N. Ruckhaberle et al., FREE-ELECTRON ATTACHMENT AND RYDBERG ELECTRON-TRANSFER TO NF3 MOLECULES AND CLUSTERS, The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory, 101(51), 1997, pp. 9942-9947
Free electron attachment in the energy range 0-10 eV and Rydberg elect
ron transfer RET) to NF3 molecules, NF3 clusters, and NF3/Ar clusters
are studied by means of negative ion mass spectrometry. The experiment
al results are compared with density functional theory (DFT) calculati
ons. In the free electron experiment gasphase NF3 generates the dissoc
iative attachment (DA) products F-, F-2(-), and NF2- appearing from a
broad resonance around 2 eV, in agreement with an earlier beam experim
ent. The most abundant fragment, F-, exhibits a small ''threshold'' si
gnal at incident energies close to 0 eV. This signal increases with th
e target gas temperature and is due to transitions from the neutral to
the anion involving vibrationally excited states close to the interse
ction between the two potential energy surfaces. From the temperature
dependence of this threshold signal the activation energy for the exot
hermic DA reaction e(-) + NF3 --> F- + NF2 is derived as E-a = 0.1 +/-
0.05 eV. Time-of-flight (TOF) analysis reveals that F- arises from a
repulsive electronic state releasing the fragments with appreciable ki
netic energy. Free electron attachment and RET to NF3 clusters produce
undissociated cluster ions (NF3)(n-) including the monomer. In the ca
se of free electrons they are still dominantly formed via the 2 eV res
onance followed by intracluster relaxation processes. DFT calculations
predict a lowering of the symmetry from C-3v to C-s on going from the
neutral to the anion with one F atom substantially enlarged from the
NF2 plane. The calculated (adiabatic) electron affinities are EA(NF3)
= 1.71 eV and EA(NF2) = 1.18 eV. From the appearance energy in the DA
experiment we derive EA(NF2) = 1.1 +/- 0.1 eV.