Showing posts with label journal of carbon nanotubes. Show all posts
Showing posts with label journal of carbon nanotubes. Show all posts

Monday, 19 December 2016

Correlation between Lanczos Method and Exact Diagonalisation Method in the Study of Highly Correlated Electrons System

The Hubbard model is an approximate model used to describe the transition between conducting and insulating systems. The Hubbard model, named after John Hubbard 1963, is the simplest model of interacting particles in lattices, with the only two tennis in the Hamiltonian; a kinetic term allowing for hopping of particles between soles of the lattice and a potential term consisting of an on sites interaction. The particles can either be fermions or bosons.

cosmoparticle physics


The Hubbard model is a good approximate for particles in a periodic potential at sufficiently low temperature that all the particles are in the lowest Bloch band, as long as any long-range interactions between the particles can be ignored. If interaction between particles on different sites of the lattice are included, the model is often referred to as the extended Hubbard model .The model was originally proposed to describe electrons in solids and has since been the focus of particular interest as a model for high temperature super conductivity. Read more>>>>>>>>>>>>>>>

Friday, 16 December 2016

GPS-Compatible Lorentz Transformation that Satisfies the Relativity Principle

The Lorentz transformation (LT) is the centerpiece of Einstein’s special theory of relativity (STR). It satisfies the two postulates of relativity: the relativity principle (RP) and the assumption of the constancy of the speed of light in free space (LSP). It was pointed out as early as 1898 by Lorentz that there is a degree of freedom in the definition of a space-time transformation that satisfies the LSP and/or leaves Maxwell’s equations invariant. He introduced a series of four equations that can be referred to as the General Lorentz transformation (GLT) in which a common normalization function appears on the right-hand side of each relation. 

GPS-Compatible Lorentz Transformation


It therefore follows that there are an infinite number of such transformations that satisfy the LSP. However, the RP puts another constraint on the definition of a fully relativistic space-time transformation. In addition, there is the obvious criterion that the equations must be in agreement with all relevant experimental data In the following it will be shown that, although the LT satisfies both of the relativity postulates, it fails to predict the results of a number of experiments that were carried out in the latter half of the 20th century. Read more>>>>>>>>>