TY - JOUR
T1 - Fine-structure dependence of the Ar ∗ ( 3P 0,2) + N 2(X) excitation transfer process
AU - Vredenbregt, E.J.D.
AU - Rooijakkers, W.J.M.
AU - van Gerwen, R.J.F.
AU - van den Hurk, P.J.
AU - Beijerinck, H.C.W.
PY - 1997/3/1
Y1 - 1997/3/1
N2 - Using diode lasers for the preparation of state selected beams of
metastable Ar ∗( 3P 0,
3P 2) atoms, the total cross section for the
formation of the N 2(C, v') final state has been measured for
v' = 0, 1, 2, and 3, respectively, in a wide range of collision energies
80 <E (meV) <2000. The energy dependence is very similar for
both initial fine structure states and all final vibrational states. The
experimental results are described in terms of a coupling of the initial
and final state by the intermediate Ar + + N
2- ionic potential, using a Landau Zener model to
calculate the transition probability. Due to the similarity in shape,
all cross sections are described by a single set of crossing parameters.
The observed threshold energy is Ex,i = 63 meV for both fine
structure states: the contribution of the 3P 0
state does not solve the discrepancy with earlier measurements of other
groups. The initial state rotation of the N 2 molecules has
no influence on the shape of the cross section, as investigated by
varying the rotational temperature of the supersonic target beam.
AB - Using diode lasers for the preparation of state selected beams of
metastable Ar ∗( 3P 0,
3P 2) atoms, the total cross section for the
formation of the N 2(C, v') final state has been measured for
v' = 0, 1, 2, and 3, respectively, in a wide range of collision energies
80 <E (meV) <2000. The energy dependence is very similar for
both initial fine structure states and all final vibrational states. The
experimental results are described in terms of a coupling of the initial
and final state by the intermediate Ar + + N
2- ionic potential, using a Landau Zener model to
calculate the transition probability. Due to the similarity in shape,
all cross sections are described by a single set of crossing parameters.
The observed threshold energy is Ex,i = 63 meV for both fine
structure states: the contribution of the 3P 0
state does not solve the discrepancy with earlier measurements of other
groups. The initial state rotation of the N 2 molecules has
no influence on the shape of the cross section, as investigated by
varying the rotational temperature of the supersonic target beam.
U2 - 10.1016/S0301-0104(97)00006-2
DO - 10.1016/S0301-0104(97)00006-2
M3 - Article
SN - 0301-0104
VL - 216
SP - 259
EP - 272
JO - Chemical Physics
JF - Chemical Physics
IS - 1
ER -