From the dipole of a crystallite to the polarization of a crystal

Abstract

The quantum-mechanical expression for the polarization of a crystalline solid does not bear any resemblance to the (trivial) expression for the dipole of a bounded crystallite; in fact, it has been proved via a conceptually different path. Here, I show how to alternatively define the dipole of a bounded sample in a somewhat unconventional way; from such a formula, the crystalline polarization formula—as routinely implemented in electronic-structure codes—follows almost seamlessly.

Document Details

Document Type
Pub Defense Publication
Publication Date
Feb 05, 2021
Source ID
10.1063/5.0040815

Entities

People

  • Raffaele Resta

Organizations

  • Donostia International Physics Center
  • Istituto Officina dei Materiali
  • Office of Naval Research

Tags

Readers

  • Calculus or Mathematical Analysis
  • Quantum Chemistry
  • Systems Analysis and Design

Technology Areas

  • Microelectronics
  • Microelectronics - Graphene
  • Quantum Computing