1997
DOI: 10.1088/0305-4470/30/15/020
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Lattice Green function in uniform magnetic fields

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Cited by 7 publications
(6 citation statements)
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“…As pointed out above, the effect of the magnetic field is contained in the local Green's function G ll , therefore, the strategy to solve the DMFT problem is to compute the eigenvalues of the non-interacting lattice in the presence of uniform magnetic field and use them in the selfconsistency loop. There are numerous methods to solve the non-interacting case 3,24,25 . For the numerical example presented below, we take the case of a uniform magnetic field perpendicular to a square lattice and we compute the energy level of Bloch electrons by solving an almost Mathieu equation named Harper equation 26 for rational ratios of magnetic flux, i.e.…”
Section: Methods and Modelmentioning
confidence: 99%
“…As pointed out above, the effect of the magnetic field is contained in the local Green's function G ll , therefore, the strategy to solve the DMFT problem is to compute the eigenvalues of the non-interacting lattice in the presence of uniform magnetic field and use them in the selfconsistency loop. There are numerous methods to solve the non-interacting case 3,24,25 . For the numerical example presented below, we take the case of a uniform magnetic field perpendicular to a square lattice and we compute the energy level of Bloch electrons by solving an almost Mathieu equation named Harper equation 26 for rational ratios of magnetic flux, i.e.…”
Section: Methods and Modelmentioning
confidence: 99%
“…Recently, the Green function obtained for the tight-binding model on a square lattice in the applied magnetic field has been expressed by means of continued fractions by Ueta [8]. However, the derived expressions are more complicated, and therefore, as stated by the author, for large values of q (q > 5) are difficult to solve.…”
Section: If One Is Interested In G ð0þmentioning
confidence: 99%
“…(28) in Ref. 13), it is possible to write the eigenvalue of T n (0) as From the above, the equation for the energy band structure is obtained as Hence, the problem of determination of the energy band is reduced to that of ∆ n (x), or a n , b n , c n , and d n .…”
Section: Formulation Of Inverse Problemmentioning
confidence: 99%