THE LIFETIMES OF GAS-PHASE CO2(CENTER-DOT-) AND N2O(CENTER-DOT-) CALCULATED FROM THE TRANSITION-PROBABILITY OF THE AUTODETACHMENT PROCESS A(-)-]A-)(E()
A. Rauk et al., THE LIFETIMES OF GAS-PHASE CO2(CENTER-DOT-) AND N2O(CENTER-DOT-) CALCULATED FROM THE TRANSITION-PROBABILITY OF THE AUTODETACHMENT PROCESS A(-)-]A-)(E(), International journal of chemical kinetics, 26(1), 1994, pp. 7-24
A procedure to calculate the quantum mechanical transition probability
of a unimolecular primary chemical process, A(-) -->, A + e(-) is inv
estigated for the circumstance where A(-) and A have different numbers
of vibrational and rotational degrees of freedom (one is linear, the
other not). A procedure is introduced to deal with the coupling betwee
n the vibrational and rotational motions. The proposed method was appl
ied to calculating the lifetimes of CO2.- and N2O.- in the gas phase.
The geometry optimizations and frequency calculations for CO2, CO2.-,
N2O, and N2O.- are performed at HF, MP2, and QCISD(T) levels with 6-31
G or 6-31+G* basis sets, in order to obtain reliable geometric and sp
ectroscopic information on these systems. Lifetimes are calculated for
several of the lower vibrational-rotational states of the anions, as
well as for the Boltzmann distribution of states at 298 K. The lifetim
e of the lowest vibrational-rotational state of CO2.-, is 1.03 x 10(-4
) s, and of the lowest vibrational state with rotational levels weight
ed by Boltzmann distribution at 298 K, 1.50 x 10(-4) s. These values a
re in good agreement with the experimental number, 9.0 +/- 2.0 x 10(-5
) s,and support the experimental evidence that CO2.- was formed in its
ground vibrational level by the techniques used. The lifetime of CO2.
- calculated with Boltzmann distribution over its vibrational and rota
tional levels at 298 K, is 1.51 x 10(-5) s. There are no direct measur
ements of the lifetime of N2O.-, but it was estimated to be greater th
an 10(-4) s from experimental evidence. The predicted lifetimes of N2O
.-, at its lowest vibrational-rotational state (0 K) and lowest vibrat
ional state with rotational levels weighted by the Boltzmann distribut
ion at 298 K, are 238 and 19.1 s, respectively. The lifetime of N2O.-
at thermal equilibrium at 298 K is 6.66 x 10(-2) s, indicating that el
ectron loss from the excited vibrational states of N2O.- is significan
t. This study represents the first theoretical investigation of CO2.-
and N2O.- lifetimes. (C) 1994 John Wiley & Sons, Inc.