Five different MnF* emitting
statesA7Π, e5Σ+,
d5Π, c5Σ+, and
b5Πhave been observed from collisions
between SF6 molecules and a pulsed, laser-ablated beam of
Mn atoms. The various excitation functions,
measured up to nominal collision energy
E
T
0 = 2000 kJ mol-1,
have been modeled by the multiple line-of-centers approach. The analysis indicates that
MnF*(A7Σ+) is predominantly formed on
a single potential
surface, with probable progenitor
Mn*(z8PJ); the
e5Σ+, d5Π, and
c5Σ+ states are formed via three
common
potential surfaces, with likely reagent state
Mn*(a6DJ), while the
a6D
J
state is also likely to be the
progenitor
of MnF*(b5Π). Partial depletion of the
b5Π state at high energy seems to be accompanied by
enhanced yield
of the other emitters. All reactions seem to be characterized by a
shift forward in transition state location
with increasing collision energy. The results suggest an electron
jump barrier at short internuclear distances,
forced outward at higher collision energies due to lack of time for the
SF6 to distort to the equilibrium geometry
of SF6
-.