Ashcroft, N. W., & Mermin, N. D. (1976). Solid state physics. Holt, Rinehart and Winston.
Kronig, R. de L., & Penney, W. G. (1931). Quantum mechanics of electrons in crystal lattices. Proceedings of the Royal Society of London A, 130(814), 499-513. quantum theory of solids kittel pdf
The nearly free electron model is a more advanced model for understanding the electronic structure of solids. Kittel presents a detailed analysis of this model, which assumes that the electrons in a solid can be treated as nearly free particles with weak periodic perturbations. The nearly free electron model provides a powerful framework for understanding the behavior of electrons in metals, enabling the calculation of important properties such as the Fermi surface and the electronic specific heat. Ashcroft, N
Kittel begins by introducing the free electron model, which posits that the electrons in a solid can be treated as non-interacting particles moving in a periodic potential. This model is a crucial starting point for understanding the behavior of electrons in solids, as it provides a simple yet powerful framework for describing the electronic structure of metals. The free electron model is based on the Sommerfeld theory, which assumes that the electrons in a metal can be described using the Fermi-Dirac distribution. Kittel derives the key results of the free electron model, including the density of states, the Fermi energy, and the electronic specific heat. (1976)
The Bloch theorem, introduced by Felix Bloch in 1928, is a fundamental concept in the quantum theory of solids. The theorem states that the wave function of an electron in a periodic potential can be written as a product of a plane wave and a periodic function with the same periodicity as the lattice. Kittel presents a detailed derivation of the Bloch theorem, highlighting its significance for understanding the behavior of electrons in solids. The Bloch theorem provides a powerful tool for analyzing the electronic structure of solids, enabling the classification of solids into metals, semiconductors, and insulators.
Kittel also explores the electronic structure of insulators and semiconductors, highlighting their distinct properties and behavior. Insulators are characterized by a full valence band and an empty conduction band, while semiconductors have a partially filled valence band and a partially empty conduction band. Kittel explains how the electronic structure of insulators and semiconductors arises from the underlying quantum mechanics of solids, highlighting the importance of energy gaps and the role of impurities.