Titlebook: Atoms in Strong Magnetic Fields; Quantum Mechanical T Hanns Ruder,Günter Wunner,Florian Geyer Book 1994 Springer-Verlag Berlin Heidelberg 1

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Highly Excited States,rengths of white dwarfs or neutron stars, can be realized for highly excited states (.. > 30, e.g.) even in terrestrial laboratory field strengths of several Tesla. The discussion of the influence of strong laboratory magnetic fields on . of the hydrogen atom is the subject of this chapter.

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Die Tatkraft der vier Basisemotionen,(3.1) can be classified according to .-parity . and the .component .. of orbital angular momentum, which are exact symmetries of ., but in general no further separation of the two-dimensional problem is possible.

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Interacting Charged Particles in Uniform Magnetic Fields,tential . at the position .. of particle . is abbreviated by .. = ..). In this section no special gauge is adopted. The Hamiltonian of the system is given by . where the potential energy . of the interaction is assumed to be momentum independent and translationally invariant. Generally, the conserve

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Methods of Solution for the Magnetized Coulomb Problem,ltonian of an electron in a static Coulomb potential and in a uniform magnetic field then reads for spin-down states . where the magnetic field is assumed to point in the .-direction and .. = ..+... The energies of the corresponding spin-up states are obtained by simply adding .. The eigenstates of

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