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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书目名称Condensed Matter Theories影响因子(影响力)




书目名称Condensed Matter Theories影响因子(影响力)学科排名




书目名称Condensed Matter Theories网络公开度




书目名称Condensed Matter Theories网络公开度学科排名




书目名称Condensed Matter Theories被引频次




书目名称Condensed Matter Theories被引频次学科排名




书目名称Condensed Matter Theories年度引用




书目名称Condensed Matter Theories年度引用学科排名




书目名称Condensed Matter Theories读者反馈




书目名称Condensed Matter Theories读者反馈学科排名

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Grasping

Quantum Spin Lattice Models: A Coupled-Cluster Treatmenttensions to regular lattices in higher numbers of dimensions, have been objects of theoretical interest for a very long time. Indeed, the exact energy eigenstates of the one-dimensional spin-half chain interacting via the isotropic Heisenberg interaction between neighbouring sites,. were exactly sol

夹克怕包裹

Time Dependent Mean Field Approximation in a Boson Systemthis approach provides the main dynamical features of the problem. It can be applied for all values of the coupling strength and number of particles and provides a description valid on both sides of the superconducting phase transition. It clearly points out the phase transition through changes in t

nonradioactive

Inhomogeneous Boson Systems Made Planartems. Both methods effectively deal with the short-range correlations induced by the twobody interaction and the long-range correlations characteristic of quantum many-body systems. In the language of perturbation theory, they both perform a reasonably selfconsistent summation of ring diagrams and l

Eeg332

Eeg332

Single Particle Properties of Atomic Deuteriumterium are evaluated beginning from the Fermi gas and the pair potential. Single particle energies, lifetimes, effective mass near the Fermi surface and the interaction between particles are determined. The aim is to see how well these properties can be evaluated using Green function methods. We fin

HEDGE

吹牛者

Collective Spin Waves in Maxwellian Electron Plasmaic phenomena. Metals, alloys, and semiconductors are, of course, the most typical conducting systems with delocalized electron spins. In these cases electrons form a strongly degenerate Fermiliquid in which the exchange interaction between electrons always plays a very important role and can never b

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