Abstract
Basic understanding of the structure and dynamics of materials and their properties often requires knowledge on a microscopic level of the underlying energetics and interaction mechanisms, whose consequences we observe and measure. Answers to material science problems are in principle possible, embodied in solutions to the Schrodinger equation subject to the appropriate boundary conditions. However, the full implementation of such a program is impossible for most (one may dare say all) material science and condensed matter systems and we must resort to various approximations and simplification. The degree of microscopic detail with which we probe physical phenomena is determined mainly by the resolution of our experimental tools, by the ability to found the theoretical analysis on microscopic principles and by the complexity, hence solubility, of the model. In constructing theoretical models of complex material systems we must apply rigorous standards of testing and assessment as to the validity and accuracy of the proposed model. Frequently we rely at this stage on the accessibility and availability of experimental data with sufficient resolution (either as a source of values for some of the model parameters or for comparative purposes) and by the level of simplifications, dictated by considerations of feasibility and practicality, which render the model soluble. In many situations the level of complexity of the model, which is necessary in order to describe faithfully the physical phenomena, is such that analytical approaches fail to provide a solution. In these situations, which include the majority of material systems and phenomena, the use of computer-based methods [1–6] is essential.
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Landman, U. (1988). Molecular Dynamics Simulations in Material Science and Condensed Matter Physics. In: Landau, D.P., Mon, K.K., Schüttler, HB. (eds) Computer Simulation Studies in Condensed Matter Physics. Springer Proceedings in Physics, vol 33. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-93400-1_12
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