Semiconductor Physics

🧗‍♀️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.

Key Concepts and Definitions

  • 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 (vdv_d) proportional to electric field (EE) and carrier mobility (μ\mu): vd=μEv_d = \mu E
    • 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 (JJ) proportional to the diffusion coefficient (DD) and concentration gradient (n\nabla n): J=qDnJ = -qD\nabla n
    • Einstein relation connects diffusion coefficient and mobility: D/μ=kBT/qD/\mu = k_BT/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\sigma) a measure of a material's ability to conduct electric current, determined by carrier concentrations (nn, pp) and mobilities (μn\mu_n, μp\mu_p): σ=q(nμn+pμp)\sigma = q(n\mu_n + p\mu_p)
  • 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


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AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.
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