Fundamentals of Quantum Physics Study Notes
Course Overview
Course Name: Fundamentals of Quantum Physics
Course Code: TEE7244
Course Credit: 3+1
Instructors: Prof. (Dr.) Meena Laad & Dr. Kuldeep Mishra
Unit 3: Semiconductors
Duration: 09 Lectures
Key Topics:
Intrinsic and extrinsic semiconductors
Dependence of Fermi level on carrier concentration and temperature (equilibrium carrier statistics)
Carrier generation and recombination
Carrier transport
Hall effect
Hall effect sensor
Magnetic field detection
Magnetic switching
Properties of Semiconductors
Semiconductors:
Definition: A solid material with electrical conductivity between a conductor and an insulator.
Applications: used as optical detectors, light-emitting diodes (LEDs), lasers, amplifiers, waveguides, modulators, sensors, and nonlinear optical elements.
Behavior at Temperature: Materials that are semiconductors at room temperature behave as perfect insulators at absolute zero (0 K).
Energy Bands at Room Temperature: 25 eV - represents the energy absorbed by an electron when subjected to a 1 V potential difference at room temperature.
Charge Carriers in Semiconductors
Types of Charge Carriers: Electrons and holes.
At Absolute Zero (T = 0 K):
Valence Band (VB) is completely filled.
Conduction Band (CB) is completely empty.
Result: The material does not conduct electricity.
As Temperature Increases:
Some electrons are thermally excited into the empty Conduction Band, forming a free electron in CB and a free hole in VB.
Definition: An empty state in the VB is referred to as a hole; the excitation of a VB electron to the CB creates an electron-hole pair (EHP).
Intrinsic Semiconductor
Definition: A perfect semiconductor crystal with no impurities or lattice defects.
At T = 0 K:
No charge carriers are present.
VB filled with electrons, CB empty.
At T > 0 K:
Electron-hole pairs (EHPs) are generated.
EHPs serve as the only charge carriers in intrinsic materials.
Relationship: The electron concentration in the conduction band (n) equals the concentration of holes in the valence band (p), both denoted as intrinsic carrier concentration (ni).
Equation:
n = p = n_i
Characteristics of Intrinsic Semiconductors
Concentration of EHPs (ni): At any given temperature, there is a certain concentration of EHPs ni.
Recombination Rate (ri):
EHPs recombine at the same rate they are generated.
Recombination occurs when an electron makes a transition to an empty state in the valence band, thereby annihilating the pair.
Equilibrium condition:
ri = gi
where g_i is the generation rate of EHPs.Rates are temperature dependent.
Temperature Influence: As temperature increases, the generation rate gi increases, establishing a new carrier concentration ni where the higher recombination rate ri balances it.
Mathematical Relation:
Rate of recombination of electrons and holes:
ri = \alphar n0 p0 = \alphar ni^2 = gi where \alphar is a constant of proportionality depending on the recombination mechanism.
Conductivity and Temperature
Effect of Temperature:
As temperature increases, the number of free electrons and holes generated grows exponentially, affecting semiconductor conductivity.
Carrier Concentration vs Temperature Example (Silicon) at Different Temperatures:
( ext{Temperature (K)}): 150, 200, 250, 300, 350, 400, 450, 500
( ext{Intrinsic Concentration (cm}^{-3} ext{)}): 1E3, 1E17, 1E10, … 1E17
Carrier Density in Intrinsic Semiconductor
Mathematical Expression for Carrier Density:
ni^2 = \frac{Ne e^{(Ec - EF)/kT}}{N1 e^{(EF - E_v)/kT}}
Where:
N_c: Effective density of states in CB
N_v: Effective density of states in VB
E_c: Conduction Band edge
E_v: Valence Band edge
E_F: Fermi energy level
k: Boltzmann constant
T: Absolute temperature
Effective Density of States for Silicon:
At Room Temperature:
N_c = 2.8 imes 10^{25} ext{ m}^{-3}
N_v = 1.0 imes 10^{25} ext{ m}^{-3}
Example of Charge Carrier Concentration
Example Problem:
Given Eg = 1.1 eV. Calculate the carrier concentrations at 300 K, taking effective masses as 0.27 m0 for holes and 0.13 m0 for electrons.
Doping in Semiconductors
Purpose of Doping:
To increase the number of charge carriers (electrons or holes) in a semiconductor material and modify its electrical properties.
Process:
Mixing pure semiconductors with impurities (dopants).
Can introduce additional charge carriers (donors or acceptors).
Types of Doped Semiconductors:
n-type: Predominantly contains electrons (donor impurities such as Phosphorus, Arsenic).
p-type: Predominantly contains holes (acceptor impurities such as Boron, Aluminum).
Doping Elements Characteristics
Group V Elements (n-type dopants):
Elements like Phosphorus, Antimony introduce additional electrons.
Group III Elements (p-type dopants):
Elements like Boron and Aluminum create holes in the valence band.
Doping and Conductivity Changes
Effects of Temperature on Doping:
Conductivity can vary widely with temperature in doped semiconductors.
Summary of Doping Impacts:
Doping enhances the concentration of mobile charge carriers significantly, thus increasing conductivity.
Doping Ionization Energy
Ionization Energy for Donor and Acceptor Levels:
Ionization energies for common dopants at room temperature are remarkably low (order of 0.01 - 0.06 eV).
Fermi Level in Semiconductors
Fermi Level Position:
The position of the Fermi level is crucial for determining the conductivity type.
In n-type: Fermi level is closer to the conduction band.
In p-type: Fermi level is closer to the valence band.
Carrier Transport Phenomena
Drift Current Definition: The current due to charge carriers moving in response to the applied electric field.
Current defined as:
J = \sigma EWhere:
J: Current density (A/m²)
\sigma: Conductivity (S/m)
E: Electric field strength (V/m)
Diffusion Current Definition: The current resulting from the movement of charge carriers from regions of high concentration to low concentration.
Governed by Fick's laws:
J_D = -D \nabla n
Where D is the diffusion coefficient.
Hall Effect
Definition: The voltage created across a conductor when an electric current flows through it in a magnetic field.
Governed by the Lorentz force, given by:
F = q[E + (v \times B)]
Applications of Hall Effect:
Used to determine semiconductor type, carrier concentration, measurement of magnetic fields.
Hall Sensor Technology
Types of Hall Sensors:
Automotive, Industrial, and Consumer applications, including digital switches and automotive functions.
Example Problem: Calculate the current density in an n-type semiconductor under an electric field using given parameters.
Example Calculations: Show calculations for determining J, based on the current density formula and provided doping parameters.
Conclusion
Key Takeaways:
Understanding semiconductors, doping mechanisms, and their applications is foundational for electronic device design.
The interplay between temperature, carrier concentration, and external fields shapes the behavior of semiconductor materials.