The reac
tion of CF
2(a
3B
1) wi
th NO(X
2) was
theore
tically inves
tiga
ted using
the B3LYP, MP2, CCSD(T),G2M, CASSCF, and CASPT2 quan
tum chemical me
thods wi
th various basis se
ts including 6-31G(d), 6-311G(d), 6-311+G(3df), cc-pVDZ, and cc-pVTZ. In agreemen
t wi
th
the experimen
tal kine
tic da
ta,
the CF
2(a
3B
1)+ NO(X
2) reac
tion is found
to proceed via a fas
t, barrier-free combina
tion. This process, occurring on
thedouble
t po
ten
tial energy surface, leads
to
the elec
tronically exci
ted adduc
t F
2C-NO(2
2A' '), which readilyundergoes a surface hopping
to
the 1
2A' elec
tronic surface, wi
th a Landau-Zener
transi
tion probabili
tyes
tima
ted
to be close
to 90% per C-N vibra
tion. The me
tas
table adduc
t F
2C-NO(1
2A') can
then ei
therspon
taneously decompose in
to CF
2(X
1A
1) + NO(X
2) in a direc
t chemical quenching mechanism or relax
to i
ts ground-s
ta
te equilibrium s
truc
ture F
2CNO(X
2A'). The produc
t dis
tribu
tion resul
ting from
the la
tter,chemically ac
tiva
ted in
termedia
te was evalua
ted by solu
tion of
the mas
ter equa
tion (ME), under differen
treac
tion condi
tions, using
the exac
t s
tochas
tic simula
tion me
thod; microcanonical ra
te cons
tan
ts were compu
tedusing Rice-Ramsperger-Kassel-Marcus (RRKM)
theory, based on
the po
ten
tial energy surfaces (PESs)cons
truc
ted using bo
th G2M and CASPT2 me
thods. The RRKM/ME analysis reveals
tha
t the ho
t F
2CNO(X
2A') rapidly fragmen
ts almos
t exclusively
to
the same produc
ts as above, CF
2(X
1A
1) + NO(X
2), whichamoun
ts
to an indirec
t chemical quenching mechanism. The reac
tion on
the quar
te
t PES is unlikely
to besignifican
t excep
t a
t very high
tempera
tures. The high crossing probabili
ty (up
to 90%) be
tween
the
two"avoided" double
t PESs poin
ts ou
t the inheren
t difficul
ty in
trea
ting chemically ac
tiva
ted reac
tions wi
th fas
t-moving nuclei wi
thin
the Born-Oppenheimer approxima
tion.