The toluene radical ion
C6H5CH3
•+,
generated by resonance two-photon ionization, does not react with
a
single isobutene molecule (i-C4H8)
which has a significantly higher ionization potential (ΔIP = 0.42
eV). However,
a reaction is observed involving two
i-C4H8 molecules, to form the dimer
ion C8H16
•+. A
coupled reaction of dimer
formation and charge transfer to the dimer is exothermic if the product
is an ionized hexene with a low IP.
Correspondingly, the observed nominal second-order rate
coefficients, (5−25) × 10-12
cm3 s-1, are enhanced by
a
factor of >105 over the expected value for
direct endothermic charge transfer. Pressure and concentration
effects
suggest a sequential mechanism that proceeds through a
C6H5CH3
•+(i-C4H8)
reactive π complex. The complex can
isomerize to a nonreactive
CH3C6H4-t-C4H9
•+
adduct, or react with a second
i-C4H8 molecule to form a
C6H5CH3
•+(i-C4H8)2 complex, in
which the olefin molecules are activated by the aromatic ion.
Similar reactions are observed
in the benzene/propene system with a somewhat larger ΔIP of 0.48 eV,
suggesting that the charge density on the
olefin in the complex is still sufficient to activate it for
nucleophilic attack. However, aromatic/olefin systems
with
ΔIP > 0.87 eV show no olefin dimer formation. At low
[i-C4H8] and [Ar] number
densities, the rate of formation
of C8H16
•+ is
proportional to
[i-C4H8]2[Ar].
The corresponding fourth-order rate coefficient shows a strong
negative
temperature coefficient with k = 11 ×
10-42 cm9
s-1 at 300 K and 2 ×
10-42 cm9
s-1 at 346 K, suggesting that
the
mechanism can be efficient in low-temperature industrial and
interstellar environments. The direct formation of
the
dimer bypasses the monomer olefin cation and its consequent
side-reactions, and directs the products selectively
into radical ion polymerization. The products and energy
relationships that apply in the gas phase are observed
also
in clusters.