For any canonical linearization, we compute for every linearly bounded lattice the largest distance (in memory words) between any two live lattice elements during the code execution.
The nature of the shift is clearly explained in (Holland 1970): modularity is in effect a weakening of the distributive laws (limiting their validity to certain selected triples of lattice elements), and orthomodularity is a weakening of modularity (limiting the validity of the distributive laws to an even smaller set of triples of lattice elements).
With low lattice densities the effect of each lattice element can be seen in the wake, while the lattice structures act as a porous media for higher densities.
In electric polarization, the centre of positive charge within an atom, molecule, or crystal lattice element is separated slightly from the centre of negative charge.
Here, we break the underlying Si crystal lattice symmetries by including foreign elements in the lattice.
Namely, a good lattice should be as compact as possible, and should be large enough to cover all of the elements; moreover, the quantization error and the error probability of the transmission in AWGN channels should be as small as possible; furthermore, any linear combination of two elements in the lattice should belong to this lattice [19, 20].
At higher N2 partial pressures the growth assumes a columnar epitaxial nature. 1 Å resolution of the lattice enabling location of all elements in the Ti2AlN unit cell is demonstrated.
Markov Random Fields (MRF) represents the distribution of conditional probabilities over elements in a lattice.
In addition, there perhaps exist a few defects or other doping elements in the lattice, which can be found in the left corner of the image.
In order to couple the GRNs in a compartmentalised (cellular) domain, we considered a discrete lattice of n × n elements, in which each element (i, j) represents a cell with a GRN.
