Titlebook: Atoms in Strong Fields; Cleanthes A. Nicolaides,Charles W. Clark,Munir H. Book 1990 Springer Science+Business Media New York 1990 UV.Zeem

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Atoms in Static Electric and Magnetic Fields: The Experimental Aspectsics and numerous experimental studies were undertaken all around the world. These states called “Rydberg states” have few well established characteristics: they have a long life time and a very weak radiative transition probability connects them to the ground state, they are weakly bound, the bendi

Dawdle

Theory of the Zeeman Effect in Highly Excited Atoms5 tesla) magnetic fields. These developments began in the early seventies in attempts to understand spectra of the alkaline earths obtained in the pioneering measurements by Garton and Tomkins [1], but, (together with those in classical theory), have been greatly stimulated over the last few years b

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Hydrogen in Strong DC and Low Frequency Fieldsexternal fields of all varieties: electric, magnetic or radiation, applied individually or simultaneously.. The interest stems from the ability to produce, in the laboratory, fields which are comparable in strength to internal atomic fields. Although it is almost impossible to create dc fields in th

Debark

Elliptic Atomic Statesrbits with minimum quantum fluctuations. These states are uniquely defined from symmetry considerations and are stationary states of the Coulomb hamiltonian. They exhibit the best spatial localization it is possible to achieve within quantum-mechanical constraints, on a classical Kepler ellipse. Exp

Implicit

regale

Magneto-Optical Spectroscopy in Strong Fieldsng field problem. Several lecture courses in the present volume recount the remarkable progress achieved in recent years in the understanding of . for atoms in high magnetic fields. A noteworthy feature of such progress is that semi-classical approximations achieve most, if not all, of the understan

TATE

The Single Atom Maser, Chaos and Order of Ions in a Trap and Rydberg Atoms in Crossed Electric and Melds will be reviewed. In the latter experiment the electric dipole moment of the atoms in the external fields is determined. For this purpose the deflection of the atoms in an inhomogeneous electric field was investigated.