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Resonance condition zero-field interactions

In general, no simple, consistent set of analytical expressions for the resonance condition of all intradoublet transitions and all possible rhombicities can be derived with the perturbation theory for these systems. Therefore, the rather different approach is taken to numerically compute all effective g-values using quantum mechanics and matrix diagonalization techniques (Chapters 7-9) and to tabulate the results in the form of graphs of geff,s versus the rhombicity r = E/D. This is a useful approach because it turns out that if the zero-field interaction is sufficiently dominant over... [Pg.84]

Here 2tt Aft = trm is imposed to eliminate the effect by the zero-order interaction of the RF field, otherwise a term containing Ix will remain and it will distort the longitudinal magnetization, transverse magnetization, as well as the BSPS of the 13C . For the on-resonance condition, 5 = 0, all the higher-order average Hamiltonians vanish since [7f(/ ), = 0 for arbitrary l and... [Pg.39]

We have considered here the influence of dispersion asymmetry and Zee-man splitting on the Josephson current through a superconductor/quantum wire/superconductor junction. We showed that the violation of chiral symmetry in a quantum wire results in qualitatively new effects in a weak superconductivity. In particularly, the interplay of Zeeman and Rashba interactions induces a Josephson current through the hybrid ID structure even in the absence of any phase difference between the superconductors. At low temperatures (T critical Josephson current. For a transparent junction with small or moderate dispersion asymmetry (characterized by the dimensionless parameter Aa = (vif — v2f)/(vif + V2f)) it appears, as a function of the Zeeman splitting Az, abruptly at Az hvp/L. In a low transparency (D Josephson current at special (resonance) conditions is of the order of yfD. In zero magnetic field the anomalous supercurrent disappears (as it should) since the spin-orbit interaction itself respects T-symmetry. However, the influence of the spin-orbit interaction on the critical Josephson current through a quasi-ID structure is still anomalous. Contrary to what holds... [Pg.225]


See other pages where Resonance condition zero-field interactions is mentioned: [Pg.82]    [Pg.147]    [Pg.152]    [Pg.122]    [Pg.165]    [Pg.360]    [Pg.655]    [Pg.103]    [Pg.514]    [Pg.183]    [Pg.145]    [Pg.135]    [Pg.542]    [Pg.161]    [Pg.234]    [Pg.89]    [Pg.642]    [Pg.89]    [Pg.372]    [Pg.162]    [Pg.73]    [Pg.52]    [Pg.642]   
See also in sourсe #XX -- [ Pg.67 , Pg.82 , Pg.83 , Pg.84 , Pg.85 , Pg.86 ]




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Field condition

Field resonance

Interacting field

Interacting resonances

Interaction field

Resonance condition

Resonance interaction

Resonant interaction

Zero-field

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