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DEpartment of physics

THUSHARI Jayasekera - ASSistant Professor

Solid State Physics - PHYS 425
Class Meets on MWF 1.00 pm - 1.50 pm,
Office Hours - MWF 11.00 am - 1.00 pm (Neckers 489)
 

       

Main Content Area

Electronic Properties of Materials

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The objective of this section is to understand the electron energy levels in periodic solids. This is called the Electron structure theory.

In fact, electron structure theory is a major part of solid state physics. The knowledge of electron structure leads to many other directions to understand/explain experimental observations such as optical absorption, electron mobility, electron transport etc.

Here we will discuss several models that have been developed to explain experimental observations for different situations. First we are going to assume that electrons are free to move across solid. This model is called the free electron gas model, which means, some electron of solid are free like gas particles. Let's first start with a classical approach to describe the free electron gas.


So, how can we understand the electronic energy of a periodic solid. In principle, the answer is simple. All we have to do is to solve the Schrodinger equation for the system.

$$ H \Psi = \epsilon \Psi $$

where HH is the Hamiltonian of the system. ϵ\epsilon gives the energy levels that we have been looking for.

Hamiltonian of the system can be written as:

$$H=H_{KE}+H_{ee}+H_{eN}+H_{nn}+H_{KE_n} $$

HKEH_{KE}        - Kinetic Energy of electrons
HeeH_{ee}     -electron-electron electrstatic potential energy (or electron-electron interaction energy)
HeNH_{eN}     - electron - Nucleus electrostatic potential energy
HnnH_{nn}     - Nucleus-Nucleus interaction energy
HKEnH_{KE_n}   - Kinetic Energy of Electrons

All we have to do is solve the Schrodinger equation. But the problem is, how do we solve it? Do we know how to exlicitly write this hamiltonian.

In your Quantum Mechanics classes, you have solved the Schrodinger equation for a particle in a box - Quantum Well problem, an electron in a Simple Harmonic Oscillator Potential, Hydrogen atom.

That's pretty much it. We did not even solve for the electronic energy levels in Helium atom. Why?  We are not able to solve the problem exactly. Some level of approximations and Computational algorithms are needed to solve this problem.

Good News is: Over the years of work with several approximation schemes, and with advanced computational power, the field of electronic structure theory is well developed.

We will discuss the Quantum Mechanical approach to describe electronic properties of materials in various steps.







Thushari Jayasekera, Assistant Professor of Physics, Southern Illinois University - Carbondale
Tel: 618 453 1055 Fax: 618 453 1056

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