1. Electrical Engineering Materials
Dr. Md. Sherajul Islam
Associate Professor
Department of Electrical and Electronics Engineering Khulna University of Engineering & Technology
Khulna, Bangladesh

2. LECTURE - 5
Modern Theory of Solids

3. Infinite Square-Well Potential
Time-independent Schrödinger equation
Infinite Square-Well Potential
The simplest such system is that of a particle trapped in a box with infinitely hard walls that the particle cannot penetrate. This potential is called an infinite square well and is given by
Clearly the wave function must be zero where the potential is infinite.
Where the potential is zero inside the box, the Schrödinger wave equation becomes where .
The general solution is .

6. Finite Square-Well Potential
The finite square-well potential is
The Schrödinger equation outside the finite well in regions I and III is
or using
yields The solution to this differential has exponentials of the form eαx and e-αx. In the region x > L, we reject the positive exponential and in the region x < L, we reject the negative exponential.

7. Finite Square-Well Solution
Inside the square well, where the potential V is zero, the wave equation becomes where
Instead of a sinusoidal solution we have
The boundary conditions require that
and the wave function must be smooth where the regions meet.
Note that the wave function is nonzero outside of the box.

8. Band structure of Solids
The energy spectrum gradually changes as atoms are assembled to form the solid

9. Band Theory of Solids Two ways: both same direction (+) Or
Molecular orbital formation
Two ways: both same direction (+) Or
opposite direction (-)

10. Molecular orbital formation
The bonding orbital shows a local minimum in the wavefunction but the function does not go to zero. Thus there is a finite probability of finding the electron between the 2 atoms. The anti-bonding orbital wavefuntion goes to zero hence the probability of finding the electron between the 2 atoms is zero. This is called a node.

11. Molecular orbital formation
Figure 1.3: (a) Energy vs. bond length plot for 2 H atoms. (b) The schematic representation of the formation of the H2 molecule. Both electrons go to the bonding orbital while the anti-bonding orbital is empty.

12. Figure 1. 4: MOs formed when 3 H atoms come together
Figure 1.4: MOs formed when 3 H atoms come together. The number of nodes increases while the stability decreases. The configuration with the lowest number of nodes is most stable.

13. Figure 1. 6: Energy vs. bond length diagram for N Li atoms
Figure 1.6: Energy vs. bond length diagram for N Li atoms. There are a total of 2N energy states (including spin) out of which N are occupied, half full. This makes Li a metal

14. The band formed by the empty 2p shell as the conduction band.
Figure 1.7: Energy vs. bond length diagram for large values of N showing a continuous band formation. The overlap between the 2s, 2p, and 3s levels are also shown
The energy required to remove an electron from the Fermi level to vacuum level (where the electron is free of the influence of the metal) is called the work function.
The separation between the filled states and the empty states is called the Fermi energy and is denoted by EF
The band formed by the empty 2p shell as the conduction band.

15. energy of vibrating electron = (any integer) x hf
So how does this explain the spectrum of blackbody radiation? Planck said that an electron vibrating with a frequency f could only have an energy of 1 hf, 2 hf, 3 hf, 4 hf, ... ; that is,
energy of vibrating electron = (any integer) x hf
But the electron has to have at least one quantum of energy if it is going to vibrate. If it doesn't have at least an energy of 1hf, it will not vibrate at all and can't produce any light. "A ha!" said Planck: at high frequencies the amount of energy in a quantum, hf, is so large that the high-frequency vibrations can never get going! This is why the blackbody spectrum always becomes small at the left-hand (high 
Figure 1.8: Fermi energy and work function in Li. By convention the vacuum level is taken as zero and energy levels within the metal are shown as negative. If the lowest energy level in the valence band is used as reference all these energy levels become positive

16. Figure 2. 4: Formation of energy bands in Si
Figure 2.4: Formation of energy bands in Si. (a) Si atom with 4 electrons in outer shell form (b) 4 sp3 hybrid orbitals. (c) The hybrid orbitals form σ and σ ∗ orbitals. (d) These orbitals overlap in a solid to form the valence and conduction band.

17. Properties of Electron in a Band

18. Properties of Electron in a Band

19. Electron Effective Mass

20. Electron Effective Mass

21. E-K Diagram E

22. Calculation of Effective mass from E-K Diagram
What is the significance of E-K Diagram ??

23. Density of states in an Energy Band
The density of states (DOS) of a system describes the number of available states per unit energy per unit volume

24. Density of states in an Energy Band

25. Detail derivation of DOS from Book
Density of states in an Energy Band
Detail derivation of DOS from Book

26. Boltzman Classical Statistics
In statistical mechanics, Maxwell–Boltzmann statistics describes the average distribution of non-interacting material particles over various energy states in thermal equilibrium, and is applicable when the temperature is high enough or the particle density is low enough to render quantum effects negligible.

27. Boltzman Classical Statistics

28. Fermi-Dirac Statistics
In quantum statistics, a branch of physics, Fermi–Diracstatistics describe a distribution of particles over energy states in systems consisting of many identical particles that obey the Pauli exclusion principle.