Unit 5 - Notes

PHY110 8 min read

Unit 5: Solid State Physics

1. Free Electron Theory

1.1 Introduction

The free electron theory attempts to explain the physical properties of metals, such as electrical and thermal conductivity.

  • Classical Free Electron Theory (Drude-Lorentz Model): Assumes metals contain a gas of free electrons that move randomly inside the lattice. These electrons collide with positive ion cores, but between collisions, they move freely.
  • Quantum Free Electron Theory (Sommerfeld Model): Improves upon the classical model by treating electrons as quantum particles obeying Fermi-Dirac statistics and the Pauli Exclusion Principle. Electrons are confined to a potential well, and energy levels are quantized.

1.2 Drift and Diffusion Current (Qualitative)

Current in solids arises from two distinct transport mechanisms:

A. Drift Current

  • Definition: The directed flow of charge carriers under the influence of an applied external electric field.
  • Mechanism: When an electric field () is applied, carriers accelerate but undergo collisions. This results in a constant average velocity called drift velocity ().
  • Formula:
    • where is current density, is conductivity, is carrier concentration, is charge, and is mobility.

B. Diffusion Current

  • Definition: The flow of charge carriers from a region of higher concentration to a region of lower concentration.
  • Mechanism: This is a statistical process driven by the random thermal motion of particles seeking equilibrium (concentration gradient). No electric field is required.
  • Formula (Fick's Law):
    • where is the diffusion coefficient and is the concentration gradient.

2. Statistical Mechanics of Electrons

2.1 Fermi Energy ()

Fermi energy is a critical concept in quantum mechanics referring to the energy state of electrons in a solid.

  • Definition at 0K: The highest energy level occupied by an electron in a solid at absolute zero temperature (0 Kelvin).
  • Significance: It separates filled energy states from empty energy states at 0K. Only electrons near the Fermi level participate in conduction at temperatures above 0K.

2.2 Fermi-Dirac Distribution Function

This function gives the probability that a quantum state with energy is occupied by an electron at a given temperature .

The Formula:

Where:

  • = Boltzmann constant
  • = Absolute temperature
  • = Fermi Energy

Behavior with Temperature:

  1. At :
    • If , the exponential term is $0$, so (100% occupancy).
    • If , the exponential term is , so (0% occupancy).
    • Result: A step function.
  2. At :
    • Electrons near the Fermi level gain thermal energy and jump to higher states. The step function "smears" out.
    • At exactly , .

A 2D plot showing the Fermi-Dirac distribution function f(E) versus Energy (E). The Y-axis represent...
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3. Theory of Solids: Band Theory

3.1 Formation of Allowed and Forbidden Energy Bands

  • Isolated Atoms: In a single isolated atom, electrons occupy discrete, sharp energy levels.
  • Crystal Formation: As atoms are brought together to form a solid lattice, the wave functions of outer electrons overlap. Due to the Pauli Exclusion Principle, discrete energy levels split into multiple closely spaced levels (N levels for N atoms).
  • Bands: These closely spaced levels form continuous Energy Bands.
    • Valence Band (VB): The band containing valence electrons (highest occupied band).
    • Conduction Band (CB): The next higher band, which may be empty or partially filled. Electrons here are free to move.
    • Forbidden Energy Gap (): The energy difference between the top of the VB and the bottom of the CB. No electrons can exist in this region.

3.2 Classification: Semiconductors and Insulators

Based on the band structure ():

  1. Insulators:

    • Very wide band gap ( eV, typically ~6 eV like Diamond).
    • VB is full; CB is empty.
    • Electrons cannot jump the gap at room temperature; hence, conductivity is negligible.
  2. Semiconductors:

    • Narrow band gap ( eV; Si = 1.1 eV, Ge = 0.7 eV).
    • At 0K, they behave like insulators.
    • At Room Temp, thermal energy excites some electrons from VB to CB, enabling conductivity.
  3. Conductors (Metals):

    • VB and CB overlap ().
    • Electrons are always free to move.

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3.3 Concept of Effective Mass

When an electron moves inside a periodic lattice, it interacts with the internal potential of the nuclei. It does not respond to external forces as a "free" particle of mass .

  • Effective Mass (): A parameter that accounts for the internal forces within the crystal lattice. It relates external force to acceleration: .
  • Mathematical Definition: Depends on the curvature of the (Energy-momentum) curve.
  • Significance:
    • Near the bottom of the CB, curvature is positive is positive (Electron).
    • Near the top of the VB, curvature is negative is negative. This negative mass behavior is treated physically as a positive charge carrier called a Hole.

4. Semiconductor Physics

4.1 Fermi Level in Intrinsic and Extrinsic Semiconductors

A. Intrinsic (Pure) Semiconductors:

  • Electron concentration () = Hole concentration ().
  • The Fermi level lies exactly in the middle of the forbidden gap.

B. Extrinsic (Doped) Semiconductors:
Doping introduces impurity energy levels.

  1. N-Type (Donor Doped):

    • Pentavalent impurity (e.g., Phosphorus).
    • Donates extra electrons.
    • Donor energy level () forms just below the Conduction Band.
    • Fermi Level: Shifts upward toward the Conduction Band ().
  2. P-Type (Acceptor Doped):

    • Trivalent impurity (e.g., Boron).
    • Creates holes (vacancies).
    • Acceptor energy level () forms just above the Valence Band.
    • Fermi Level: Shifts downward toward the Valence Band ().

4.2 Direct vs. Indirect Band Gap Semiconductors

Based on the alignment of the Conduction Band minimum and Valence Band maximum in "k-space" (momentum space).

Feature Direct Band Gap Indirect Band Gap
Structure Max of VB and Min of CB occur at the same momentum value (). Max of VB and Min of CB occur at different momentum values ().
Recombination Electron falls directly to VB emitting a photon. Electron needs a change in momentum (via lattice vibration/phonon) to recombine.
Emission Emits light efficiently (Photons). Energy released mostly as heat (Phonons).
Examples GaAs (Gallium Arsenide), InP. Si (Silicon), Ge (Germanium).
Uses LEDs, Laser Diodes. Rectifiers, Transistors.

5. The Hall Effect

5.1 Definition

When a magnetic field () is applied perpendicular to a current-carrying conductor (), a voltage is developed across the specimen in a direction perpendicular to both the current and the magnetic field. This is called the Hall Voltage ().

5.2 Derivation

Consider a slab of semiconductor:

  • Current flows in X-direction ().
  • Magnetic field is in Z-direction ().
  • Lorentz Force deflects carriers to the Y-direction.
  1. Magnetic Force (): Deflects carriers.
    (magnitude)
  2. Electric Force (): Accumulation of charge creates an internal electric field ().
  3. Equilibrium: Charges accumulate until electric force balances magnetic force.

  4. Current Density Relation:
  5. Hall Field:
  6. Hall Coefficient (): Defined as .

Final Hall Voltage Formula:
If is the width of the specimen ():


(Where is thickness).

A 3D block diagram illustrating the Hall Effect. A rectangular slab of conductive material. Show an ...
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5.3 Applications

  • Determination of semiconductor type (N-type is negative; P-type is positive).
  • Calculation of carrier concentration ().
  • Calculation of carrier mobility ().

6. Solar Cell Basics

6.1 Principle

A solar cell (photovoltaic cell) is a P-N junction diode that converts light energy (photons) directly into electrical energy. It operates on the Photovoltaic Effect.

6.2 Working Mechanism

  1. P-N Junction: A junction is formed between P-type and N-type silicon. A depletion region forms with an internal electric field.
  2. Photon Absorption: When light with energy strikes the junction, photons are absorbed.
  3. Carrier Generation: The energy breaks bonds, generating Electron-Hole Pairs (EHPs).
  4. Separation: The internal electric field in the depletion region sweeps electrons toward the N-side and holes toward the P-side.
  5. Collection: This charge accumulation creates a potential difference (Open Circuit Voltage, ). If an external load is connected, current flows (Short Circuit Current, ).

6.3 I-V Characteristics

The solar cell operates in the fourth quadrant of the I-V characteristic curve (power is delivered, not consumed).

  • (Open Circuit Voltage): Voltage when current is zero.
  • (Short Circuit Current): Current when voltage is zero.
  • Fill Factor (FF): A measure of the squareness of the I-V curve, indicating efficiency.

A cross-sectional diagram of a Solar Cell. The diagram shows layers from top to bottom: 1) Anti-refl...
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