Splitting rules of electronic miniband in Fibonacci superlattices: a gap map approach

The splitting rules of fragmental miniband in Fibonacci superlattices (FSLs) with arbitrary basis and generation orders are presented through a gap map diagram. Based on the gap map, we find the invariant conditions of the band structure splitting in the FSL for arbitrary generation orders. Moreover, the band structure splitting can be divided to form many regions, each having a similar pattern. In each region, the widths of most gap bands except two major gaps will decrease for increasing the generation order. It is interesting that the center and gap width of the major gaps will converge to constant values for increasing the generation order of the FSL. Based on the splitting rules displayed in the gap map, it is convenient to predict the fragmental band structure in the FSL for arbitrary generation orders and bases.

[1]  B. Djafari-Rouhani,et al.  Localised electronic states in semiconductor superlattices , 2002 .

[2]  Kumar,et al.  Electronic structure of a quasiperiodic superlattice. , 1987, Physical review letters.

[3]  P. Anderson Absence of Diffusion in Certain Random Lattices , 1958 .

[4]  C. Gong,et al.  PROPERTY OF FIBONACCI NUMBERS AND THE PERIODICLIKE PERFECTLY TRANSPARENT ELECTRONIC STATES IN FIBONACCI CHAINS , 1998 .

[5]  J. C. Flores Transport in models with correlated diagonal and off-diagonal disorder , 1989 .

[6]  Liu,et al.  Branching rules of the energy spectrum of one-dimensional quasicrystals. , 1991, Physical review. B, Condensed matter.

[7]  F. Moura,et al.  Delocalization in the 1D Anderson Model with Long-Range Correlated Disorder , 1998 .

[8]  Nori,et al.  Spectral splitting and wave-function scaling in quasicrystalline and hierarchical structures. , 1990, Physical review. B, Condensed matter.

[9]  Wei Hong,et al.  Evolution of wrinkles in hard films on soft substrates. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[10]  E. L. Albuquerque,et al.  Theory of elementary excitations in quasiperiodic structures , 2003 .

[11]  Roy,et al.  Landauer resistance of Thue-Morse and Fibonacci lattices and some related issues. , 1994, Physical review. B, Condensed matter.

[12]  J. Cahn,et al.  Metallic Phase with Long-Range Orientational Order and No Translational Symmetry , 1984 .

[13]  Chao Tang,et al.  Localization Problem in One Dimension: Mapping and Escape , 1983 .

[14]  Felix M. Izrailev,et al.  LOCALIZATION AND THE MOBILITY EDGE IN ONE-DIMENSIONAL POTENTIALS WITH CORRELATED DISORDER , 1999 .

[15]  Domínguez-Adame,et al.  Physical nature of critical wave functions in Fibonacci systems. , 1995, Physical review letters.

[16]  Enrique Maciá,et al.  The role of aperiodic order in science and technology , 2006 .

[17]  P. Mahapatra,et al.  Current density in generalized Fibonacci superlattices under a uniform electric field , 2008, Journal of physics. Condensed matter : an Institute of Physics journal.

[18]  D. Nolte,et al.  Electroabsorption spectroscopy of effective-mass Al x Ga 1 − x A s / G a A s Fibonacci superlattices , 1997 .

[19]  D. Jin,et al.  Matrix maps for substitution sequences in the biquaternion representation , 2005 .

[20]  Critical level statistics of the Fibonacci model , 2004, cond-mat/0410187.

[21]  Merlin,et al.  Quasiperiodic GaAs-AlAs heterostructures. , 1985, Physical review letters.

[22]  P. Carpena,et al.  Metal-insulator transition in random Kronig-Penney superlattices with long-range correlated disorder , 2006 .

[23]  P. Phillips,et al.  Localization and Its Absence: A New Metallic State for Conducting Polymers , 1991, Science.

[24]  Danhong Huang,et al.  Electrical resistance of ballistic-electron transport through a finite disordered Fibonacci chain , 2004 .