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Aca - Departamento de Física - Universidad Técnica Federico Santa ...

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V Encuentro Sud Americano <strong>de</strong> Colisiones Inelásticas en la Materia<br />

Ab-Initio Sturmian method for three-body quantum mechanical problems:<br />

Atomic and molecular bound states<br />

J. M. Randazzo 1 , 5 , A. L. Frapiccini 1 , 5 ,<br />

G. Gasaneo 2 , 5 , F. D. Colavecchia 1 , 5 , D. M. Mitnik 3 , 5 and L. U. Ancarani 4<br />

1 División <strong>de</strong> Colisiones Atómicas, Centro atómico Bariloche, San Carlos <strong>de</strong> Bariloche, Río Negro, Argentina.<br />

2 Depto. <strong>de</strong> <strong>Física</strong>, <strong>Universidad</strong> Nacional <strong>de</strong>l Sur, Bahía Blanca, Buenos Aires, Argentina<br />

3 Instituto <strong>de</strong> Astronomía y <strong>Física</strong> <strong>de</strong>l Espacio and <strong>Departamento</strong> <strong>de</strong> <strong>Física</strong>, Facultad <strong>de</strong> Ciencias Exactas y Naturales,<br />

<strong>Universidad</strong> <strong>de</strong> Buenos Aires C.C. 67, Suc. 28, (C1428EGA) Buenos Aires, Argentina.<br />

4 Laboratoire <strong>de</strong> Physique Moléculaire et <strong>de</strong>s Collisions,Université Paul Verlaine-Metz, 57078 Metz, France.<br />

5 Consejo Nacional <strong>de</strong> Investigaciones Científicas y <strong>Técnica</strong>s (CONICET).<br />

email address corresponding author: randazzo@cab.cnea.gov.ar<br />

In this work we review a recently introduced<br />

methodology to solve the<br />

Schrödinger equation of three particles. We<br />

assume that the particles interact through<br />

potentials <strong>de</strong>pending only on the distances<br />

between them. The most general Schrödinger<br />

equation we will consi<strong>de</strong>r reads:<br />

together with the boundary conditions:<br />

and<br />

Where U 1 , U 2 and U 12 can be any well behaved<br />

atomic potentials. We also assume that<br />

U 12 admits a simple partial wave expansion,<br />

such as Coulomb, Yukawa, armonic potentials,<br />

etc.<br />

Because of the symmetries of the Eq.<br />

(1), the wave function can be evaluated separately<br />

for each L, M, S and Π (total angular<br />

momentum, its projection along the z axis,<br />

the spin symmetry and parity, respectively).<br />

We then propose a partial wave expansion in<br />

terms of the bi-spherical harmonics, and obtain<br />

a coupled set of two-dimensional equations<br />

in the radial coordinates r 1 and r 2 .<br />

The set of coupled equations is solved<br />

by means of a Sturmian expansion (one<br />

Sturmian set for each coordinate)[1]. The<br />

Generalized Sturmian functions are solutions<br />

of the Sturm-Liouville equation:<br />

where V is a short range generating potential,<br />

β is the eigenvalue and E is consi<strong>de</strong>red<br />

as a parameter. Constructing the basis in this<br />

way enables us to set boundary conditions of<br />

the complete problem in each Sturmian <strong>de</strong>pending<br />

on coordinates r 1 and r 2 : Kato cusp<br />

conditions and Coulomb exponentially <strong>de</strong>caying<br />

behaviour for negative energies, or Coulomb<br />

outgoing wave conditions for positive<br />

ones[2].<br />

In this work we will show some results of the<br />

application of the Sturmian expansion to the<br />

solution of equation (1) for a variety of three<br />

body boun<strong>de</strong>d atomic and molecular systems<br />

and mo<strong>de</strong>ls. We choose here using negative<br />

energy Sturmian functions, and compute<br />

ground as well as the different manifolds of<br />

excited states. We also analyze different<br />

choices for the generating potential to<br />

achieve a high <strong>de</strong>gree of accuracy in the en-<br />

15 Valparaíso, Chile

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