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Coupled‐channel investigation of rotationally and vibrationally inelastic collisions between He and H 2
Author(s) -
Mcguire Paul,
Micha David A.
Publication year - 2009
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/qua.560060614
Subject(s) - excitation , atomic physics , angular momentum , rotational partition function , rotational transition , excited state , physics , chemistry , total angular momentum quantum number , rotational–vibrational spectroscopy , quantum mechanics
The coupled‐channel formalism has been employed for He + H 2 collisions including rotational ( j = 0, 2) and vibrational ( n = 0, 1) levels and making use of the Kraus‐Mies potential energy surface. Integral and differential cross sections are obtained at the total energies 0.3884, 0.9, and 1.4116 eV for rotational and vibrational transitions separately, and for the combined processes. Considerable use has been made of the microscopic reversibility principle to extract cross sections from the S matrix for de‐excitations as well as for excitations. Cross sections for vibrational excitation are found to decrease when accompanied by rotational excitation. For vibrational de‐excitation, the effect of rotational excitation is to increase the cross sections. Defining a most probable impact parameter b̄ max from the maximum in the partial integral cross sections, vibration excitation is found to occur at low b̄ max , while rotational excitation is observed at comparatively higher values. For simultaneous rotational and transitions, b̄ max decreases with increasing energy transfer. A deflection angle © (cl is defined in terms of the impact parameters and the turning point radii for the initial and final channels, and a correlation between this angle and the maxima in the computed angular distributions is found. The transition probabilities for the rotational excitation j = 0 → 2 with simultaneous vibrational excitation and their physical interpretation are also discussed within the total angular momentum coupling scheme.

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