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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