Titlebook: Condensed Matter Theories; Volume 6 S. Fantoni,S. Rosati Book 1991 Plenum Press, New York 1991 atom.condensed matter.development.diffusion.

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https://doi.org/10.1007/978-3-476-99696-1e neglected. It is the exchange interaction that determines the basic magnetic properties of such systems and gives the predominant contribution to the dynamics of macroscopic magnetization. In particular, the spectrum of spin fluctuations is determined mainly by the magnitude of electron-electron exchange interaction.

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Book 1991ba, Italy, from 18-23 June, 1990. The Workshop started in 1977 in Sao Paolo, Brazil, as the 1st Pan American Workshop on Condensed Matter Theories, with the purpose of bringing together scientists from the Western countries, working in many different topics of Condensed Matter Theories, to facilitat

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Changing Structure of Rural Employment. Since there are in general many pathways by which information can travel through an intricate mesh of connections, processing in a neural network is said to be “massively parallel” as opposed to sequential.

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https://doi.org/10.1007/978-3-0348-6560-9agg intensities. A detailed comparison with neutron and x-ray scattering results is made wherever possible. The anomalous diffuse neutron and x-ray scattering in the vicinity of q.=(1.6, 1, 0) is calculated.

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Artificial Neural Networks that Learn Many-Body Physics. Since there are in general many pathways by which information can travel through an intricate mesh of connections, processing in a neural network is said to be “massively parallel” as opposed to sequential.

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Quantum Statistical Microdynamics and Critical Phenomenadinary differential equations (ODEs) plus a stochastic ruleset constitute a system of microscopic Langevin equations that can be solved numerically for the quantum statistical microdynamic behavior of the many-atom optical svstem being: studied.

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Bragg Intensities and Diffuse Scattering in Ag2Se: A Molecular Dynamics Studyagg intensities. A detailed comparison with neutron and x-ray scattering results is made wherever possible. The anomalous diffuse neutron and x-ray scattering in the vicinity of q.=(1.6, 1, 0) is calculated.