Presentation is loading. Please wait.

Presentation is loading. Please wait.

Overview of a Realistic Treatment of Semiconductor Materials.

Similar presentations


Presentation on theme: "Overview of a Realistic Treatment of Semiconductor Materials."— Presentation transcript:

1 Overview of a Realistic Treatment of Semiconductor Materials.
The Tightbinding (LCAO) Method Overview of a Realistic Treatment of Semiconductor Materials.

2 Tightbinding Method Realistic Treatment for Semiconductor Materials!
For most of the materials of interest, in the isolated atom, the valence electrons are in s & p orbitals. Before looking at the bands in the solid, lets first briefly & QUALITATIVELY look at the molecular orbitals for the bonding & antibonding states. A Quantitative treatment would require us to solve the Molecular Schrödinger Equation That is, it would require us to do some CHEMISTRY!! Now, a mostly qualitative review of elementary molecular physics.

3 s orbitals are spherically
Shapes of charge (& probability) densities |ψ|2 for atomic s & p orbitals: s orbitals are spherically symmetric! p orbitals have directional lobes! The py lobe is along the y-axis The px lobe is along the x-axis The pz lobe is along the z-axis

4 Ψ = (ψsA+ ψsB)/(2)½ Ψ = (ψsA - ψsB)/(2)½
Wavefunctions Ψ and energy levels ε for molecular orbitals in Diatomic Molecule AB Ψ for a σ antibonding orbital ψsA ψs An s-electron on atom A bonding with an s-electron on atom B. Ψ for a σ bonding orbital For a homopolar molecule (A = B) ε for a σ antibonding orbital ε for atomic  s electrons ε for a σ bonding orbital Result: A  bonding orbital (occupied; symmetric on exchange of A & B) Ψ = (ψsA+ ψsB)/(2)½ A  antibonding orbital (unoccupied; antisymmetric on exchange of A & B) Ψ = (ψsA - ψsB)/(2)½

5 Ψ = (ψsA+ ψsB)/(2)½ Ψ = (ψsA - ψsB)/(2)½
Wavefunctions Ψ & energy levels ε for molecular orbitals in a Diatomic Molecule AB Ψ for σ antibonding orbital An s-electron on atom A bonding with an s-electron on atom B. Ψ for σ bonding orbital For a heteropolar molecule (A  B) ε for σ antibonding orbital ε for atomic  s electrons on atoms A & B ε for σ bonding orbital Result: A  bonding orbital (occupied; symmetric on exchange of A & B) Ψ = (ψsA+ ψsB)/(2)½ A  antibonding orbital (unoccupied; antisymmetric on exchange of A & B) Ψ = (ψsA - ψsB)/(2)½

6 Ψ = (ψsA+ ψsB)/(2)½  antibonding orbital Ψ = (ψsA - ψsB)/(2)½
Charge (probability) densities |Ψ|2 for molecular orbitals in a Diatomic Molecule AB An s-electron on atom A bonding with an s-electron on atom B to get  bonding (+) &  antibonding (-) molecular orbitals.  bonding orbital: Ψ = (ψsA+ ψsB)/(2)½ (occupied; symmetric on exchange of A & B)  antibonding orbital Ψ = (ψsA - ψsB)/(2)½ (unoccupied; antisymmetric


Download ppt "Overview of a Realistic Treatment of Semiconductor Materials."

Similar presentations


Ads by Google