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Issue 39, 2009
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Depolarisation of rotational orientation and alignment of OH (X2Π) in collisions with molecular partners: N2 and O2

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Abstract

The depolarisation of selected OH (X2Π3/2v = 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 N2 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 HOOO attractive minimum at shorter range clearly does not outweigh other factors that favour k(K)PS for N2.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.

Graphical abstract: Depolarisation of rotational orientation and alignment of OH (X2Π) in collisions with molecular partners: N2 and O2

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Publication details

The article was received on 06 May 2009, accepted on 06 Jul 2009 and first published on 31 Jul 2009


Article type: Paper
DOI: 10.1039/B909051G
Citation: Phys. Chem. Chem. Phys., 2009,11, 8813-8820
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    Depolarisation of rotational orientation and alignment of OH (X2Π) in collisions with molecular partners: N2 and O2

    G. Paterson, S. Marinakis, M. L. Costen and K. G. McKendrick, Phys. Chem. Chem. Phys., 2009, 11, 8813
    DOI: 10.1039/B909051G

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