Materials/Semiconductors/Collections
Semiconductor materials
semiconductor-materialsAbout semiconductor materials
Semiconductor materials (silicon, germanium, silicon-germanium, gallium arsenide, gallium nitride, selenium, tellurium, bismuth telluride): band gap, thermal and electrical data with sources.
Semiconductors are the base of chips, solar cells, detectors and thermoelectric generators. Their electrical behaviour depends strongly on purity, doping and temperature, so each value names its condition.
At a glance
- Highest density: Bismuth telluride reaches 7.64 g/cm³. Lowest: Silicon starts at 2.33 g/cm³. (10 of 10 grades have a sourced value.)
- Highest melting point: Gallium nitride (GaN) reaches 2,500 °C. Lowest: Selenium starts at 221 °C. (9 of 10 grades have a sourced value.)
Ranges run across the conditions each source reports (temper, heat treatment, form), measured at room temperature where the source says so.
How they compare
The same measurements for every material in the collection. A range means the grade has values under several conditions; "at least" means the source gives a specified minimum. "no data" means no sourced value yet. For ranked tables, open a benchmark.
| Material | Density | Melting point | Electrical resistivity | Thermal conductivity | Young's modulus | Thermal expansion |
|---|---|---|---|---|---|---|
| Siliconsemiconductor | 2.33 g/cm³ | 1,415 °C | no data | 150 W/(m·K) | no data | no data |
| Germaniumsemiconductor | 5.33 g/cm³ | 936 to 937 °C | no data | 58.6 W/(m·K) | 103 GPa | 5.8 to 6.1 ppm/K |
| Silicon-germanium alloy (SiGe)semiconductor | 4.31 g/cm³ | no data | no data | no data | no data | no data |
| Gallium arsenide (GaAs)semiconductor | 5.32 g/cm³ | 1,238 to 1,240 °C | 3,300,000 Ω·m | 46 to 55 W/(m·K) | no data | 5.73 to 6.86 ppm/K |
| Gallium nitride (GaN)wide-bandgap semiconductor | 6.15 g/cm³ | 2,500 °C | no data | 130 W/(m·K) | no data | 5.59 ppm/K |
| Arsenic (As)Metalloid: feedstock for gallium arsenide semiconductors and a dopant | 5.73 g/cm³ | 817 °C | no data | 50 W/(m·K) | 8 GPa | no data |
| Boronneutron absorber, hard amorphous powder and reinforcing fibre | 2.35 to 2.61 g/cm³ | 2,075 °C | no data | 27 W/(m·K) | 428 GPa | 4.5 to 6 ppm/K |
| Seleniumchalcogen element; photoconductor and CIGS solar-cell component | 4.81 g/cm³ | 221 °C | no data | 0.52 W/(m·K) | 10 GPa | no data |
| Telluriummetalloid, semiconductor compound element and alloy additive | 6 to 6.25 g/cm³ | 450 °C | no data | 3 W/(m·K) | 43 GPa | no data |
| Bismuth telluridethermoelectric alloy base and layered topological insulator | 6.5 to 7.64 g/cm³ | 573 to 629 °C | no data | 1.29 to 1.48 W/(m·K) | no data | no data |
What these materials are made of
Composition by weight, as printed in the sources for each grade (the first constituents listed).
| Material | Main constituents |
|---|---|
| Silicon | Si 100% |
| Germanium | Ge 100% |
| Silicon-germanium alloy (SiGe) | Si 80% · Ge 20% |
| Gallium arsenide (GaAs) | Ga 48.2% · As 51.8% |
| Arsenic (As) | As 100.0% |
| Boron | 10B 20% · 11B 80% |
| Selenium | Se 100% |
| Tellurium | Te 100.0% |
| Bismuth telluride | Bi 40% · Te 60% |
Where they are used
| Use | Grades |
|---|---|
| Single-crystal silicon wafer substrate | Silicon |
| Semiconductor chips | Silicon |
| Silicon solar cell | Silicon |
| Infrared lenses and windows for thermal imaging | Germanium |
| ATR prisms for infrared spectroscopy | Germanium |
| Optical fibre glass | Germanium |
| SiGe heterojunction bipolar transistors (HBTs) in RF and mixed-signal chips | Silicon-germanium alloy (SiGe) |
| SiGe strain layer in CMOS transistors | Silicon-germanium alloy (SiGe) |
| Radioisotope thermoelectric generators (MHW-RTG and GPHS-RTG; a power source, not a battery) | Silicon-germanium alloy (SiGe) |
| Triple-junction space solar cell (GaInP/GaAs/Ge) | Gallium arsenide (GaAs) |
| Power amplifier in cellular handsets | Gallium arsenide (GaAs) |
| Laser diodes, LEDs and photodetectors | Gallium arsenide (GaAs) |
| GaN power transistor (EPC2045, 100 V) | Gallium nitride (GaN) |
| GaN integrated circuits and optoelectronic devices | Gallium nitride (GaN) |
| EPC1001 enhancement-mode GaN transistor (ground test) | Gallium nitride (GaN) |
| Gallium arsenide and indium gallium arsenide semiconductors | Arsenic (As) |
When each grade fits
| Material | Best for | Weakest at |
|---|---|---|
| Silicon | Semiconductor wafers: a 1.12 eV band gap at 300 K and a well-documented resistivity range from doping | Light emission and heat flow: an indirect band gap (not stated in the sources read) and thermal conductivity of 150 W/(m·K), well below metals |
| Germanium | Infrared optics from 1.8 to 23 µm (thermal-imaging lenses, ATR prisms) and substrates for triple-junction space solar cells | Temperature limit and supply: Crystran says germanium becomes opaque at all wavelengths a little above 350 K, and the USGS says supply runs through a few producers, China the leading one |
| Silicon-germanium alloy (SiGe) | High-temperature thermoelectric legs for radioisotope generators, and SiGe transistors for fast RF chips | Thermoelectric efficiency: NASA says the figure of merit of Si-Ge is much lower than that of lead telluride |
| Gallium arsenide (GaAs) | Light emission, RF power and multijunction space solar cells, where the band gap and electron mobility of GaAs beat silicon (1.424 eV and up to 8500 cm2/(V·s)) | Cost and toxicity: the arsenic content is classed as carcinogenic in GHS, and the gallium supply is concentrated in China (99% of primary low-purity gallium) |
| Gallium nitride (GaN) | High-voltage and high-frequency power switching, and radiation-tolerant electronics where a wide band gap and high breakdown field matter (NASA ground tests of GaN transistors) | Modest electron mobility compared with the best III-V materials, and the cost and limited supply of gallium |
| Arsenic (As) | Source of high-purity arsenic metal for GaAs and InGaAs semiconductors and for specialty infrared optics (USGS) | Toxicity: PubChem reports H301 and H331 for most reporting companies, and ATSDR classes inorganic arsenic as a known human carcinogen |
| Boron | Thermal-neutron absorption where boron-10 content matters (NIST cross sections; NASA 1995 shielding report) and boron fibre for stiff composite plies (Specialty Materials datasheet) | Oxidation and reactivity: amorphous boron powder can ignite spontaneously as dust and reacts violently with steam at red heat (Materion; PubChem, citing Bretherick) |
| Selenium | Thin-film photovoltaics and photoconductive devices where a selenium compound is the active absorber or photoconductor | Toxicity and reactivity: the supplier SDS classes it as toxic if swallowed or inhaled, it burns in air when heated, and it releases toxic hydrogen selenide if heated above 50 degC in water |
| Tellurium | CdTe thin-film solar cells and bismuth telluride thermoelectric devices, the two largest uses (USGS) | Supply and toxicity: most of it is a copper by-product, China leads refined output, and the element is toxic if swallowed |
| Bismuth telluride | Room-temperature thermoelectric coolers and generators, where the p-type alloy reached zT 1.24 before storage | Humid, hot storage: 600 h at 85 degC and 85% RH oxidised the surface and cut zT by 19 and 22 percent (authors) |