TF EIM Chapt3
Semiconductor physics
There are 5 states of matter: Solid, liquid, gas, plasma (ionized gas) , and a Bose-Einstein condensate (quantum effects on a macroscopic scale).
Crystal Lattice
Semiconductor physics focuses on the solid state of matter in the form of crystals.
Crystals are formed when atoms are arranged in repeating structures called the crystal lattice. The recurrent structure which forms the crystal lattice is referred to a a cell.
Some popular cell names are
(SC) Simple Cubic | (BCC) Body Centered Cubic | (FCC) Face Centered Cubic |
The above images are suppose to represent the distribution of electrons in the crystal lattice cell.
To understand this structure more let's consider the structure of a 1-D crystal of atoms
A single free atom will have electrons bound to the atom due to the coulomb force. The bound electrons are found in various energy levels.
- Notice
- When you add the atoms to form the lattice, the potential barrier is lowered. This allows the electrons in the higher (more valence) states to become shared among adjacent atoms.( Delocalized)
There are 14 different Bravais lattice configurations
Crystal System | Lattice type |
Cubic | Simple, Face Centered, Body Centered |
Tetragonal | Simple, Body Centered |
Orthorhombic | Simple, Face Centered, Body Centered, End Centered |
Monoclinic | Simple, End Centered |
Rhombohedral | Simple |
Triclinic | Simple |
Hexagonal | Simple |
Most Semiconductors are made from Silicon and GaAs.
Silicon is a Face Centered Cubic cell
Silicon is an insulator if in pure form with 4 weakly bound (valence) electrons.
If you replace silicon atoms in the lattice with atoms that have either 3 valance or 5 valence electrons (doping) your can create sites with either a deficient number of electrons (a missing bond) or extra electrons (complete bond with a free electron)
By Doping silicon you can create sites with extra electrons (n-type) or sites with a deficient number of electrons (vacancies or holes ) (P-type)