Upload
allenhermann
View
46
Download
0
Tags:
Embed Size (px)
Citation preview
Lecture II.
. Insulators
Charge Transport Theory, narrow bands
Delocalized (Bloch) Wave Functions
Localized Wave Functions
Excitons
Peirels Distortion (1D systems)
Review of Electronic Properties of Solids
Free Electron Fermi Gas
•Electron in a box: example
Electrons are sufficiently delocalized in
•conjugated molecules that they can be
•considered as an electron box
Electronic absorption of β-carotene
0.294nm
Energy Bands, Semiconductors, Doping
Hydrogen Molecule
Charge Transport Theory General
Figure 9.11. (a) Energy levels in an isolated silicon atom and (b) in a
silicon crystal of N atoms, illustrating the formation of energy bands. The
valence band contains 4N states and can accommodate all 4N valence
electrons.
Figure 7.1. Schematic plot of the single particle energy spectrum in a bulk
semiconductor for both the electron and hole states on the left side of the
panel with appropriate electron (e) and hole (h) discrete quantum states
shown on the right. The upper parabolic band is the conduction band, the
lower the valence.
Holes
Figure 9.12. A valence electron jumping across the energy gap in pure
silicon resulting in the generation of a free electron and hole in the crystal:
(a) energy band model, (b) bond model.
Figure 9.13. Extrinsic n-type silicon doped with P donor atoms. (a) Energy
band diagram and (b) Bond model.
Figure 9.14. Extrinsic p-type silicon doped with B acceptor atoms. (a)
Energy band diagram and (b) Bond model.
Electronic structures of Organic Molecules (1) Core electrons. (2) s electrons, localized between two atoms. (3) n electrons, located at a particular heteroatom, usually have high orbital
energy and could be promoted easily. (4) p electrons, delocalized over an array of atoms, usually have high MO
energy and could be promoted easily.
Linear Combination of Atomic Orbitals
LCAO
Density Functional Theory
Background
• 1920s: Introduction of the Thomas-Fermi model.
• 1964: Hohenberg-Kohn paper proving existence of exact DF.
• 1965: Kohn-Sham scheme introduced.
• 1970s and early 80s: LDA. DFT becomes useful.
• 1985: Incorporation of DFT into molecular dynamics (Car-Parrinello)
(Now one of PRL’s top 10 cited papers).
• 1988: Becke and LYP functionals. DFT useful for some chemistry.
• 1998: Nobel prize awarded to Walter Kohn in chemistry for
development of DFT.
1 1( , ,..., , )N Ns s r r
Lecture 8: Introduction to Density Functional
Theory
Marie Curie Tutorial Series: Modeling Biomolecules December 6-11, 2004
Mark Tuckerman
Dept. of Chemistry
and Courant Institute of Mathematical Science
100 Washington Square East
New York University, New York, NY 10003
Amorphous Semiconductors
Let’s estimate the mean free path, lmax=l. Let vmax=v.
The carrier mobility is defined as μ= eτ/m*, where τ is the carrier relaxation time. Consider for mfree carrier=m*=m. We take l=v τ . and ½mv2=3/2 kT, all of which gives l=√(3kTm/e2 ) μ or l=0.7 μ where l is in angstrom units and μ is in cm2/v sec
Transport between “isolated” molecules
Excitons
A peculiarity in some One-dimensional systems:
Peierls Distortion