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1.
J Chem Phys ; 141(17): 174305, 2014 Nov 07.
Artigo em Inglês | MEDLINE | ID: mdl-25381512

RESUMO

Using the recently developed explicitly correlated coupled cluster method in connection with the aug-cc-pVTZ basis set, we generated the three-dimensional potential energy surface (3D-PES) of the ground state of the Ar-BeO complex. This PES covers the regions of the global and local minima, the saddle point, and the dissociation of the complex. The PES is also used for the calculation of the rovibrational spectrum up to the dissociation limit. The high density of levels which is observed favors the mixing of the states and hence the occurrence of anharmonic resonances. The wavefunctions of the high rovibrational levels exhibit large amplitude motions in addition to strong anharmonic resonances. Our theoretical spectrum should be helpful in identifying the van der Waals modes of this complex in laboratory.

2.
Phys Chem Chem Phys ; 13(42): 19142-7, 2011 Nov 14.
Artigo em Inglês | MEDLINE | ID: mdl-21947359

RESUMO

In the present study we investigate the role played by the hyperfine structure of manganese in the cooling and magnetic trapping of MnH((7)Σ(+)). The effect of the hyperfine structure of Mn on the relaxation of the magnetically trappable maximally stretched low-field seeking state of MnH((7)Σ(+)) in collisions with (3)He is deduced from comparison between the results of the present approach and our previous nuclear spin free calculations. We show that our previous results are unchanged at the temperature of the buffer gas cooling experiment but find a new resonance at very low collision energy. The role played by the different contributions to the hyperfine diatomic Hamiltonian considered in this work as well as the effect of an applied magnetic field on this resonance are also analyzed.

3.
J Chem Phys ; 129(10): 104308, 2008 Sep 14.
Artigo em Inglês | MEDLINE | ID: mdl-19044914

RESUMO

The first quantum mechanical investigation of the rotational deactivation of HF induced by collisions with ortho- and para-H(2) molecules is reported. Ab initio potential energy calculations are carried out at the coupled cluster level with single and double excitations, using a quadruple-zeta basis set. The global rigid rotor four-dimensional potential energy surface is obtained by fitting ab initio points with a least squares procedure for the angular terms and interpolating the radial coefficients with cubic splines. It is shown that the equilibrium structure of the H(2)-HF complex is T-shaped and the well depth is found to be 359 cm(-1). Close coupling scattering calculations are performed at collision energy ranging from 10(-2) to 1600 cm(-1). A comparison of the rotational quenching of HF with para-H(2) and (4)He is used to validate our potential energy surface. The rotational quenching cross sections of HF by ortho- and para-H(2) are also compared and found to be very different. An explanation of these differences based on a resonance mechanism is proposed.

4.
Phys Chem Chem Phys ; 7(12): 2446-52, 2005 Jun 21.
Artigo em Inglês | MEDLINE | ID: mdl-15962028

RESUMO

In this paper we report the first theoretical study of the title reaction. A global, single-valued model of the ground-state potential energy surface has been obtained by fitting to an extensive set of high-level ab initio calculations. The surface is found to be attractive apart from linear geometries where energy barriers appear due to conical intersections. This model was then used to calculate the reactive reactant state selected cross sections for collision energies ranging from threshold up to 4000 cm(-1). These calculations were performed using our version of the Baer's approach of the RIOSA-NIP method which is based on the use of a negative imaginary potential. We find that the reaction probability is extremely oscillatory as a function of kinetic energy as it is a case for insertion reactions with a low exoergicity. The resulting reaction rate coefficient is found to first increase slowly as a function of temperature up to a broad maximum around 20 K and then to decrease slowly when temperature keeps increasing.

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