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Ga0.2Al0.8P

semiconductor

Ga₀.₂Al₀.₈P is a III-V semiconductor alloy combining gallium phosphide and aluminum phosphide in a 20:80 molar ratio, belonging to the direct-bandgap compound semiconductor family. This material is primarily investigated for optoelectronic and high-frequency electronic applications where the aluminum content increases bandgap energy and lattice constant tunability compared to pure GaP. The alloy is notable in research contexts for UV-to-visible light emission, high-temperature device operation, and integrated photonic circuits, though commercial deployment remains limited compared to GaAs or GaN alternatives.

ultraviolet LEDshigh-temperature electronicsintegrated photonics
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Ga0.2In0.8As

semiconductor

Ga₀.₂In₀.₈As is a ternary III-V compound semiconductor alloy composed of gallium, indium, and arsenic, engineered to achieve a direct bandgap in the near-infrared region. It is primarily used in optoelectronic and high-speed electronic devices where its lattice-matched or near-lattice-matched properties with InP substrates enable efficient epitaxial growth; notably employed in photodetectors, laser diodes, and integrated photonic circuits for telecommunications and sensing applications. This alloy is valued for its superior electron mobility and direct bandgap characteristics compared to binary alternatives, making it particularly relevant for long-wavelength infrared detection and high-frequency analog/mixed-signal integrated circuits.

infrared photodetectorsfiber-optic communicationshigh-speed integrated circuits
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Ga0.3As0.3Zn0.7Se0.7

semiconductor

Ga₀.₃As₀.₃Zn₀.₇Se₀.₇ is a quaternary III-V semiconductor alloy combining gallium arsenide and zinc selenide constituents, engineered to achieve intermediate bandgap and lattice properties between its parent compounds. This research material is primarily investigated for optoelectronic applications where tunable energy bandgap and direct band-to-band transitions are required, particularly in the visible to near-infrared spectrum. The composition represents an experimental exploration of ternary and quaternary semiconductor space rather than an established commercial material, with potential relevance to developers of photonic devices, photodetectors, and light-emitting systems seeking alternatives to GaAs or ZnSe alone.

optoelectronic researchphotonic devicesphotodetectors
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Ga0.3P0.3Zn0.7Se0.7

semiconductor

Ga0.3P0.3Zn0.7Se0.7 is a quaternary II-VI semiconductor alloy combining gallium phosphide and zinc selenide in a mixed-cation, mixed-anion structure. This is a research-stage compound designed to engineer the bandgap and lattice parameters for optoelectronic applications by blending the constituent binary semiconductors. The material belongs to the family of tunable wide-bandgap semiconductors that bridge traditional optoelectronic materials, offering potential for UV-to-visible photonic devices where bandgap engineering and lattice matching are critical.

UV photodetectorsvisible light LEDslaser diodes
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Ga0.4Al0.6As

semiconductor

Ga₀.₄Al₀.₆As is a III-V semiconductor alloy combining gallium arsenide and aluminum arsenide in a 40:60 ratio, engineered to tune the bandgap and lattice properties between pure GaAs and AlAs. This material is used in optoelectronic and high-frequency devices where direct bandgap control is critical, particularly in heterojunction structures for laser diodes, photodetectors, and high-electron-mobility transistors (HEMTs); the aluminum content increases bandgap energy and reduces lattice mismatch compared to GaAs alone, making it valuable for quantum well layers and lattice-matched heterostructures on GaAs substrates. The alloy enables engineers to balance optical transparency, carrier confinement, and thermal stability in integrated photonic and RF circuits where precision bandgap engineering is essential.

semiconductor heterostructuresquantum well lasershigh-electron-mobility transistors (HEMTs)
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Ga0.4Al0.6P

semiconductor

Ga₀.₄Al₀.₆P is a direct-bandgap III-V compound semiconductor alloy that combines gallium phosphide and aluminum phosphide in a 40:60 molar ratio. This material is engineered for optoelectronic and high-frequency electronic applications where the bandgap energy and lattice properties of the GaP–AlP system offer advantages over binary compounds. It appears primarily in research and specialized industrial contexts for visible and near-infrared light emission, high-power RF devices, and heterostructure layers in advanced semiconductor devices.

LED emitters (red-green spectral range)High-electron-mobility transistors (HEMT)Laser diode heterostructures
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Ga0.4As0.4Zn0.6Se0.6

semiconductor

Ga₀.₄As₀.₄Zn₀.₆Se₀.₆ is a quaternary II-VI semiconductor alloy combining gallium arsenide and zinc selenide constituents, designed to engineer the bandgap and lattice properties for optoelectronic applications. This material is primarily a research-phase compound explored for tunable optoelectronic devices where bandgap engineering between visible and infrared wavelengths is critical; it competes with more established ternary alloys (like ZnSe or GaAs) by offering composition flexibility to match specific emission wavelengths or detector response requirements. The mixed cation-anion structure makes it particularly relevant for next-generation light-emitting devices, photodetectors, and laser applications where precise wavelength control and lattice matching to substrates is necessary.

optoelectronic bandgap engineeringvisible and near-IR light emittersphotodetectors and sensors
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Ga0.58As0.58Zn0.42Se0.42

semiconductor

Ga₀.₅₈As₀.₅₈Zn₀.₄₂Se₀.₄₂ is a quaternary III-V semiconductor alloy combining gallium arsenide with zinc selenide, engineered to achieve specific bandgap and lattice properties for optoelectronic applications. This compound exists primarily in research and specialized manufacturing contexts, where tuning the GaAs/ZnSe composition ratio enables optimization for light emission, detection, or high-frequency electronic devices across the visible to near-infrared spectrum. Engineers select quaternary alloys like this when binary or ternary semiconductors cannot simultaneously meet lattice-matching, bandgap energy, and thermal stability requirements—making it relevant for advanced photonics, quantum devices, and specialized RF/microwave circuits.

optoelectronic devicesquantum well structureslight-emitting diodes (LEDs)
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Ga0.5Al0.5As

semiconductor

Ga₀.₅Al₀.₅As is a III-V compound semiconductor alloy formed by combining gallium arsenide (GaAs) and aluminum arsenide (AlAs) in a 50/50 molar ratio. This direct bandgap material is engineered to achieve intermediate electronic and optical properties between its constituent binaries, making it valuable for optoelectronic and high-frequency devices where precise bandgap control is critical. The 50% aluminum composition positions this alloy in the range commonly used for lattice-matched heterostructures on GaAs substrates, enabling the fabrication of quantum wells, laser active regions, and high-electron-mobility transistors (HEMTs) with well-defined band offsets.

semiconductor lasers and LEDshigh-electron-mobility transistors (HEMTs)quantum well structures
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Ga0.5As0.5Zn0.5Se0.5

semiconductor

Ga₀.₅As₀.₅Zn₀.₅Se₀.₅ is a quaternary compound semiconductor formed by alloying gallium arsenide (GaAs) with zinc selenide (ZnSe), combining elements from Groups II-VI and III-V semiconductor families. This material is primarily of research and developmental interest for optoelectronic applications where bandgap engineering and lattice matching are critical; it represents an experimental composition rather than an established commercial material, but the GaAs/ZnSe alloy family shows promise for tunable emission wavelengths and potential photovoltaic or detector applications.

optoelectronic researchbandgap engineeringphotovoltaic development
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Ga0.5In0.5As

semiconductor

Ga₀.₅In₀.₅As is a lattice-matched III-V semiconductor alloy combining gallium arsenide and indium arsenide in equal proportions, engineered to achieve a bandgap and lattice constant intermediate between its constituent binaries. This material is primarily used in high-speed optoelectronic and RF devices, particularly in heterojunction structures for infrared detectors, high-electron-mobility transistors (HEMTs), and integrated photonic circuits where lattice matching to InP substrates is critical for device performance and yield.

infrared photodetectorshigh-electron-mobility transistors (HEMTs)millimeter-wave RF circuits
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Ga0.5P0.5Zn0.5Se0.5

semiconductor

Ga₀.₅P₀.₅Zn₀.₅Se₀.₅ is a quaternary semiconductor compound formed by alloying gallium phosphide with zinc selenide in equal proportions, creating a mixed crystal structure with tunable electronic properties. This is primarily a research and development material rather than a mature commercial compound, explored for its potential to bridge the bandgap range between established III-V semiconductors (like GaP) and II-VI semiconductors (like ZnSe), making it relevant for optoelectronic device engineering where specific wavelength or bandgap tuning is needed. Engineers would evaluate this material in contexts where conventional binary or ternary semiconductors cannot achieve the required bandgap, luminescence, or carrier transport properties, though material quality and reproducibility remain active research challenges.

optoelectronic deviceslight-emitting diodes (experimental)bandgap engineering
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Ga0.65Al0.35As

semiconductor

Ga₀.₆₅Al₀.₃₅As is a III-V direct bandgap semiconductor alloy combining gallium arsenide and aluminum arsenide, engineered to deliver a wider bandgap than pure GaAs while maintaining good lattice matching for heterostructure devices. This material is primarily used in optoelectronic and high-frequency applications where its tunable bandgap enables efficient light emission and detection, and its superior electron transport properties support faster, lower-noise operation compared to silicon-based alternatives.

laser diodes and LEDshigh-speed integrated circuitsheterojunction bipolar transistors
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Ga0.6Al0.4P

semiconductor

Ga₀.₆Al₀.₄P is a III-V semiconductor alloy combining gallium phosphide and aluminum phosphide in a 60:40 ratio, forming a direct bandgap material in the visible-to-near-infrared spectrum. This compound is primarily used in optoelectronic devices, particularly red and orange light-emitting diodes (LEDs) and laser diodes, where its tunable bandgap and lattice properties enable efficient photon emission. Compared to pure GaP, the aluminum incorporation increases the bandgap energy, shifting emission wavelength and improving performance in display and signaling applications where precise color control is required.

red/orange LEDsdisplay backlightingoptical signaling
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Ga0.6In0.4As

semiconductor

Ga₀.₆In₀.₄As is a III-V semiconductor alloy combining gallium arsenide and indium arsenide in a 60:40 ratio, engineered to achieve an intermediate bandgap energy between its parent compounds. This material is used primarily in high-speed optoelectronic and photonic integrated circuits, particularly for infrared photodetectors, heterojunction bipolar transistors (HBTs), and quantum well devices operating in the near-to-mid infrared wavelength ranges. Its lattice-matched or near-lattice-matched properties with GaAs and InP substrates make it valuable for epitaxial growth in monolithic integrated circuits, offering superior performance over bulk InAs or GaAs alone in applications demanding both high electron mobility and wavelength tunability.

infrared photodetectorsoptoelectronic integrated circuitshigh-speed transistors
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Ga0.75As0.75Zn0.25Se0.25

semiconductor

Ga0.75As0.75Zn0.25Se0.25 is a quaternary III-V semiconductor alloy combining gallium arsenide with zinc selenide components, engineered to tune the bandgap and lattice parameters for optoelectronic applications. This material belongs to the wide-bandgap semiconductor family and is primarily of research and development interest for tunable light-emitting devices, photodetectors, and high-efficiency optoelectronic systems where bandgap engineering enables wavelength customization across the visible and near-infrared spectrum. The zinc and selenium additions to the GaAs base provide lattice-matching flexibility and bandgap control that make this composition attractive for heterostructure devices where conventional binary or ternary compounds fall short.

optoelectronic heterostructurestunable light-emitting devicesinfrared photodetectors
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Ga0.75P0.75Zn0.25Se0.25

semiconductor

Ga₀.₇₅P₀.₇₅Zn₀.₂₅Se₀.₂₅ is a quaternary III-V semiconductor alloy combining gallium phosphide, gallium arsenide family elements with zinc and selenium dopants, designed to engineer the bandgap and electronic properties for optoelectronic applications. This is primarily a research-phase material used to explore direct bandgap semiconductors with tunable wavelength performance; the zinc and selenium substitution into the GaP lattice allows precision control of optical and electrical characteristics compared to binary or ternary compounds. The material is notable in the context of experimental photovoltaic devices, light-emitting structures, and photodetectors where bandgap engineering is critical for matching specific wavelengths or improving conversion efficiency.

experimental optoelectronicsbandgap engineeringphotovoltaic research
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Ga0.7Al0.3As

semiconductor

Ga₀.₇Al₀.₃As is a III-V compound semiconductor alloy formed by combining gallium arsenide and aluminum arsenide in a 70:30 ratio. This direct bandgap material is engineered to deliver intermediate electronic and optical properties between its binary components, making it valuable for optoelectronic and high-frequency applications where bandgap tuning is critical. The aluminum content increases bandgap energy and lattice strain compared to pure GaAs, enabling optimization for specific wavelength ranges in the near-infrared spectrum and higher operational temperatures in devices requiring thermal stability.

laser diodes and LEDshigh-electron-mobility transistors (HEMTs)optoelectronic integrated circuits
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Ga0.7In0.3As

semiconductor

Ga₀.₇In₀.₃As is a ternary III-V semiconductor alloy combining gallium arsenide and indium arsenide, engineered to achieve a specific bandgap and lattice parameter intermediate between its binary constituents. This material is primarily used in optoelectronic and high-frequency electronic devices, particularly in infrared photodetectors, laser diodes, and high electron mobility transistors (HEMTs) where its tailored bandgap enables detection or emission in the near-to-mid infrared spectrum. The 70/30 Ga/In ratio is selected for lattice compatibility with common substrates and to optimize carrier transport properties, making it preferred over binary compounds when a specific wavelength range or monolithic integration is required.

infrared photodetectorslaser diodes and emittershigh-frequency transistors (HEMT)
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Ga0.85Al0.15As

semiconductor

Ga₀.₈₅Al₀.₁₅As is a direct-bandgap III-V semiconductor alloy combining gallium arsenide with aluminum arsenide in a 85:15 molar ratio. This material is engineered for optoelectronic applications where the aluminum composition tunes the bandgap to intermediate wavelengths, balancing emission wavelength, carrier confinement, and lattice matching with GaAs substrates. It is widely used in high-brightness light-emitting diodes (LEDs), laser diodes, and integrated photonic circuits, where it offers superior performance over bulk GaAs in the red-to-infrared spectrum and serves as a lattice-matched window layer in heterostructure devices.

High-brightness LEDs (red spectrum)Laser diode heterostructuresOptoelectronic integrated circuits
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Ga0.85As0.85Zn0.15Se0.15

semiconductor

Ga0.85As0.85Zn0.15Se0.15 is a quaternary III-V semiconductor alloy combining gallium arsenide with zinc selenide constituents, representing a research-level material engineered to tune the bandgap and lattice parameters of traditional GaAs. This compound is primarily explored in photonic and optoelectronic applications where precise control over band structure is needed, such as in wide-bandgap device engineering and specialized light-emitting or light-detecting systems. The zinc and selenium incorporation allows researchers to shift electronic and optical properties relative to binary GaAs, making it relevant for next-generation semiconductor devices that demand custom spectral responses or improved performance in niche operating conditions.

optoelectronic semiconductorsphotonic device engineeringbandgap-tuned light emitters
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Ga0.8Al0.2P

semiconductor

Ga₀.₈Al₀.₂P is a direct-bandgap III-V semiconductor alloy composed of gallium phosphide and aluminum phosphide, positioned between pure GaP and AlP in the compositional phase space. This material is used primarily in optoelectronic devices, particularly red and amber light-emitting diodes (LEDs) and infrared detectors, where its bandgap energy and direct transition characteristics enable efficient photon emission. The aluminum content raises the bandgap relative to pure GaP, shifting emission toward shorter wavelengths and improving lattice matching with certain substrates; this composition exemplifies the tunable bandgap strategy central to III-V semiconductor engineering.

Red and amber LEDsInfrared optoelectronicsLight-emitting devices
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Ga0.8In0.2As

semiconductor

Ga₀.₈In₀.₂As is a ternary III-V semiconductor alloy composed primarily of gallium arsenide with 20% indium substitution, designed to tune the bandgap and lattice parameters for optoelectronic applications. This material is used in high-speed photodetectors, infrared emitters, and integrated photonic circuits where its intermediate bandgap and lattice characteristics between GaAs and InAs enable efficient operation in the near-infrared spectrum. The indium addition is selected to balance lattice matching with substrates, achieve specific emission wavelengths, or improve carrier transport compared to binary GaAs, making it valuable for telecommunications and sensing systems.

infrared photodetectorsoptoelectronic integrated circuitshigh-speed photoreceivers
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Ga0.8Sb0.8Cd0.2Te0.2

semiconductor

Ga₀.₈Sb₀.₈Cd₀.₂Te₀.₂ is a quaternary III-V semiconductor alloy combining gallium antimonide with cadmium telluride constituents, designed to engineer the bandgap and lattice properties for infrared applications. This experimental material targets the mid-to-long wavelength infrared detection range, where it offers potential advantages over binary compounds through compositional tuning of electronic and thermal properties. The alloy family is primarily of research interest for advanced infrared sensors, thermal imaging, and space-based detection systems where bandgap engineering and temperature performance are critical.

infrared detectorsthermal imaging sensorsspace instrumentation
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Ga0.8Sb0.8Zn0.2Te0.2

semiconductor

Ga0.8Sb0.8Zn0.2Te0.2 is a quaternary III-V semiconductor alloy combining gallium antimonide and zinc telluride constituents, engineered to tune bandgap and lattice properties for optoelectronic and thermal applications. This is primarily a research and development material used to explore intermediate bandgap semiconductors and thermoelectric devices where conventional binary compounds (GaSb, ZnTe) cannot achieve the required performance envelope. The quaternary composition allows precise control of electronic structure for infrared detectors, mid-IR LEDs, and solid-state cooling applications where bandgap engineering and thermal transport optimization are critical.

infrared detectorsmid-IR optoelectronicsthermoelectric cooling
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Ga0.95Hg0.05Sb0.95Te0.05

semiconductor

Ga0.95Hg0.05Sb0.95Te0.05 is a narrow-bandgap III-V semiconductor alloy based on gallium antimonide (GaSb) with mercury and tellurium additions, designed to operate in the infrared spectral region. This ternary/quaternary compound is primarily of research and specialized commercial interest for infrared detection and thermal imaging applications where tuned bandgap engineering enables response in specific wavelength windows. The mercury and tellurium dopants modify the electronic structure relative to binary GaSb, making this alloy relevant for applications requiring sensitivity in the mid-wave or long-wave infrared bands where traditional silicon detectors are insensitive.

infrared detectorsthermal imaging sensorsnight vision systems
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Ga0.95Sb0.95Cd0.05Te0.05

semiconductor

Ga₀.₉₅Sb₀.₉₅Cd₀.₀₅Te₀.₀₅ is a quaternary III-V semiconductor alloy based on the GaSb-CdTe system, combining gallium antimonide with cadmium telluride dopants to modify bandgap and lattice parameters. This is a specialized research-phase compound designed for infrared detection and sensing applications, where the controlled addition of cadmium and tellurium shifts the material's optical properties into the mid-wave infrared (MWIR) band relative to binary GaSb. Engineers would consider this alloy when developing high-sensitivity thermal imaging detectors, night-vision focal plane arrays, or space-based infrared spectroscopy systems where bandgap engineering and lattice matching to substrate materials are critical—though it remains largely confined to advanced research and specialized defense/aerospace applications rather than high-volume production.

infrared detectorsthermal imaging focal plane arraysMWIR sensing
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Ga0.95Sb0.95Hg0.05Te0.05

semiconductor

Ga0.95Sb0.95Hg0.05Te0.05 is a quaternary III-V semiconductor alloy combining gallium antimonide with small additions of mercury and tellurium, designed to engineer the bandgap and lattice parameters for infrared optoelectronic applications. This material belongs to the mercury-containing narrow-bandgap semiconductor family and is primarily investigated for mid-wave and long-wave infrared detectors and emitters operating at cryogenic to moderate temperatures. The mercury and tellurium dopants reduce the effective bandgap compared to GaSb, making this composition relevant for thermal imaging, military surveillance systems, and scientific instrumentation where sensitivity to longer infrared wavelengths is critical.

infrared detectorsthermal imaging sensorsmilitary surveillance optics
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Ga0.95Sb0.95Zn0.05Te0.05

semiconductor

Ga0.95Sb0.95Zn0.05Te0.05 is a quaternary III-V semiconductor alloy based on gallium antimonide with small additions of zinc and tellurium dopants, engineered to modify electronic and optical properties for specialized device applications. This material belongs to the GaSb family—a narrow-bandgap semiconductor platform widely used in infrared optoelectronics—with zinc and tellurium additions tuning carrier concentration and band structure for specific detector or emitter designs. The composition sits at the research/development stage rather than mature production, targeting applications where conventional GaSb or related alloys require property refinement for mid-to-long-wavelength infrared sensing or high-speed electronic devices.

infrared detectorsthermal imaging sensorshigh-speed optoelectronic devices
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Ga0.99Al0.01P

semiconductor

Ga₀.₉₉Al₀.₀₁P is a III-V direct bandgap semiconductor alloy—a gallium phosphide (GaP) lattice with minimal aluminum doping—used primarily in optoelectronic devices where efficient light emission and detection are required. This material is commonly found in red and infrared LEDs, solar cells, and integrated photonic applications where its direct bandgap and lattice compatibility with GaP substrates enable reliable performance. The small aluminum fraction allows fine-tuning of the bandgap energy relative to pure GaP, making it valuable for wavelength engineering in lighting and sensing systems where conventional silicon cannot operate efficiently.

red and infrared LEDsphotovoltaic devicesintegrated photonics
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Ga0.99As0.99Zn0.01Se0.01

semiconductor

Ga₀.₉₉As₀.₉₉Zn₀.₀₁Se₀.₀₁ is a quaternary III-V compound semiconductor alloy based on gallium arsenide, with small substitutions of zinc and selenium dopants that modify its electronic and optical properties. This is primarily a research-stage material rather than a widely commercialized compound; it belongs to the GaAs family but the specific dopant combination is explored for tuning bandgap energy, carrier concentration, and optical emission characteristics for specialized optoelectronic devices. The material would appeal to researchers and engineers developing next-generation photodetectors, light-emitting devices, or solar cells where fine control of bandgap and minority-carrier lifetime is critical, though production volumes and standardized supply chains remain limited compared to standard GaAs or InGaAs variants.

optoelectronic research devicesIII-V semiconductors and solar cellsbandgap engineering and tuning
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Ga0.99Hg0.01Sb0.99Te0.01

semiconductor

Ga0.99Hg0.01Sb0.99Te0.01 is a quaternary III-V semiconductor alloy based on the GaSb-GaTe system with minor mercury doping, designed to engineer the band gap and lattice parameters for infrared optoelectronic applications. This material family is primarily explored in research contexts for tuning electronic and optical properties in the mid- to long-wavelength infrared range, where it competes with established systems like HgCdTe and InSb for thermal imaging, gas sensing, and space-based spectroscopy. The precise compositional control offers potential advantages in lattice matching and thermal stability compared to binary or simpler ternary alternatives, making it relevant for next-generation infrared detectors and emitters where band gap engineering is critical.

infrared detectorsthermal imaging sensorsmid-wave infrared (MWIR) optoelectronics
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Ga0.99In0.01As

semiconductor

Ga₀.₉₉In₀.₀₁As is a III-V semiconductor alloy consisting of gallium arsenide (GaAs) with 1% indium doping, forming a direct bandgap material with a bandgap near that of pure GaAs. This composition is used primarily in optoelectronic and high-frequency electronic devices where the slight indium addition provides lattice matching flexibility and modest bandgap tuning compared to undoped GaAs, enabling integration with other III-V compounds and improved device performance in specific wavelength ranges.

infrared optoelectronicshigh-speed transistorsintegrated photonics
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Ga0.99P0.99Zn0.01Se0.01

semiconductor

Ga0.99P0.99Zn0.01Se0.01 is a quaternary III-V semiconductor alloy based on gallium phosphide with small additions of zinc and selenium dopants, designed to modify the electronic and optical properties of the base GaP compound. This material is primarily of research interest for optoelectronic and photovoltaic applications where band gap engineering and defect compensation are desired; zinc acts as an acceptor dopant while selenium substitution can tune lattice parameters and optical response. The material represents experimental work in tuning wide-band-gap semiconductors for improved efficiency in LEDs, solar cells, or radiation detectors compared to undoped GaP.

optoelectronic devicessemiconductor researchband gap engineering
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Ga0.99Sb0.99Cd0.01Te0.01

semiconductor

Ga0.99Sb0.99Cd0.01Te0.01 is a quaternary III-V semiconductor alloy based on gallium antimonide (GaSb) with small additions of cadmium and tellurium. This composition represents a research material designed to engineer the bandgap and lattice parameters of the GaSb binary compound, primarily for infrared optoelectronic applications where precise control of optical properties is needed. The cadmium and tellurium dopants modify the electronic structure compared to baseline GaSb, making this material attractive for tuning performance in mid-infrared to long-wavelength infrared (LWIR) detector systems and potentially for thermoelectric or thermal imaging device optimization.

infrared detectors and sensorsthermal imaging systemsbandgap engineering research
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Ga0.99Sb0.99Hg0.01Te0.01

semiconductor

Ga0.99Sb0.99Hg0.01Te0.01 is a quaternary III-V semiconductor alloy based on gallium antimonide with minor mercury telluride additions. This material is primarily of research interest for infrared detection and thermal imaging applications, where the incorporated mercury and tellurium modify the bandgap to extend sensitivity into the mid- to long-wave infrared spectrum compared to conventional GaSb. The small dopant concentrations allow precise tuning of optoelectronic properties while maintaining the stability and processing advantages of the GaSb host lattice.

infrared detectorsthermal imaging sensorsresearch/experimental compound
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Ga0.99Sb0.99Zn0.01Te0.01

semiconductor

Ga0.99Sb0.99Zn0.01Te0.01 is a quaternary III-V semiconductor alloy based on gallium antimonide with small additions of zinc and tellurium dopants. This is a research-phase material designed to modify the electronic and thermal properties of GaSb for specialized optoelectronic and infrared detector applications. The zinc and tellurium dopants are typically introduced to tune bandgap, carrier concentration, or lattice properties, making this alloy relevant for mid-infrared sensing, thermal imaging, or high-temperature semiconductor device development where standard binary or ternary GaSb may not meet performance targets.

infrared detectorsthermal imaging sensorsoptoelectronic devices
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Ga0.9Hg0.1Sb0.9Te0.1

semiconductor

Ga0.9Hg0.1Sb0.9Te0.1 is a quaternary III-V semiconductor alloy combining gallium antimonide (GaSb) and mercury telluride (HgTe) components, engineered to achieve specific bandgap and lattice properties intermediate between its parent compounds. This is a research-focused material rather than a widely commercialized alloy, developed primarily for infrared detector and optoelectronic applications where precise control of the narrow bandgap is required. The material's HgTe content confers semimetal-like electronic properties, making it particularly relevant for long-wavelength infrared sensing and narrow-gap device engineering, though it requires careful thermal and compositional management compared to more stable binary or ternary alternatives.

infrared detectorslong-wavelength IR opticsnarrow-bandgap semiconductors
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Ga0.9Sb0.9Cd0.1Te0.1

semiconductor

Ga₀.₉Sb₀.₉Cd₀.₁Te₀.₁ is a quaternary III-V semiconductor alloy combining gallium antimonide (GaSb) with cadmium telluride (CdTe) dopants, engineered to tune bandgap and carrier properties for infrared and thermal sensing applications. This is a research-phase material composition designed to optimize performance in mid-to-long-wavelength infrared detection where traditional binary GaSb or CdTe alone may fall short; the dual alloying strategy allows independent control of lattice constant and electronic structure to improve detector sensitivity, reduce noise, and extend operating temperature range compared to single-component alternatives.

infrared detectorsthermal imaging sensorsmilitary surveillance systems
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Ga0.9Sb0.9Hg0.1Te0.1

semiconductor

Ga0.9Sb0.9Hg0.1Te0.1 is a quaternary III-V semiconductor alloy combining gallium antimonide with mercury telluride dopants, designed to engineer the bandgap and carrier transport properties for infrared and thermal applications. This material belongs to the HgCdTe family of narrow-bandgap semiconductors and is primarily investigated for mid- to long-wave infrared detection, where its tunable bandgap enables sensitivity across specific thermal windows. Engineers select this composition when standard GaSb or HgTe prove insufficient for wavelength specificity or when the mercury and tellurium additions offer improved thermal stability or detector responsivity compared to binary alternatives.

infrared photodetectorsthermal imaging sensorsmilitary/defense surveillance
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Ga0.9Sb0.9Zn0.1Te0.1

semiconductor

Ga0.9Sb0.9Zn0.1Te0.1 is a quaternary III-V semiconductor alloy combining gallium antimonide (GaSb) with zinc telluride (ZnTe) dopants, designed to tune the bandgap and carrier properties of the GaSb host material. This is a research-grade compound rather than a widely commercialized material, developed to explore intermediate bandgap semiconductors and improve optoelectronic or thermoelectric performance in specific wavelength or temperature regimes where pure GaSb is suboptimal.

infrared photodetectorsnarrow-bandgap semiconductorsthermoelectric devices
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Ga1

semiconductor

Ga1 is a gallium-based semiconductor material, likely a gallium arsenide (GaAs) or gallium nitride (GaN) compound or derivative, used in optoelectronic and high-frequency applications. It is employed in integrated circuits, photodetectors, light-emitting devices, and RF/microwave components where direct bandgap properties and high electron mobility offer advantages over silicon. The material is valued in aerospace, telecommunications, and photovoltaic industries for its superior performance at high frequencies and in high-temperature environments compared to conventional semiconductors.

optoelectronic devicesRF/microwave circuitshigh-frequency amplifiers
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Ga1.001Sb0.999Se0.003

semiconductor

Ga₁.₀₀₁Sb₀.₉₉₉Se₀.₀₀₃ is a III-V semiconductor alloy based on gallium antimonide with trace selenium doping, representing a deliberate compositional engineering of the GaSb binary system. This material is primarily of research and development interest for infrared (IR) optoelectronic applications, where the selenium incorporation modulates bandgap and electronic properties compared to undoped GaSb. The near-unity stoichiometry with minimal Se content suggests optimization for mid-to-long-wavelength IR detection or emission in specialized photonic devices, where precise alloy tuning enables performance advantages over conventional GaSb or more complex quaternary systems.

infrared detectorsthermal imaging sensorsmid-IR optoelectronics
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Ga1.001Sb0.999Te0.003

semiconductor

Ga₁.₀₀₁Sb₀.₉₉₉Te₀.₀₀₃ is a III-V semiconductor alloy based on gallium antimonide with trace tellurium doping, representing a precisely engineered variant of the GaSb family. This material is primarily of research and specialized device interest, where the small tellurium incorporation is used to tune bandgap, carrier concentration, or lattice properties for infrared detection, thermal imaging sensors, or next-generation photovoltaic applications. The near-stoichiometric GaSb backbone combined with controlled Te incorporation makes it relevant in contexts requiring narrow-bandgap semiconductors with tailored carrier dynamics—applications where fine compositional control delivers performance advantages over standard binary GaSb.

infrared detectorsthermal imaging sensorsnarrow-bandgap photovoltaics
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Ga1.002Sb0.998Se0.006

semiconductor

Ga₁.₀₀₂Sb₀.₉₉₈Se₀.₀₀₆ is a III-V semiconductor alloy based on gallium antimonide (GaSb) with a small selenium dopant, engineered to tune bandgap and carrier properties for infrared and optoelectronic applications. This composition sits in the research/development space rather than high-volume production, targeting infrared detectors, thermal imaging systems, and mid-wavelength infrared (MWIR) sensors where GaSb substrates and near-stoichiometric variants are desirable for sensitivity and thermal stability. The selenium incorporation modifies lattice parameters and defect behavior compared to binary GaSb, making it relevant for specialized detector systems and heterojunction devices where precise bandgap engineering is critical.

infrared detectorsthermal imaging sensorsmid-wavelength IR (MWIR) devices
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Ga1.002Sb0.998Te0.006

semiconductor

Ga₁.₀₀₂Sb₀.₉₉₈Te₀.₀₀₆ is a III-V semiconductor alloy based on gallium antimonide (GaSb) with trace tellurium doping, designed to engineer the bandgap and carrier properties for infrared and thermal detection applications. This near-stoichiometric composition represents a research-grade material optimized for mid-to-long wavelength infrared (MWIR/LWIR) sensing, where the tellurium incorporation provides defect compensation and improved carrier mobility compared to undoped GaSb. The material is used primarily in photodetector arrays, thermal imaging sensors, and military/space-based infrared systems where sensitivity in the 3–5 μm and 8–12 μm atmospheric windows is critical.

infrared photodetectorsthermal imaging sensorsMWIR/LWIR detection
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Ga1.005Sb0.995Se0.015

semiconductor

Ga1.005Sb0.995Se0.015 is a III-V semiconductor alloy based on gallium antimonide (GaSb) with a small selenium dopant addition. This material belongs to the narrow-bandgap semiconductor family and is primarily a research compound designed to tune electronic and optical properties for specialized infrared and optoelectronic applications.

infrared detectorsthermal imaging sensorsmid-infrared optoelectronics
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Ga1.005Sb0.995Te0.015

semiconductor

Ga₁.₀₀₅Sb₀.₉₉₅Te₀.₀₁₅ is a ternary III-V semiconductor alloy based on gallium antimonide (GaSb) with a small tellurium dopant addition, designed to engineer the bandgap and carrier properties of the GaSb system. This composition falls within the research and development space for infrared optoelectronics and thermal management applications, where the tellurium incorporation modifies lattice properties and electronic structure compared to undoped GaSb. The material is notable for potential use in tuning detector sensitivity and thermal emission characteristics in the mid- to long-wavelength infrared region, making it relevant to applications requiring custom bandgap engineering beyond standard binary or well-established quaternary compounds.

infrared detectorsthermal imaging sensorsbandgap engineering
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Ga1.01Cu0.99Se2.01

semiconductor

Ga₁.₀₁Cu₀.₉₉Se₂.₀₁ is a quaternary semiconductor compound based on the copper gallium diselenide (CuGaSe₂) family, with near-stoichiometric composition and slight gallium enrichment. This material belongs to the chalcopyrite semiconductor class and is primarily investigated for photovoltaic and optoelectronic applications, where it offers tunable bandgap and potential for thin-film solar cells and photodetectors. While not yet widely commercialized compared to established alternatives like CdTe or CIGS absorbers, this composition is of research interest for its stability, defect-tolerance properties, and compatibility with scalable deposition methods in emerging photovoltaic technology.

thin-film solar cellsphotodetectorsoptoelectronic devices
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Ga1.01Sb0.99Se0.03

semiconductor

Ga₁.₀₁Sb₀.₉₉Se₀.₀₃ is a III-V compound semiconductor alloy based on gallium antimonide with selenium doping, engineered to modify bandgap and electronic properties for infrared and optoelectronic applications. This is a research-phase material composition, part of the GaSb family which is valued for mid-to-long-wavelength infrared detection and emission where materials like InSb and HgCdTe are used; the selenium incorporation fine-tunes performance for specific wavelength windows and carrier transport characteristics. Engineers would consider this alloy where customized bandgap control, thermal stability, or detector sensitivity in the infrared spectrum is critical, though it remains primarily in development rather than high-volume production.

infrared detectors and sensorsoptoelectronic devicesthermal imaging
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Ga1.01Sb0.99Te0.03

semiconductor

Ga₁.₀₁Sb₀.₉₉Te₀.₀₃ is a III-V compound semiconductor alloy based on gallium antimonide (GaSb) with minor tellurium doping, belonging to the narrow-bandgap semiconductor family. This material is primarily studied for infrared optoelectronic applications, particularly in the mid-infrared to far-infrared spectral range where the tellurium addition fine-tunes the bandgap. The near-stoichiometric gallium-to-antimony ratio with controlled tellurium incorporation makes it relevant for thermoelectric devices, infrared detectors, and laser applications where precise band structure engineering is required; it represents an experimental or specialized composition rather than a widely commercialized alloy.

infrared photodetectorsthermoelectric devicesmid-infrared emitters/lasers
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Ga1.02Sb0.98Se0.06

semiconductor

Ga1.02Sb0.98Se0.06 is a III-V semiconductor alloy based on gallium antimonide with selenium doping, representing a narrow-bandgap compound semiconductor system. This material belongs to the gallium antimonide family and is primarily investigated for infrared optoelectronic applications where its bandgap and carrier mobility characteristics enable detection and emission in the mid-to-long wavelength infrared spectrum. The selenium incorporation modifies the electronic structure compared to binary GaSb, making it suitable for specialized sensing and thermal imaging systems where sensitivity in specific infrared windows is required.

infrared photodetectorsthermal imaging sensorsmid-wave infrared (MWIR) applications
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Ga1.02Sb0.98Te0.06

semiconductor

Ga₁.₀₂Sb₀.₉₈Te₀.₀₆ is a III-V semiconductor alloy based on gallium antimonide with minor tellurium doping, belonging to the family of narrow-bandgap semiconductors used in infrared and thermal imaging applications. This material is primarily of research and development interest for mid-infrared to far-infrared photodetectors and thermal sensing devices, where its narrow bandgap enables detection of longer wavelengths than conventional semiconductors. The tellurium addition modulates the electronic properties and bandgap of the GaSb host, making it relevant for tuning detector sensitivity in specialized imaging and spectroscopy systems where GaSb alone may not provide optimal performance.

infrared photodetectorsthermal imaging sensorsspectroscopy applications
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Ga1.05Sb0.95Se0.15

semiconductor

Ga₁.₀₅Sb₀.₉₅Se₀.₁₅ is a ternary III-V semiconductor alloy combining gallium antimonide with selenium incorporation, designed to engineer the bandgap and carrier transport properties for infrared and optoelectronic applications. This composition falls within the gallium antimonide family—a mature semiconductor system used for infrared detectors and thermal imaging—but the selenium substitution is a research-level modification to tailor electronic and optical characteristics for specific wavelength ranges or device performance targets. The slight gallium over-stoichiometry (Ga₁.₀₅ vs. Ga₁.₀) and selenium alloying suggest optimization for narrow-bandgap infrared detection or thermal sensing devices where precise bandgap engineering is critical.

infrared photodetectorsthermal imaging sensorsnarrow-bandgap optoelectronics
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Ga1.05Sb0.95Te0.15

semiconductor

Ga₁.₀₅Sb₀.₉₅Te₀.₁₅ is a III-V compound semiconductor alloy based on gallium antimonide with tellurium doping, engineered to modify the bandgap and carrier properties of the base GaSb material. This quaternary or pseudo-ternary composition falls within the narrow-bandgap semiconductor family, with tellurium incorporation typically serving to tune electronic properties for infrared and thermal imaging applications. The composition sits in an experimental or specialized research domain rather than mainstream production; such Te-doped GaSb variants are investigated primarily for infrared detectors, thermoelectric devices, and high-mobility transistor channels where lattice-matched epitaxy and low-temperature carrier transport are critical.

infrared detectors and thermal imagingthermoelectric cooling/power generationhigh-mobility transistors
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Ga1.1Cu0.9Se2.1

semiconductor

Ga₁.₁Cu₀.₉Se₂.₁ is a quaternary semiconductor compound based on the copper gallium diselenide (CuGaSe₂) family, with slight copper deficiency and gallium excess. This material exists primarily in research and development contexts as a candidate for thin-film photovoltaic absorbers, where non-stoichiometry is intentionally engineered to modify electronic properties and crystal defect characteristics. Compared to the stoichiometric CuGaSe₂ baseline, composition-tuned variants like this one are investigated to improve photoelectric efficiency, reduce recombination losses, and enhance device stability in solar cells.

thin-film solar cellsphotovoltaic absorber layersdirect bandgap semiconductors
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Ga11 N1 O15

semiconductorGa11 N1 O15

Ga₁₁N₁O₁₅ is an experimental gallium nitride-based oxide compound that belongs to the family of wide-bandgap semiconductors. This material is primarily of research interest for advanced optoelectronic and high-temperature semiconductor applications, as gallium nitride systems are known for high breakdown fields and thermal stability. The oxide phase composition suggests potential use in developing transparent conductive oxides, high-k dielectrics, or novel heterostructure interfaces, though this specific stoichiometry remains in early-stage investigation rather than established industrial production.

wide-bandgap semiconductor researchhigh-temperature electronicstransparent conductive oxides
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Ga1.1Sb0.9Se0.3

semiconductor

Ga₁.₁Sb₀.₉Se₀.₃ is a quaternary III-V semiconductor alloy combining gallium antimonide (GaSb) with selenium doping or alloying. This composition sits in the infrared detector and thermal imaging material space, representing an experimental or specialized research compound rather than a commodity semiconductor. The material is investigated for mid-infrared and thermal detection applications where its bandgap and carrier properties offer potential advantages over binary GaSb or related alternatives like InSb.

infrared detectorsthermal imaging sensorsmid-infrared photodetectors
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Ga1.1Sb0.9Te0.3

semiconductor

Ga₁.₁Sb₀.₉Te₀.₃ is a ternary III-V semiconductor alloy combining gallium antimonide with tellurium doping, designed to engineer the bandgap and carrier transport properties of the GaSb base compound. This is primarily a research and development material rather than a production commodity; it belongs to the family of narrow-bandgap semiconductors used when thermal sensitivity, infrared responsivity, or high-mobility performance is critical. The tellurium alloying enables tuning of electronic and optical properties for specialized detector and optoelectronic applications where standard binary compounds (GaSb, InSb) do not provide the required performance window.

infrared detectorsthermal imaging sensorshigh-mobility electronics
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Ga12 Co4

semiconductorGa12 Co4

Ga₁₂Co₄ is an intermetallic compound combining gallium and cobalt, belonging to the class of metallic semiconductors or intermediate phases found in the Ga-Co binary system. This material exists primarily in research contexts, where it is studied for its potential electronic and structural properties within gallium-cobalt alloy systems used in advanced semiconductor and thermoelectric applications. The compound represents an intermediate stoichiometry in a system explored for high-temperature performance and potential magnetoelectronic properties, though industrial adoption remains limited compared to more established III-V semiconductors or Co-based superalloys.

research semiconductorsintermetallic compoundsthermoelectric materials (experimental)
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