TY - JOUR
T1 - Depolarisation of rotational orientation and alignment of OH (X 2Π) in collisions with molecular partners
T2 - N2 and O2
AU - Paterson, Grant
AU - Marinakis, Sarandis
AU - Costen, Matthew L.
AU - McKendrick, Kenneth G.
PY - 2009
Y1 - 2009
N2 - The depolarisation of selected OH (X2?3/2v = 0, J = 1.5 and 4.5, e) levels in collisions with the molecular partners N2 and O2 at room temperature (nominally 298 K) has been studied using the polarisation spectroscopy (PS) technique. We obtain total depolarisation rate constants, k(K)PS, which are the combination of population transfer out of the initial level and elastic depolarisation of the tensor moment of respective rank K = 1 (orientation) or K = 2 (alignment) of its angular momentum distribution. N2 causes more rapid decay of PS signals than O2. There are no clear dependences of k (K)PS on J for either partner. The K-dependence for N 2 mirrors that determined previously for the noble gases, but is less regular for O2, warranting further investigation. Comparison with independent line-broadening data suggests that there may be an additional, pure-elastic-dephasing contribution to collisional broadening for N2 that is not apparent for O2. The presence of an independently established deeper HO-OO attractive minimum at shorter range clearly does not outweigh other factors that favour k(K)PS for N 2.The most obvious explanation is stronger, longer-range attractive interactions due to the larger quadrupole moment of N2. However, this appears to be contradicted by the rigorous ab initio calculations currently available on OH-O2. © the Owner Societies 2009.
AB - The depolarisation of selected OH (X2?3/2v = 0, J = 1.5 and 4.5, e) levels in collisions with the molecular partners N2 and O2 at room temperature (nominally 298 K) has been studied using the polarisation spectroscopy (PS) technique. We obtain total depolarisation rate constants, k(K)PS, which are the combination of population transfer out of the initial level and elastic depolarisation of the tensor moment of respective rank K = 1 (orientation) or K = 2 (alignment) of its angular momentum distribution. N2 causes more rapid decay of PS signals than O2. There are no clear dependences of k (K)PS on J for either partner. The K-dependence for N 2 mirrors that determined previously for the noble gases, but is less regular for O2, warranting further investigation. Comparison with independent line-broadening data suggests that there may be an additional, pure-elastic-dephasing contribution to collisional broadening for N2 that is not apparent for O2. The presence of an independently established deeper HO-OO attractive minimum at shorter range clearly does not outweigh other factors that favour k(K)PS for N 2.The most obvious explanation is stronger, longer-range attractive interactions due to the larger quadrupole moment of N2. However, this appears to be contradicted by the rigorous ab initio calculations currently available on OH-O2. © the Owner Societies 2009.
UR - http://www.scopus.com/inward/record.url?scp=70349876651&partnerID=8YFLogxK
U2 - 10.1039/b909051g
DO - 10.1039/b909051g
M3 - Article
SN - 1463-9076
VL - 11
SP - 8813
EP - 8820
JO - Physical Chemistry Chemical Physics
JF - Physical Chemistry Chemical Physics
IS - 39
ER -