Semiconductor
Written by Gemini 4 Argon from Google Search
Contents
A semiconductor is a material whose electrical conductivity lies between that of an electrical conductor, such as copper, and that of an insulator, such as glass.1 Unlike metals, whose electrical resistance increases as they grow hotter, semiconductors become more conductive as temperature rises.23 Because their conductivity can be altered by orders of magnitude through the precise introduction of chemical impurities—a process known as doping—or by the application of electric fields, heat, or light, semiconductors serve as the physical foundation for nearly all modern electronics.4
In colloquial and economic usage, the term also refers to the electronic components fabricated from these materials, including diodes, transistors, photovoltaic cells, and integrated circuits (microchips).5 While pure elements from Group 14 of the periodic table, particularly silicon and germanium, defined the early decades of solid-state electronics, compound semiconductors such as gallium arsenide, silicon carbide, and gallium nitride have become indispensable for optoelectronics, radio-frequency communications, and high-voltage power conversion.67
The mastery of semiconductor physics and fabrication drove the transition from vacuum-tube machinery to the digital information age.89 By the mid-2020s, global semiconductor sales approached $800 billion annually, propelled by demand for artificial intelligence data centers, consumer computing, telecommunications, and electric vehicles, making the highly concentrated semiconductor supply chain a focal point of international trade policy and environmental scrutiny.101112
Physical principles
The distinctive electrical behavior of a semiconductor arises from its atomic crystal lattice and the quantum-mechanical arrangement of its electrons into energy bands.1314 In any solid crystalline material, electrons are restricted to specific ranges of energy.15 The highest energy range that is completely filled with electrons at absolute zero temperature is called the valence band, where electrons remain bound to individual atoms within covalent bonds. Above the valence band lies the conduction band, where electrons are detached from their parent atoms and can move freely through the crystal lattice to carry an electric current.
The energy difference separating the top of the valence band from the bottom of the conduction band is known as the band gap. In conductors like metals, the valence and conduction bands overlap, allowing electrons to flow effortlessly. In insulators, the band gap is wide—typically several electron volts (eV)—preventing thermal energy at room temperature from exciting electrons across the divide. Semiconductors possess a moderate band gap, such as 1.12 eV in silicon or 1.42 eV in gallium arsenide at room temperature. When thermal energy or incident photons with energy exceeding the band gap strike an intrinsic (pure) semiconductor, electrons jump from the valence band into the conduction band.16 Each excited electron leaves behind a vacant state in the valence band called an electron hole.17 Neighboring valence electrons can shift into this vacancy, causing the hole itself to migrate through the lattice as if it were a positively charged particle.
Doping and junctions
Because intrinsic semiconductors have relatively few free charge carriers at room temperature, device manufacturing relies on extrinsic semiconductors modified through doping. Doping introduces a trace fraction of impurity atoms—often on the order of one dopant atom per 100 million host atoms—into the crystal lattice to establish a dominant type of charge carrier. When a Group 14 element like silicon, which has four valence electrons, is doped with a pentavalent Group 15 element such as phosphorus, arsenic, or antimony, four of the dopant's electrons form covalent bonds with surrounding silicon atoms while the fifth electron remains loosely bound. This introduces a donor energy level just below the conduction band, allowing the extra electrons to enter the conduction band easily and creating an n-type (negative-type) semiconductor. Conversely, doping silicon with a trivalent Group 13 element such as boron, gallium, or indium leaves one bond short of an electron, introducing an acceptor level just above the valence band. Electrons from the valence band readily fill these states, generating mobile positive holes and creating a p-type (positive-type) semiconductor.
When a single crystal is doped so that an n-type region and a p-type region meet, the interface forms a p-n junction. Near the boundary, excess electrons from the n-type side diffuse into the p-type side and recombine with holes, while holes diffuse in the opposite direction. This diffusion strips mobile carriers from the immediate interface, leaving behind fixed, charged dopant ions that establish a non-conducting space-charge region, or depletion zone, with a built-in electric field. Applying an external voltage in the forward direction narrows this depletion zone and permits substantial current to flow, whereas applying voltage in the reverse direction widens the barrier and blocks current.18 This rectifying behavior is the operating mechanism of diodes, light-emitting diodes (LEDs), solar cells, and transistors.
Materials
Semiconductor materials are broadly categorized into elemental semiconductors, composed of a single species of atom, and compound semiconductors, synthesized from two or more elements across different groups of the periodic table.19 Historically, researchers refer to elemental germanium and silicon as first-generation materials, direct-bandgap III-V compounds as second-generation materials, and wide-bandgap compounds as third-generation materials.
Germanium was the primary material used for the earliest diodes and transistors during the late 1940s and early 1950s because it has a lower melting point (937 °C) than silicon and was easier to refine to high purity.2021 However, germanium devices exhibit high leakage currents in the off state and cease functioning reliably above 70 °C. Once chemical refinement techniques improved in the mid-1950s, silicon supplanted germanium and came to account for more than 95 percent of all semiconductor devices manufactured globally. Silicon operates across a much wider temperature range (-55 °C to 125 °C), is the second-most abundant element in Earth's crust in the form of silica, and naturally grows a chemically stable insulating layer of silicon dioxide () on its surface when heated in oxygen—an attribute crucial for planar circuit fabrication.2223
Compound semiconductors address the physical limitations of silicon. Gallium arsenide (GaAs) and indium phosphide (InP), formed from Group 13 and Group 15 elements, possess electron mobilities up to six times higher than that of silicon, allowing transistors to switch at microwave and millimeter-wave frequencies used in satellite communications, radar, and cellular base stations. Furthermore, unlike silicon's indirect band gap, GaAs and InP feature a direct band gap, meaning electrons can transition directly from the conduction band to the valence band and emit energy as photons without requiring lattice vibrations (phonons) to conserve momentum. This property makes direct-bandgap compounds essential for laser diodes, fiber-optic transceivers, and high-efficiency space photovoltaics.24
A growing segment of the industry relies on wide-bandgap semiconductors, principally silicon carbide (SiC) and gallium nitride (GaN), whose band gaps exceed 3 eV. Silicon carbide has a band gap of approximately 3.2 eV, a thermal conductivity three times that of silicon, and a breakdown electric field strength ten times higher. These characteristics allow SiC metal-oxide-semiconductor field-effect transistors (MOSFETs) to handle voltages of 1,200 V to 1,700 V with minimal energy loss, making them the standard in electric-vehicle traction inverters, fast-charging stations, and photovoltaic grid converters.252627 Gallium nitride excels in high-frequency switching and mid-voltage power conversion (typically around 600 V) as well as solid-state LED lighting. Researchers are also developing ultra-wide-bandgap materials, including gallium oxide and synthetic diamond, which offers five times the thermal conductivity of SiC for extreme-temperature aerospace and defense electronics.
History
Scientific observation of semiconducting behavior predates atomic theory. Although Alessandro Volta used the term "semiconducting" as early as 1782, the first documented experimental finding occurred in 1833, when English physicist Michael Faraday reported that the electrical resistance of silver sulfide decreased when heated, contrary to the behavior of metallic conductors. In 1873, English engineer Willoughby Smith discovered photoconductivity after observing that light lowered the electrical resistance of selenium. Three years later, William Grylls Adams and Richard Evans Day found that illuminating a junction of selenium and platinum generated an electric current, demonstrating the photovoltaic effect and enabling American inventor Charles Fritts to construct the first rudimentary selenium solar cell in 1883. Meanwhile, in 1874, German physicist Karl Ferdinand Braun observed that pressing a thin metal wire against metallic sulfide crystals allowed current to pass in only one direction. This point-contact rectification became the basis of "cat's-whisker" crystal radio detectors in the early twentieth century.
The word "semiconductor" (German: Halbleiter) was introduced in its modern context by Josef Koenigsberger and Jakob Weiss in 1911. Theoretical understanding remained incomplete until the formulation of quantum mechanics in the late 1920s. In 1929, German physicist Walter Schottky confirmed the existence of potential barriers at metal-semiconductor junctions, and in 1931 British physicist Alan Herries Wilson published The Theory of Electronic Semiconductors, applying quantum band theory to explain conduction, insulation, and the role of impurities. In 1940, American physicist Russell Ohl at Bell Laboratories stumbled upon the p-n junction while examining a cracked sample of purified silicon that produced a voltage when exposed to a flashlight.
Transistors and integrated circuits
Seeking a solid-state replacement for fragile, power-hungry vacuum tubes in telephone switching networks, Bell Laboratories established a solid-state physics group led by William Shockley.28 In December 1947, Bell Labs physicists John Bardeen and Walter Brattain constructed the first working point-contact transistor by pressing two closely spaced gold foil contacts against a crystal of germanium, demonstrating signal amplification. Shockley followed in 1948 with the theoretical design of the more durable bipolar junction transistor, which Gordon Teal and Morgan Sparks first fabricated from single-crystal germanium in April 1950.29 Shockley, Bardeen, and Brattain shared the 1956 Nobel Prize in Physics for their work.
The shift from germanium to silicon occurred in 1954. On January 26, 1954, Bell Labs physical chemist Morris Tanenbaum demonstrated the first working silicon transistor using high-purity silicon supplied by DuPont, though Bell Labs declined to commercialize his rate-grown design.30 Working independently at Texas Instruments, Gordon Teal and chemist Willis Adcock fabricated a grown-junction silicon transistor on April 14, 1954, and stunned the industry on May 10 by announcing commercial production at an Institute of Radio Engineers conference in Dayton, Ohio. In 1955, Carl Frosch and Lincoln Derick at Bell Labs discovered that a layer of silicon dioxide could mask and passivate a silicon wafer's surface. Building on this oxide-passivation principle, Egyptian-born engineer Mohamed Atalla and Korean-born engineer Dawon Kahng invented the metal-oxide-semiconductor field-effect transistor (MOSFET) at Bell Labs in 1959–1960, creating the scalable transistor structure that came to dominate electronics.31
As electronic systems grew more complex, soldering thousands of discrete transistors together created a reliability bottleneck known as the "tyranny of numbers". In 1958, engineer Jack Kilby at Texas Instruments demonstrated the first integrated circuit (IC) by fabricating a transistor, capacitor, and resistor on a single bar of germanium connected by fine gold wires. Months later, in 1959, Robert Noyce at Fairchild Semiconductor invented the monolithic integrated circuit in silicon, utilizing Jean Hoerni's planar process to deposit interconnected aluminum wiring directly over an insulating silicon dioxide layer. Integrated circuits drove rapid miniaturization—described by Fairchild co-founder Gordon Moore's 1965 observation ("Moore's Law") that component density on a chip roughly doubled every 18 to 24 months—and culminated in Intel's release of the first commercial single-chip microprocessor, the 4004, in 1971.
Device fabrication
Modern semiconductor manufacturing transforms raw mineral quartz into wafers packed with billions of nanoscale devices through hundreds of sequential chemical, optical, and thermal steps conducted inside ultra-clean facilities known as foundries or "fabs".3233 The process begins by reducing quartzite sand () with carbon in a furnace at roughly 1,800 °C to produce metallurgical-grade silicon of about 98 percent purity.34 This crude silicon is chemically converted into liquid trichlorosilane gas, distilled, and redeposited as electronic-grade polycrystalline silicon (polysilicon) reaching a purity of 99.9999999 percent—commonly called "nine nines"—or higher.35
To form the continuous crystal lattice required for electronic devices, polysilicon is melted inside a high-purity quartz crucible at temperatures just above silicon's melting point of 1,414 °C via the Czochralski process.36 A precisely oriented single-crystal seed mounted on a rod is dipped into the molten silicon and slowly withdrawn while rotating. The liquid solidifies around the seed into a cylindrical single-crystal ingot, or boule, which is then sliced by diamond wire saws into thin circular discs called wafers, lapped flat, chemically etched, and polished to a mirror finish.
Inside the fabrication plant, the polished wafer undergoes repeated cycles of deposition, photolithography, etching, and doping. First, an insulating oxide film or conductive layer is grown or deposited on the wafer surface. The wafer is then coated with a light-sensitive chemical called photoresist. During photolithography, a specialized scanner projects ultraviolet light through a patterned template, or photomask, onto the photoresist, transferring the geometric layout of a circuit layer.37 Exposed regions of the resist are dissolved away, and reactive plasma gases or wet chemicals etch the underlying exposed material.38 Ion implantation machines then fire accelerated beams of dopant ions into designated regions of the silicon, followed by thermal annealing to repair the crystal lattice.
For the most advanced logic and memory chips—such as 3-nanometer (nm) and 2 nm process nodes—chipmakers rely on extreme ultraviolet (EUV) lithography machines produced exclusively by the Dutch manufacturer ASML.3940 An EUV system fires a high-powered laser at falling droplets of molten tin 50,000 times per second inside a vacuum chamber, creating a plasma that emits light at a wavelength of 13.5 nanometers, which is focused onto the wafer by atomically smooth reflective mirrors.
Global industry and applications
Semiconductors are divided commercially into four major product categories: logic chips (including central processing units, graphics processing units, and application-specific processors), memory chips (such as volatile Dynamic Random-Access Memory and non-volatile NAND flash), analog integrated circuits (which translate continuous real-world signals like sound, temperature, and power into digital data), and optoelectronics, sensors, and discrete components.4142
Driven by the rapid build-out of artificial intelligence (AI) data centers, cloud infrastructure, and vehicle electrification, global semiconductor industry revenues expanded by 25.6 percent in 2025 to reach $791.7 billion, up from $630.5 billion in 2024, according to the Semiconductor Industry Association (SIA) and World Semiconductor Trade Statistics (WSTS). Monthly global sales reached $82.5 billion in January 2026, putting the industry on pace to approach $1 trillion in annual revenue. Demand for accelerated AI computing has reshaped market shares: companies specializing in AI logic processors, such as Nvidia, and high-bandwidth memory (HBM) manufacturers, including SK Hynix, Samsung Electronics, and Micron Technology, recorded the steepest revenue gains in 2025 and 2026, even creating memory allocation shortages for traditional personal computer and smartphone makers. Meanwhile, the automotive semiconductor segment is projected to nearly double from $68 billion in 2024 to $132 billion by 2030 as automakers adopt electric drivetrains and advanced driver-assistance systems.
The industry operates through a specialized global division of labor. "Fabless" design companies—such as Nvidia, Apple, Qualcomm, and AMD—design integrated circuit architectures using electronic design automation software but own no manufacturing plants. They contract fabrication out to pure-play foundries, led by Taiwan Semiconductor Manufacturing Company (TSMC), which entered volume production of its 2 nm nanosheet (gate-all-around) transistor process in late 2025.43 Integrated device manufacturers (IDMs) such as Intel, Samsung Electronics, and Texas Instruments both design and manufacture chips, while specialized vendors supply lithography equipment, silicon wafers, and outsourced assembly and testing.
In 2026, leading-edge manufacturers diverged in their adoption of next-generation High Numerical Aperture (High-NA) EUV lithography—machines costing roughly $370 million each that shift the optical numerical aperture from 0.33 to 0.55 to print features at an 8 nm resolution. Intel Foundry pioneered High-NA EUV in high-volume production on selected layers of its 18A process node for Core Ultra Series 3 ("Panther Lake") processors in 2026. Conversely, Samsung committed to deploying High-NA EUV for DRAM production by 2028, while TSMC opted to manufacture its 2 nm and subsequent generations with conventional EUV, deferring High-NA volume production until 2030 alongside a joint industry initiative to transition from 6-inch to 12-inch photomasks by 2033.44
Geopolitics and environmental impact
Because over 50 percent of global semiconductor revenue is concentrated in the Asia-Pacific region—with advanced logic fabrication heavily centered in Taiwan and memory fabrication in South Korea—governments in North America, Europe, and Asia treat semiconductor supply chains as matters of national security.45 Following pandemic-era chip shortages and escalating technological competition, the United States and the Netherlands instituted export controls restricting the sale of advanced AI processors and EUV lithography systems to China. Simultaneously, governments launched major industrial subsidy programs, such as the U.S. CHIPS and Science Act and India's Semicon India program, to incentivize domestic wafer fabrication.
The physical supply chain also remains vulnerable to geographic bottlenecks and climate shocks. In September 2024, Hurricane Helene temporarily halted mining operations in Spruce Pine, North Carolina, a single locality that supplies roughly 70 percent of the world's ultra-high-purity quartz required to manufacture the crucibles used in Czochralski silicon ingot pulling. Furthermore, a 2024 World Economic Forum analysis noted that 40 percent of existing semiconductor fabs and 40 percent of facilities announced since 2021 are located in watersheds projected to face high or extremely high water stress between 2030 and 2040.
Chip fabrication is resource-intensive, requiring vast quantities of ultrapure water to rinse wafers between hundreds of chemical steps, as well as substantial electrical energy to run cleanroom climate controls and lithography tools. Manufacturing processes also rely on hundreds of per- and polyfluoroalkyl substances (PFAS)—synthetic compounds with strong carbon-fluorine bonds used in photoresists, anti-reflective coatings, and etching fluids because they withstand harsh chemical and thermal conditions.4647 Because PFAS persist in the environment and have been linked to adverse human health outcomes, wastewater discharges from expanding fabrication plants have drawn regulatory scrutiny in Europe and the United States. While semiconductor trade groups argue that immediate bans could disrupt global electronics production due to a lack of qualified drop-in chemical substitutes, environmental researchers estimate that global expenditures to treat and remove PFAS from semiconductor and electronics wastewater could reach $16.5 billion to $50 billion annually by 2035.48
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