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The gas-phase reactivity of Ta(a 4 F 3/2 ) with O 2 , N 2 O, CO 2 and NO in the temperature range 296–548 K is reported. The room-temperature removal rate constants for the spin–orbit excited states (a 4 F J , J=5/2, 7/2, 9/2) are reported for these oxidants and CH 4 . Tantalum atoms were produced by the photodissociation of tetracarbonyl cyclopentadienyl tantalum(0) [Ta(C 5 H 5 )(CO) 4 ] and detected by laser-induced fluorescence. The reaction rate constants of the a 4 F 3/2 ground state with O 2 , N 2 O, CO 2 and NO are temperature dependent. The disappearance rates in the presence of all the reactants are independent of total pressure, indicating a bimolecular abstraction mechanism. The bimolecular rate constants are described in Arrhenius form by k(O 2 )=(1.7±0.2) ×10 -10 exp(-7.8±0.4 kJ mol -1 /RT) cm 3 s -1 , k(N 2 O)=(7.1±1.0)×10 -11 exp(-13.6±0.6 kJ mol -1 /RT) cm 3 s -1 , k(CO 2 )=(1.0±0.1)×10 -10 exp(-26.8±0.5 kJ mol -1 /RT) cm 3 s -1 and k(NO)=(1.0±0.2)×10 -10 exp(-1.6±0.8 kJ mol -1 /RT) cm 3 s -1 where the uncertainties are ±2σ. The removal rates of the spin–orbit excited states with O 2 , N 2 O, CO 2 and NO are spin–orbit state dependent and are generally faster than for the ground state. The a 4 F 3/2 ground state is unreactive with methane, although the spin–orbit excited states are quenched by methane. The a 4 F 5/2 , a 4 F 7/2 and a 4 F 9/2 states have second-order room-temperature removal rate constants in methane of 6.0×10 -13 , 9.5×10 -13 and 2.3×10 -11 cm 3 s -1 , respectively.
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Campbell et al. (1997) studied this question.
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