Titlebook: Recent Trends in Theory of Physical Phenomena in High Magnetic Fields; Israel D. Vagner,Peter Wyder,Tsofar Maniv Book 2003 Springer Scienc

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Excitons in Single and Vertically Coupled Type II Quantum Dots in High Magnetic Fields, dot is modelled by a quantum disk with radius . and thickness . in which the electron is confined in the disk whereas the dot acts as an antidot for the hole. For disk-like dots, i.e. . ? 2., the hole is located above and below the disk, while for pillar-like systems, i.e. . ? 2., the hole is locat

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Spin Transport in Diluted Magnetic Semiconductor Superlattices,n. A II-VI compound with Mn substituted at the group II site exhibits large band electron spin splittings at moderately low magnetic fields. We elaborate on a theory of the influence of exchange coupling with Mn ion spins on electric field domain formation and on the sensitivity of this influence to

織物

Magnetic Impurities in a Strong Magnetic Field,ce impurity scattering. It is shown that this scattering results in an appearance of bound Landau states with zero angular moment between the Landau subbands. The resonance scattering is spin selective, and it results in a strong spin polarization of Landau states, as well as in a noticeable magneti

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On Deriving Relaxation Equations for Nuclear Spins,derivation holds within the adiabatic approximation for a general stationary non-equilibrium state of the environment and also for an arbitrary value of .. The system of coupled relaxation equations contains two independent characteristic times. The stationary solution of the equations is the correc

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NMR Revisited, to the progress of electronics during that period. And it happened that, thanks to the loose coupling of nuclear spins, both among themselves and with the surroundings, it has been possible to manipulate the spin systems in many tricky ways and thus obtain a lot of precise information about their s

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Chessboard Magnetoconductance of a Quantum Dot in the Kondo Regime,he magnetic field or the number of electrons in the QD is varied, the Kondo temperature shows large oscillations due to the successive appearance of ground states having alternately strong and weak correlation effects.