1979
DOI: 10.1063/1.438203
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Rotational compound state resonances for an argon and methane scattering system

Abstract: A broad compound state (closed channel) resonance in the argon–methane system is investigated using a realistic model potential, and approximations are developed which allow one to search for such resonances easily. Methane is treated as a rigid rotor and the energy of the resonance is such that there are only three rotational states with open channels. The coupled states approximation proved invaluable in characterizing the resonances. A perturbation technique was developed which allows one to predict accurat… Show more

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Cited by 90 publications
(36 citation statements)
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“…As one can see, the cross sections present several resonances (shape and Feshbach), particularly at low kinetic energies. This typical behavior for cross sections was pointed out by different studies (Smith et al 1979;Christoffel & Bowman 1983;Hammami et al 2008a,b,c;Nkem et al 2009). These resonances are precisely detected in our calculated cross sections.…”
Section: Cross Sectionssupporting
confidence: 63%
“…As one can see, the cross sections present several resonances (shape and Feshbach), particularly at low kinetic energies. This typical behavior for cross sections was pointed out by different studies (Smith et al 1979;Christoffel & Bowman 1983;Hammami et al 2008a,b,c;Nkem et al 2009). These resonances are precisely detected in our calculated cross sections.…”
Section: Cross Sectionssupporting
confidence: 63%
“…Noticeable resonances appear at low collisional energies. This is related to the presence of an attractive potential well, which allows for O 2 -H 2 bound and quasi-bound states to be formed before the complex dissociates (Smith et al 1979;Christoffel & Bowman 1983).…”
Section: Cross Sectionsmentioning
confidence: 99%
“…The quasibound states may arise from the tunneling from the centrifugal barrier and from excitation of N 2 to an asymptotically closed channel where N 2 becomes temporarily trapped in one of the bound states of the potential well. [21][22][23] Compared to the depth of the potential well, the energy spacing of the N 2 rotational structure is small, so that both types of quasibound states occur in the same energy range. The disappearance of the resonances as a function of the collision energy can be qualitatively understood by examining the radial functions V λ (R): the spherical term V 0 , which governs the elastic transitions, has a potential well of about 25.2 cm −1 positioned at R = 10.50 a.u., close to the equilibrium distance of the van der Waals complex.…”
Section: Cross Sectionsmentioning
confidence: 99%