🧗♀️Semiconductor Physics Unit 2 – Energy Bands & Carrier Transport in Semiconductors
Energy bands and carrier transport are fundamental concepts in semiconductor physics. They explain how electrons behave in solid materials, determining electrical and optical properties. Understanding these principles is crucial for designing and optimizing electronic devices.
Semiconductors bridge the gap between insulators and conductors. By manipulating energy bands through doping and device structure, we can control carrier generation, recombination, and transport. This forms the basis for various applications, from simple diodes to complex integrated circuits and quantum devices.
Semiconductors materials with electrical conductivity between insulators and conductors, enabling control of current flow
Energy bands ranges of allowed energy states for electrons in a solid, formed by overlapping atomic orbitals
Valence band highest occupied energy band at absolute zero temperature, where electrons are bound to atoms
Conduction band lowest unoccupied energy band, where electrons can move freely and contribute to electrical conduction
Energy gap (bandgap) separates valence and conduction bands, determining electrical properties
Fermi level energy level with 50% probability of being occupied by an electron at thermodynamic equilibrium
Carriers charge carriers in semiconductors, including electrons (negative) and holes (positive)
Doping intentional introduction of impurities to modify electrical properties by altering band structure and carrier concentrations
n-type doping introduces excess electrons (pentavalent impurities like phosphorus)
p-type doping introduces excess holes (trivalent impurities like boron)
Energy Band Formation in Solids
Solid-state physics describes the formation of energy bands through the interaction of atomic orbitals
Isolated atoms have discrete energy levels, but in solids, these levels split and form continuous energy bands due to the periodic potential of the crystal lattice
Wave functions of electrons in neighboring atoms overlap, leading to the formation of bonding and antibonding orbitals
Bonding orbitals lower energy states occupied by valence electrons
Antibonding orbitals higher energy states that are usually unoccupied
Energy bands are separated by forbidden energy gaps (bandgaps) where no electron states exist
The width of energy bands and bandgaps depends on the strength of atomic interactions and the periodicity of the crystal structure
The electronic structure of a solid determines its electrical, optical, and thermal properties
The filling of energy bands follows the Pauli exclusion principle and Fermi-Dirac statistics
Types of Energy Bands in Semiconductors
Direct bandgap semiconductors have the conduction band minimum and valence band maximum at the same crystal momentum (k-value)
Examples: GaAs, InP, and CdTe
Enable efficient optical transitions and are used in optoelectronic devices (LEDs, lasers)
Indirect bandgap semiconductors have the conduction band minimum and valence band maximum at different crystal momenta
Examples: Si, Ge, and GaP
Optical transitions require phonon assistance, making them less efficient
The bandgap energy determines the wavelength of absorbed or emitted light and the intrinsic carrier concentration
Degenerate semiconductors have high doping levels, causing the Fermi level to lie within the conduction or valence band
Behave more like metals due to the high carrier concentration
Amorphous semiconductors lack long-range periodic order, resulting in localized states and a distribution of bandgap energies
Example: amorphous silicon (a-Si) used in thin-film solar cells and displays
Carrier Generation and Recombination
Carrier generation the process of creating electron-hole pairs in a semiconductor
Thermal generation dominates at room temperature, with electrons excited across the bandgap by absorbing thermal energy
Optical generation occurs when electrons absorb photons with energy greater than the bandgap
Carrier recombination the process of eliminating electron-hole pairs, with electrons relaxing from the conduction band to the valence band
Radiative recombination releases energy as photons and is dominant in direct bandgap semiconductors
Non-radiative recombination releases energy as phonons (lattice vibrations) and is dominant in indirect bandgap semiconductors
Shockley-Read-Hall (SRH) recombination occurs through defect states within the bandgap
Auger recombination involves three-particle interactions, becoming significant at high carrier concentrations
Generation and recombination rates determine the carrier lifetime and affect device performance
Minority carrier lifetime the average time before a minority carrier (electron in p-type, hole in n-type) recombines
Photovoltaic devices (solar cells) aim to maximize carrier lifetime for efficient charge collection
Light-emitting devices (LEDs) aim to maximize radiative recombination for high quantum efficiency
Carrier Transport Mechanisms
Drift the movement of carriers under the influence of an electric field
Drift velocity (vd) proportional to electric field (E) and carrier mobility (μ): vd=μE
Electron mobility typically higher than hole mobility due to lower effective mass
Diffusion the movement of carriers from regions of high concentration to low concentration, driven by concentration gradients
Diffusion current density (J) proportional to the diffusion coefficient (D) and concentration gradient (∇n): J=−qD∇n
Einstein relation connects diffusion coefficient and mobility: D/μ=kBT/q
Carrier mobility a measure of how easily carriers move through a semiconductor under an electric field
Affected by scattering mechanisms: lattice vibrations (phonons), ionized impurities, and defects
Temperature dependence: mobility decreases with increasing temperature due to enhanced phonon scattering
Conductivity (σ) a measure of a material's ability to conduct electric current, determined by carrier concentrations (n, p) and mobilities (μn, μp): σ=q(nμn+pμp)
Current-voltage (I-V) characteristics of semiconductor devices depend on carrier transport mechanisms and device structure
Ohmic contacts have linear I-V characteristics and low resistance
Rectifying contacts (p-n junctions) have nonlinear I-V characteristics and enable current flow in one direction
Doping and Its Effects on Band Structure
Doping introduces impurities into a semiconductor to modify its electrical properties
n-type doping (donor impurities) adds electrons to the conduction band, increasing conductivity
Examples: phosphorus, arsenic, and antimony in silicon
p-type doping (acceptor impurities) adds holes to the valence band, increasing conductivity
Examples: boron, aluminum, and gallium in silicon
Doping shifts the Fermi level towards the conduction band (n-type) or valence band (p-type)
Ionization energy the energy required to ionize dopant atoms and contribute carriers to the bands
Dopant activation the fraction of dopant atoms that are ionized at a given temperature
Heavy doping can lead to the formation of impurity bands, narrow energy bands associated with dopant states
Impurity bands can overlap with the conduction or valence band, leading to metallic behavior
Compensation the presence of both donor and acceptor impurities, reducing the effective doping concentration
Modulation doping a technique to spatially separate dopants from the conducting channel, reducing ionized impurity scattering and enhancing mobility
Used in high-electron-mobility transistors (HEMTs) and quantum well structures
Semiconductor Device Applications
p-n junctions the foundation of many semiconductor devices, formed by joining p-type and n-type regions
Diodes allow current flow in one direction (forward bias) and block it in the reverse direction
Solar cells convert light into electrical energy by separating photogenerated carriers
Light-emitting diodes (LEDs) emit light through electroluminescence when forward biased
Bipolar junction transistors (BJTs) three-terminal devices with emitter, base, and collector regions
Amplify current and are used in analog circuits and high-power applications
Field-effect transistors (FETs) three-terminal devices that use electric fields to control current flow
Metal-oxide-semiconductor FETs (MOSFETs) have an insulated gate and are the building blocks of modern electronics
Junction FETs (JFETs) have a reverse-biased p-n junction as the gate and are used in low-noise amplifiers
Optoelectronic devices convert between electrical and optical signals
Photodetectors (photodiodes, phototransistors) convert light into electrical current
Laser diodes emit coherent light through stimulated emission in a resonant cavity
Power devices handle high voltages and currents in power electronics applications
Thyristors (SCRs, TRIACs) are four-layer (pnpn) devices used for switching and power control
Power MOSFETs and IGBTs (insulated-gate bipolar transistors) are used in high-efficiency power converters
Advanced Topics and Current Research
Quantum confinement effects arise when the size of a semiconductor structure approaches the de Broglie wavelength of carriers
Quantum wells, wires, and dots exhibit discrete energy levels and modified optical properties
Enables the development of quantum cascade lasers, quantum dot displays, and single-photon sources
Spintronics exploits the spin degree of freedom of electrons in addition to their charge
Spin-based devices (spin valves, spin transistors) offer low power consumption and non-volatility
Topological insulators have conducting surface states protected by time-reversal symmetry, promising for spintronic applications
Wide and ultrawide bandgap semiconductors (GaN, SiC, Ga2O3, diamond) have bandgaps larger than 3 eV
Enable high-power, high-frequency, and high-temperature electronics for power grids, electric vehicles, and 5G networks
Organic and perovskite semiconductors offer low-cost, flexible, and solution-processable alternatives to inorganic semiconductors
Organic light-emitting diodes (OLEDs) are used in displays and solid-state lighting
Perovskite solar cells have achieved power conversion efficiencies over 25% in a short time
Neuromorphic computing aims to emulate the energy efficiency and parallel processing of biological neural networks
Memristors and phase-change memory devices can act as artificial synapses and neurons
Enables brain-inspired computing for AI, machine learning, and edge computing applications