机构:HARVARD UNIV, DEPT PHYS, CAMBRIDGE, MA 02138 USA
Cote, R
Heller, EJ
论文数: 0引用数: 0
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机构:HARVARD UNIV, DEPT PHYS, CAMBRIDGE, MA 02138 USA
Heller, EJ
Dalgarno, A
论文数: 0引用数: 0
h-index: 0
机构:HARVARD UNIV, DEPT PHYS, CAMBRIDGE, MA 02138 USA
Dalgarno, A
机构:
[1] HARVARD UNIV, DEPT PHYS, CAMBRIDGE, MA 02138 USA
[2] HARVARD UNIV, DEPT ASTRON, CAMBRIDGE, MA 02138 USA
来源:
PHYSICAL REVIEW A
|
1996年
/
53卷
/
01期
关键词:
D O I:
10.1103/PhysRevA.53.234
中图分类号:
O43 [光学];
学科分类号:
070207 ;
0803 ;
摘要:
Very-low-energy collisions between two atoms are usually suppressed, in that the probability of close approach of the atoms becomes greatly reduced as the collision energy vanishes, even if the potential is completely attractive (with the exception of the Coulomb interaction). The suppression is a quantum effect, related to the Wigner threshold law. It is gauged by comparing the ratio of the probability of being inside the well to the probability of being outside for both the classical and quantum regimes. As the asymptotic kinetic energy vanishes, the approaching atoms reach a minimum distance of typically 20 or 30 a.u. Here we study attractive interaction potentials of the form -alpha/r(n), and give some numerical results for accurate X (1) Sigma(g)(+) and a (3) Sigma(u)(+) states of Li-2 and Na-2 molecules. We show that in some circumstances it is possible to use Wentzel-Kramers-Brillouin theory in the suppression regime (where it fails) and to correct for its failure with a simple factor.