1982
DOI: 10.1103/physreva.26.1283
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Angularly resolved rotationally inelastic scattering ofNa2-Ne: Comparison between experiment and theory

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Cited by 84 publications
(16 citation statements)
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“…Comparison with data on Na2~rare-gas collisions by Bergmann and co-workers [14] indicates that our DCS values peak at somewhat lower values than those shown in Ref. [14]. This is not surprising since the work cited on Na2 was performed on the ground state of that molecule and our results are for the Li2 A 1 !!…”
Section: The Final Velocity Component Distribution P V Xf (Vzf\v Z )supporting
confidence: 62%
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“…Comparison with data on Na2~rare-gas collisions by Bergmann and co-workers [14] indicates that our DCS values peak at somewhat lower values than those shown in Ref. [14]. This is not surprising since the work cited on Na2 was performed on the ground state of that molecule and our results are for the Li2 A 1 !!…”
Section: The Final Velocity Component Distribution P V Xf (Vzf\v Z )supporting
confidence: 62%
“…Comparison with data on Na2~rare-gas collisions by Bergmann and co-workers [14] indicates that our DCS values peak at somewhat lower values than those shown in Ref. [14].…”
Section: The Final Velocity Component Distribution P V Xf (Vzf\v Z )supporting
confidence: 46%
“…(For a review of current theoretical and experimental progress see Schinke and Bowman [1].) Most of the studies, however, employ the infinite order sudden (IOS) approximation [-4] in quantum I- [4][5][6][7], classical [-8-10] and semiclassical 1-10-11] mechanics. The most widely studied collisions are sudden, i.e.…”
Section: Introductionmentioning
confidence: 99%
“…The rotational rainbow phenomena are directly related to the anisotropy of the potential; they arise from an interference of classical trajectories (typically two) with the same scattering angle and angular momentum transfer, but different orientations of the molecule. In other words, the orientation angle 7 of the target molecule is frozen during the collision and the trajectory of the scattered atom is approximated by a trajectory in a spherically symmetric potential V(R, 7) with fixed parameter 7-The typical rotational rainbow structure of the j---~j' differential cross sections under sudden conditions can be considered as well understood for initially nonrotating (/=0) molecules with purely repulsive interactions: The classical cross sections show a rainbow (square root) singularity at the maximum allowed final rotational momentum at each scattering angle, which is quantum mechanically softened into a maximum accompanied by a series of maxima (supernumerary rainbows) on the classically allowed ('bright') side. characterized by short collision times, negligible energy transfer and steep repulsive potentials.…”
Section: Introductionmentioning
confidence: 99%
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