𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Electronic States in Crystals of Finite Size: Quantum Confinement of Bloch Waves

✍ Scribed by Ren Sh. Y.


Book ID
127451943
Year
2005
Tongue
English
Weight
2 MB
Edition
1st edition
Category
Library
ISBN-13
9780387263045

No coin nor oath required. For personal study only.

✦ Synopsis


This book presents an analytical theory on the electronic states in ideal low-dimensional systems and finite crystals, recently developed by the author, based on a differential equation theory approach. It gives some exact and general fundamental understandings on the electronic states in ideal low-dimensional systems and finite crystals, and provides new insights into some fundamental problems in low-dimensional systems such as the surface states, quantum confinement effects, etc., some of which are quite different from what is traditionally believed in the solid state physics community.


πŸ“œ SIMILAR VOLUMES


Electronic States in Crystals of Finite
✍ Shang Yuan Ren (eds.) πŸ“‚ Library πŸ“… 2006 πŸ› Springer 🌐 English βš– 1 MB

The theory of electronic states in the traditionally solid state physics is essentially a theory of electronic states in crystals of infinite size. However, any real crystal always has a finite size. This book presents an analytical theory on the electronic states in ideal low-dimensional systems an

Density of non-Bloch electron states in
✍ T. Bulski; S. Olszewski; A. Wierzbicki πŸ“‚ Article πŸ“… 1980 πŸ› John Wiley and Sons 🌐 English βš– 992 KB

## Abstract This paper gives an abbreviated method for the calculation of the density of states of a crystal on the basis of that band theory in which the crystal electron states are represented by the standinglike wave functions classified according to the point‐group symmetry species. The crystal

Two Types of Electronic States in One-Di
✍ Shang Yuan Ren πŸ“‚ Article πŸ“… 2002 πŸ› Elsevier Science 🌐 English βš– 84 KB

Exact and general results on the electronic states in one-dimensional crystals bounded at Ο„ and Ο„ + L, where L = Na, N is a positive integer, and a is the potential period, are presented. Corresponding to each energy band of the Bloch wave, there are N -1 states in the finite crystal whose energies