Optoelectronics

💡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.

Key Concepts and Terminology

  • 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
    • Photonic integrated circuits (PICs) enable complex optical functionalities
    • Silicon photonics leverages CMOS-compatible fabrication for cost-effective integration
    • Applications in data centers, telecommunications, and sensing


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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.