𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Ground states of atoms and molecules in strong magnetic fields

✍ Scribed by P. Schmelcher

Publisher
John Wiley and Sons
Year
1998
Tongue
English
Weight
298 KB
Volume
70
Category
Article
ISSN
0020-7608

No coin nor oath required. For personal study only.

✦ Synopsis

The ground states of small atoms and molecules, namely those of the hydrogen, helium, and lithium atoms and the hydrogen molecular ion and hydrogen molecule, are studied in the presence of an external magnetic field. For the one-electron systems the ground state is of the same symmetry for arbitrary field strengths, and the corresponding binding energy shows a monotonic increase with increasing field strength. More interesting, the two-and three-electron systems show ground-state transitions which involve both transitions in the spin multiplicity and spatial quantum numbers. An outlook on the expected cascade of transitions in many electron atoms and molecules is provided.

πŸ“œ SIMILAR VOLUMES

Molecules in strong magnetic fields: Som
Molecules in strong magnetic fields: Some perspectives and general aspects
✍ P. Schmelcher; L. S. Cederbaum πŸ“‚ Article πŸ“… 1997 πŸ› John Wiley and Sons 🌐 English βš– 189 KB πŸ‘ 1 views

In view of the coming availability of magnetic field strengths in the regime B f 100 T at the National High Magnetic Field Laboratory in Tallahassee, we present a brief overview of some relevant problems associated with molecular systems in strong magnetic fields. Both perspectives for future resear

Differential equations for ground-state
Differential equations for ground-state electron density and Slater sum in atoms and molecules with and without external fields
✍ N. H. March πŸ“‚ Article πŸ“… 1998 πŸ› John Wiley and Sons 🌐 English βš– 294 KB πŸ‘ 1 views

The ground-state density amplitude r for atoms and molecules Ž . satisfies a Schrodinger equation in which the customary one-body potential energy V r ¨Ž . of density functional theory is supplemented by the addition of the Pauli potential V r . p Since neither the exchange᎐correlation potential V o