar rule, the other involving tellurium-123. It is also the rarest primordial nuclide in the Universe observed for any element which has any stable isotopes. In an s-process stellar environment with a thermal energy kBT = 26keV (i.e. a temperature of 300 million kelvin), the nuclear isomers are expected to be fully thermalized, meaning that 180Ta is equilibrated between spin states and its overall half-life is predicted to be 11 hours.

It is one of only five stable nuclides to have both an odd number of protons and an odd number of neutrons, the other four stable odd-odd nuclides being 2H, 6Li, 10B and 14N.

See also

Daughter products other than tantalum