the provision of telecommunications structures to esb, including, but not limited to,

triangular lattice structures, monopoles, birdcage and stealth structure solutions of various heights and sizes.

To design their novel acoustic metamaterial, the team 3D-printed a series of small trimers, arranged and connected in a

triangular lattice. Each trimer unit consisted of three acoustic resonators.

A conformation C of n residues can be expressed in the form of movement direction such as C e {F, B, U, D}(n-1) and C e {F, B, U, D, FU, BU, BD, FD}(n-1) for two-dimension square and

triangular lattice, respectively.

In this paper, our PC waveguide is operated at 1,550 nm [31], and our PC waveguide is constructed using a 2D

triangular lattice array of air holes embedded in polysilicon (p-Si).

The sub-wavelength resolution of an imaging effects have been demonstrated experimentally [6-9] and theoretically [4, 10-16] for

triangular lattice, square lattice and hexagon lattice PCs.

For the

triangular lattice discussed above all nearest-neighbor interactions are the same.

The grain growth Monte Carlo simulation is performed on a two-dimensional

triangular lattice, where for each lattice site "i" a number [S.sub.i] is assigned which corresponds to the grain orientation [10, 11].

On the diffraction pattern of POVs the formation of a truncated

triangular lattice can be seen, in which the number of the spots along an edge of the triangle minus one represents the topological charge of the incident POV [38].

It is well known to us that in usual

triangular lattice PCF the conventional notations of air-hole diameter are "d" and hole-to-hole distance is "[LAMBDA]." In the analysis of the present square-lattice PCF structures, we use [LAMBDA] as the hole-to-hole spacing in horizontal or vertical direction with d as the diameters of the air holes.

Using source code from the Open Source Physics library written in Java as a basis, I have developed a series of simulations to computationally calculate the critical probability in both a conventional

triangular lattice (pc = 0.5), as well as in a non-trivial lattice such as the kagome lattice (pc = 0.65).

In this work, we present the surface plasmas excitation of the SHG in three-dimensional

triangular lattice structures consisting of noncentrosymmetric split-ring resonators.

227 x [10.sup.-12] erg, mass is scaled by the atomic mass, and lengths are scaled by two-dimensional

triangular lattice parameter , 2.