💡Optoelectronics Unit 2 – Fundamentals of Semiconductor Physics
Semiconductors are the backbone of modern electronics and optoelectronics. They possess unique electrical properties that allow precise control of current flow. This unit explores the fundamental physics behind semiconductors, including band theory, carrier transport, and doping.
Understanding semiconductor physics is crucial for developing advanced electronic and photonic devices. We'll cover key concepts like band gaps, carrier concentrations, and mobility, as well as important semiconductor junctions and their applications in optoelectronic devices like LEDs and solar cells.
Semiconductors materials with electrical conductivity between insulators and conductors, enabling control of current flow
Band theory describes the energy levels and bands available for electrons in a solid, crucial for understanding semiconductor properties
Valence band highest occupied energy band in a semiconductor at absolute zero temperature
Conduction band lowest unoccupied energy band, where electrons can move freely and contribute to electrical conductivity
Band gap energy difference between the top of the valence band and the bottom of the conduction band, determining electrical and optical properties
Direct band gap allows efficient absorption and emission of light (GaAs, InP)
Indirect band gap requires additional phonon interactions for optical transitions (Si, Ge)
Fermi level energy level with a 50% probability of being occupied by an electron at thermal equilibrium
Carrier concentration number of electrons in the conduction band or holes in the valence band per unit volume
Mobility measure of how quickly charge carriers can move through a semiconductor under an applied electric field
Atomic Structure and Band Theory
Semiconductors have a periodic crystal structure, with atoms arranged in a repeating lattice
Covalent bonding between atoms leads to the formation of energy bands, separated by forbidden energy gaps
The electronic configuration of the atoms determines the number of valence electrons available for bonding
Group IV elements (Si, Ge) have four valence electrons, forming a diamond cubic crystal structure
III-V compounds (GaAs, InP) have an average of four valence electrons per atom, forming a zincblende crystal structure
The overlap of atomic orbitals leads to the formation of bonding and antibonding states, which give rise to the valence and conduction bands
The periodicity of the crystal structure results in the formation of a reciprocal lattice and Brillouin zones, which describe the allowed wave vectors for electrons
The band structure of a semiconductor can be calculated using various methods, such as the tight-binding approximation or the pseudopotential method
The effective mass of charge carriers is determined by the curvature of the energy bands near the band edges
Types of Semiconductors
Intrinsic semiconductors pure semiconductors without any intentional doping, with equal numbers of electrons and holes
Electron and hole concentrations are determined by the band gap and temperature
Examples include undoped Si and Ge
Extrinsic semiconductors semiconductors with intentional doping to control the type and concentration of charge carriers
n-type semiconductors doped with donor impurities (group V elements), providing excess electrons in the conduction band
p-type semiconductors doped with acceptor impurities (group III elements), creating excess holes in the valence band
Direct band gap semiconductors have the conduction band minimum and valence band maximum at the same wave vector (k-value)
Examples include GaAs, InP, and GaN
Efficient absorption and emission of light, suitable for optoelectronic devices (LEDs, lasers)
Indirect band gap semiconductors have the conduction band minimum and valence band maximum at different wave vectors
Examples include Si and Ge
Optical transitions require phonon assistance, making them less efficient for light emission
Compound semiconductors formed by combining elements from different groups of the periodic table
III-V compounds (GaAs, InP) widely used in optoelectronics due to their direct band gaps and high electron mobility
II-VI compounds (CdTe, ZnSe) used in solar cells and detectors
Carrier Transport and Mobility
Carrier transport in semiconductors occurs through drift and diffusion mechanisms
Drift current flow of charge carriers due to an applied electric field
Electrons move opposite to the electric field, while holes move in the same direction
Drift velocity proportional to the electric field strength and mobility
Diffusion current flow of charge carriers due to a concentration gradient
Carriers move from regions of high concentration to regions of low concentration
Diffusion current density proportional to the concentration gradient and diffusion coefficient
Mobility characterizes the ease with which charge carriers can move through a semiconductor under an applied electric field
Electron mobility generally higher than hole mobility due to their smaller effective mass
Mobility depends on various scattering mechanisms (lattice vibrations, ionized impurities, defects)
Conductivity measure of a semiconductor's ability to conduct electrical current, determined by carrier concentrations and mobilities
The Hall effect used to measure the carrier concentration, mobility, and conductivity type (n or p) of a semiconductor
High-field effects, such as velocity saturation and impact ionization, can limit carrier transport at high electric fields
Doping and Impurities
Doping intentional introduction of impurities into a semiconductor to control its electrical properties
Donor impurities (group V elements) provide excess electrons to the conduction band, creating n-type semiconductors
Examples include phosphorus (P) and arsenic (As) in silicon
Donor energy levels located slightly below the conduction band edge
Acceptor impurities (group III elements) create excess holes in the valence band, forming p-type semiconductors
Examples include boron (B) and gallium (Ga) in silicon
Acceptor energy levels located slightly above the valence band edge
Doping concentration determines the carrier concentration and Fermi level position
Higher doping levels shift the Fermi level closer to the corresponding band edge
Heavily doped semiconductors have a high conductivity and exhibit metallic behavior
Compensation occurs when both donor and acceptor impurities are present, reducing the net carrier concentration
Unintentional impurities and defects can also affect the electrical properties of semiconductors
Deep-level traps introduce energy levels within the band gap, acting as recombination centers
Oxygen and carbon are common unintentional impurities in silicon
Ion implantation and diffusion are common techniques for introducing dopants into semiconductors
Selective doping allows the creation of regions with different conductivity types, essential for device fabrication
Semiconductor Junctions
Semiconductor junctions formed by bringing together regions with different doping types or concentrations
p-n junction created by joining p-type and n-type semiconductors
Diffusion of carriers across the junction creates a depletion region with a built-in electric field
The built-in potential barrier controls the flow of carriers across the junction
Forward bias reduces the potential barrier, allowing current to flow
Reverse bias increases the potential barrier, limiting current flow
Heterojunctions formed by joining semiconductors with different band gaps
Band alignment (type I, II, or III) determines the energy barrier for carriers
Heterojunctions used in various optoelectronic devices (LEDs, lasers, solar cells)
Schottky junction formed between a metal and a semiconductor
The difference in work functions creates a potential barrier, known as the Schottky barrier
Rectifying behavior allows current flow in one direction only
Ohmic contacts provide low-resistance, non-rectifying connections to semiconductors
Formed by heavily doping the semiconductor near the metal-semiconductor interface
Essential for efficient current injection and extraction in semiconductor devices
Junction capacitance arises from the charge storage in the depletion region
Varies with the applied voltage and doping concentrations
Plays a role in the high-frequency performance of semiconductor devices
Optical Properties of Semiconductors
Semiconductors interact with light through absorption, emission, and refraction processes
Absorption occurs when a photon excites an electron from the valence band to the conduction band
The absorption coefficient depends on the photon energy and the band structure
Direct band gap semiconductors have a higher absorption coefficient than indirect band gap materials
Emission of light occurs through radiative recombination of electrons and holes
Photoluminescence emission of light due to optical excitation
Electroluminescence emission of light due to electrical injection of carriers
Refractive index determines the speed of light in the semiconductor and the reflection at interfaces
Varies with the photon energy and can be described by the Kramers-Kronig relations
Refractive index contrast enables the confinement of light in optical waveguides and cavities
Excitons bound electron-hole pairs that can form in semiconductors with strong Coulomb interaction
Excitons have a lower energy than unbound electron-hole pairs and can contribute to optical transitions
Quantum confinement effects enhance the exciton binding energy in low-dimensional structures
Nonlinear optical effects, such as second-harmonic generation and two-photon absorption, can occur at high light intensities
Nonlinear susceptibility depends on the crystal symmetry and band structure
Nonlinear effects are exploited in various optoelectronic devices (modulators, switches, frequency converters)
Applications in Optoelectronics
Light-emitting diodes (LEDs) convert electrical energy into light through electroluminescence
Based on forward-biased p-n junctions or heterojunctions
Efficiency depends on the material's internal quantum efficiency and light extraction efficiency
Used in displays, lighting, and optical communication
Laser diodes generate coherent light through stimulated emission
Require a gain medium, optical feedback, and carrier confinement
Edge-emitting lasers and vertical-cavity surface-emitting lasers (VCSELs) are common configurations
Used in optical storage, fiber-optic communication, and material processing
Photodetectors convert light into electrical signals through photogeneration of carriers
p-n photodiodes, PIN photodiodes, and avalanche photodiodes (APDs) are common types
Responsivity, dark current, and bandwidth are key performance parameters
Used in cameras, optical receivers, and spectroscopy
Solar cells convert sunlight into electrical energy through the photovoltaic effect
Based on p-n junctions or heterojunctions with a large surface area
Efficiency depends on the absorption, carrier collection, and voltage generation
Single-junction and multi-junction solar cells are used in terrestrial and space applications
Optical modulators control the amplitude, phase, or polarization of light using electrical signals
Electro-absorption modulators based on the quantum-confined Stark effect
Electro-optic modulators exploit the change in refractive index with an applied electric field
Used in optical communication and signal processing
Integrated optoelectronic circuits combine multiple optoelectronic devices on a single chip