Each lattice A in W determines a sequence of Brillouin zones Bn, fundamental regions for A bounded by Bragg hyperplanes; for example B, is the Dirichlet region. Basic geometric and topological properties of these zones are established, and we obtain asymptotic estimates (valid for almost all A) for n X(n) = £ ^(') » where L(n) is the number of connected components of the interior of Bn (called Landsberg subzones). Fermi surfaces are also briefly described. 1
Let Ln denote the lowest crossing of a square 2n×2n box for critical site percolation on the triangu...
International audienceIn solid-state physics, including photonics and wherever periodic lattice stru...
International audienceAs a consequence of Bloch's theorem, the numerical computation of the fermioni...
http://deepblue.lib.umich.edu/bitstream/2027.42/5900/5/bac5635.0001.001.pdfhttp://deepblue.lib.umich...
A simple method to overcome convergence problems in Brillouin zone summations of lattice dynamical p...
http://deepblue.lib.umich.edu/bitstream/2027.42/7723/5/agb8617.0004.001.pdfhttp://deepblue.lib.umich...
After recalling the first Brillouin zone (BZ) and the first irreducible Brillouin zone (IBZ) of a la...
The Nielsen-Ninomiya Theorem has set up a ground rule for the minimal number of the topological poin...
We extend the physics of graphene to three dimensional systems by showing that Dirac points can exis...
The Nielsen-Ninomiya theorem set up a ground rule for the minimal number of the topological points i...
For a locally finite set in R2, the order-k Brillouin tessellations form an infinite sequence of con...
For a locally finite set in R2, the order-k Brillouin tessellations form an infinite sequence of con...
We extend the physics of graphene to three dimensional systems by showing that Dirac points can exis...
We extend the physics of graphene to three dimensional systems by showing that Dirac points can exis...
The shape of the Fermi surface determines the kinetic and equilibrium properties of the elec-tron ga...
Let Ln denote the lowest crossing of a square 2n×2n box for critical site percolation on the triangu...
International audienceIn solid-state physics, including photonics and wherever periodic lattice stru...
International audienceAs a consequence of Bloch's theorem, the numerical computation of the fermioni...
http://deepblue.lib.umich.edu/bitstream/2027.42/5900/5/bac5635.0001.001.pdfhttp://deepblue.lib.umich...
A simple method to overcome convergence problems in Brillouin zone summations of lattice dynamical p...
http://deepblue.lib.umich.edu/bitstream/2027.42/7723/5/agb8617.0004.001.pdfhttp://deepblue.lib.umich...
After recalling the first Brillouin zone (BZ) and the first irreducible Brillouin zone (IBZ) of a la...
The Nielsen-Ninomiya Theorem has set up a ground rule for the minimal number of the topological poin...
We extend the physics of graphene to three dimensional systems by showing that Dirac points can exis...
The Nielsen-Ninomiya theorem set up a ground rule for the minimal number of the topological points i...
For a locally finite set in R2, the order-k Brillouin tessellations form an infinite sequence of con...
For a locally finite set in R2, the order-k Brillouin tessellations form an infinite sequence of con...
We extend the physics of graphene to three dimensional systems by showing that Dirac points can exis...
We extend the physics of graphene to three dimensional systems by showing that Dirac points can exis...
The shape of the Fermi surface determines the kinetic and equilibrium properties of the elec-tron ga...
Let Ln denote the lowest crossing of a square 2n×2n box for critical site percolation on the triangu...
International audienceIn solid-state physics, including photonics and wherever periodic lattice stru...
International audienceAs a consequence of Bloch's theorem, the numerical computation of the fermioni...