Abstract:Finite strips, composed of a periodic stacking of infinite quasiperiodic Fibonacci chains, have been investigated in terms of their electronic properties. The system is described by a tight binding Hamiltonian. The eigenvalue spectrum of such a multi-strand quasiperiodic network is found to be sensitive on the mutual values of the intra-strand and inter-strand tunnel hoppings, whose distribution displays a unique three-subband self-similar pattern in a parameter subspace. In addition, it is observed that speci… Show more
“…Finally, let us note that the possibility of Bloch-states in coupled aperiodic setups has also been observed in references [12,13], in which more complicated coupling schemes have been used.…”
Section: Coupling Only a Or Only B-sitesmentioning
confidence: 74%
“…Although the behavior of aperiodic chains has been investigated extensively and in great detail, comparatively little work has been dedicated to the case where two or more chains are coupled to each other, forming an aperiodic ladder [11][12][13][14][15]. In this work, we take a step into this realm by analyzing a range of different coupling schemes between two identical one-dimensional Fibonacci chains.…”
The Fibonacci chain, i.e., a tight-binding model where couplings and/or
on-site potentials can take only two different values distributed according to the
Fibonacci word, is a classical example of a one-dimensional quasicrystal. With its
many intriguing properties, such as a fractal eigenvalue spectrum, the Fibonacci chain
offers a rich platform to investigate many of the effects that occur in three-dimensional
quasicrystals. In this work, we study the eigenvalues and eigenstates of two identical
Fibonacci chains coupled to each other in different ways. We find that this setup allows
for a rich variety of effects. Depending on the coupling scheme used, the resulting
system (i) possesses an eigenvalue spectrum featuring a richer hierarchical structure
compared to the spectrum of a single Fibonacci chain, (ii) shows a coexistence of Bloch
and critical eigenstates, or (iii) possesses a large number of degenerate eigenstates,
each of which is perfectly localized on only four sites of the system. If additionally, the
system is infinitely extended, the macroscopic number of perfectly localized eigenstates
induces a perfectly flat quasi band. Especially the second case is interesting from an
application perspective, since eigenstates that are of Bloch or of critical character
feature largely different transport properties. At the same time, the proposed setup
allows for an experimental realization, e.g., with evanescently coupled waveguides,
electric circuits, or by patterning an anti-lattice with adatoms on a metallic substrate.
“…Finally, let us note that the possibility of Bloch-states in coupled aperiodic setups has also been observed in references [12,13], in which more complicated coupling schemes have been used.…”
Section: Coupling Only a Or Only B-sitesmentioning
confidence: 74%
“…Although the behavior of aperiodic chains has been investigated extensively and in great detail, comparatively little work has been dedicated to the case where two or more chains are coupled to each other, forming an aperiodic ladder [11][12][13][14][15]. In this work, we take a step into this realm by analyzing a range of different coupling schemes between two identical one-dimensional Fibonacci chains.…”
The Fibonacci chain, i.e., a tight-binding model where couplings and/or
on-site potentials can take only two different values distributed according to the
Fibonacci word, is a classical example of a one-dimensional quasicrystal. With its
many intriguing properties, such as a fractal eigenvalue spectrum, the Fibonacci chain
offers a rich platform to investigate many of the effects that occur in three-dimensional
quasicrystals. In this work, we study the eigenvalues and eigenstates of two identical
Fibonacci chains coupled to each other in different ways. We find that this setup allows
for a rich variety of effects. Depending on the coupling scheme used, the resulting
system (i) possesses an eigenvalue spectrum featuring a richer hierarchical structure
compared to the spectrum of a single Fibonacci chain, (ii) shows a coexistence of Bloch
and critical eigenstates, or (iii) possesses a large number of degenerate eigenstates,
each of which is perfectly localized on only four sites of the system. If additionally, the
system is infinitely extended, the macroscopic number of perfectly localized eigenstates
induces a perfectly flat quasi band. Especially the second case is interesting from an
application perspective, since eigenstates that are of Bloch or of critical character
feature largely different transport properties. At the same time, the proposed setup
allows for an experimental realization, e.g., with evanescently coupled waveguides,
electric circuits, or by patterning an anti-lattice with adatoms on a metallic substrate.
“…The strength of our analytical attempt lies in the fact that we can obtain an exact mapping of a two or multiarm quasiperiodic ladder network into a set of completely 'isolated' linear chains that describe the quantum mechanics of a class of pseudoparticles. Such an exact mapping has already been demonstrated in ladder-like geometries [16,17,23] modelling a DNA-like double chain or a quasi-two dimensional mesh with correlated disorder in the context of de-localization of single particle eigenstates.…”
Double-stranded quasiperiodic copper mean arrangement has been studied in respect of their electronic property and thermoelectric signature. The two-arm network is demonstrated by a tightbinding Hamiltonian. The eigenspectrum of such aperiodic mesh that does not convey translational invariance, is significantly dependent on the parameters of the Hamiltonian. It is observed that specific correlation between the parameters obtained from the commutation relation between the on-site energy and overlap integral matrices can eventually modify the spectral nature and generate absolutely continuous energy spectrum. This part is populated by atypical extended states that has a large localization length substantiated by the flow of the hopping integral under successive real space renormalization group method steps. This sounds delocalization of single particle energy states in such non-translationally invariant networks. Further this can be engineered at will by selective choice of the relative strengths of the parameters. This precise correlation has a crucial impact on the thermoelectric behavior. Anomalous nature of thermoelectric coefficient may inspire the experimentalists to frame tunable thermo-devices. Specific correlations can help us to tune the continuous band and determine the band position at will.
A periodic network of connected rhombii, mimicking a spintronic device, is shown to exhibit an intriguing spin-selective extreme localization, when submerged in a uniform out-of plane electric field. The topological Aharonov-Casher phase acquired by a travelling spin is seen to induce a complete caging, triggered at a special strength of the spin-orbit coupling, for half-odd integer spins s ≥ n /2, with n odd, sparing the integer spins. The observation finds exciting experimental parallels in recent literature on caged, extreme localized modes in analogous photonic lattices. Our results are exact.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.