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.
Wannier, G. H. (1937). The structure of electronic energy bands in crystals. Physical Review, 52(11), 831-836.
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. quantum theory of solids kittel pdf
Kittel, C. (2018). Introduction to solid state physics. John Wiley & Sons.
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. Kronig, R
Ashcroft, N. W., & Mermin, N. D. (1976). Solid state physics. Holt, Rinehart and Winston.
Kittel devotes considerable attention to the concept of energy bands and Brillouin zones, which are essential for understanding the electronic structure of solids. Energy bands represent the allowed energy levels of electrons in a solid, while Brillouin zones are the regions of reciprocal space where the energy bands are defined. Kittel explains how the energy bands and Brillouin zones are constructed, highlighting their significance for understanding the behavior of electrons in solids. (1931)
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.