Band Gap of Semiconductor Materials

Semiconductor band gap is the energy difference between the valence-band maximum and conduction-band minimum and is typically measured in electron volts (eV). Band-gap energy strongly influences a material's intrinsic carrier concentration, electrical and optical behavior, and suitability for applications such as solar cells, photodetectors, LEDs, power electronics, and infrared devices. Explore band-gap values and properties of silicon, GaAs, InAs, InSb, SiC, and other semiconductor materials used in research and device fabrication.

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Researching Intense Radiation Effects on Materials with Different Band Gaps

A nuclear engineering graduate student requested semiconductor materials for research on radiation-induced surface defects and the effects of intense radiation on materials with different electronic band gaps.

Customer request, edited for clarity: I am researching the effects of intense radiation on materials with different ionization energies. So far, I have primarily studied gases, but I would now like to study semiconductor materials with different band gaps.

Because the samples will be exposed to intense radiation and may be damaged during testing, I am interested in lower-cost pieces such as diced wafers , broken wafers, or other suitable research-grade pieces. Samples approximately 1 cm or larger in length and width would be useful. Thickness is not critical because the initial research will focus on surface defects.

It would be ideal to obtain a variety of semiconductor materials, including Si, Ge, GaAs, InSb, and InAs, with a combination of undoped, n-type, and p-type samples where available.

Reference #213033 for specs and pricing.

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What Is a Semiconductor Band Gap?

The band gap (Eg) is the energy difference between the valence-band maximum and the conduction-band minimum of a material. It represents the minimum energy required for an electron to be excited from the valence band into the conduction band, where it can contribute to electrical conduction.

Band-gap energy is normally expressed in electron volts (eV). In general, materials with very large band gaps have very low intrinsic carrier concentrations and behave as electrical insulators, while semiconductors have band gaps that allow their electrical properties to be controlled through doping, temperature, illumination, and applied electric fields.

A smaller semiconductor band gap generally produces a higher intrinsic carrier concentration at a given temperature because less thermal energy is required to excite electrons across the gap. However, the actual conductivity of a semiconductor also depends strongly on doping concentration, carrier mobility, temperature, defects, impurities, and material quality.

The table below lists representative room-temperature band-gap values for several common semiconductor materials, along with wide-gap silica materials for comparison. Exact values can vary with temperature, crystal structure, composition, strain, and other material conditions.

Material Material Type Typical Band Gap Near 300 K (eV)
Silicon (Si) Semiconductor ~1.12
Gallium Arsenide (GaAs) Semiconductor ~1.42
Gallium Antimonide (GaSb) Semiconductor ~0.73
4H Silicon Carbide (4H-SiC) Wide-Bandgap Semiconductor ~3.23
Germanium (Ge) Semiconductor ~0.66
Fused Silica (SiO2) Wide-Gap Insulator ~9
Single-Crystal Quartz (SiO2) Wide-Gap Insulator ~9

How Do You Determine the Energy Band Gap of a Material?

For crystalline solids, the electronic band gap is defined as the energy difference between the valence-band maximum (VBM) and the conduction-band minimum (CBM). The molecular terms HOMO and LUMO are more commonly used for discrete molecules and molecular systems and should not generally be used as direct substitutes for the valence and conduction bands of a bulk crystalline semiconductor.

Band gaps can be determined experimentally or estimated through electronic-structure calculations. The appropriate technique depends on the material, whether the transition is direct or indirect, the sample geometry, and the accuracy required.

  1. Experimental Methods

    • Optical Absorption Spectroscopy: A semiconductor absorbs photons capable of producing electronic transitions. Analysis of the absorption edge can be used to estimate the optical band gap. The analysis must account for whether the material has a direct or indirect transition and for effects such as disorder, excitons, defects, and sample thickness.

    • Photoluminescence Spectroscopy: The material is optically excited and the emitted photons are analyzed. Photoluminescence can provide valuable information about band-edge transitions, excitons, impurities, and defects. The strongest emission peak does not necessarily equal the fundamental band-gap energy in every material.

    • Photoconductivity: Changes in electrical conductivity are measured while the sample is illuminated with photons of different energies. The onset of photoconductivity can provide information about electronic excitation thresholds and the band gap.

    • Electron Energy-Loss Spectroscopy (EELS): EELS measures the energy lost by electrons as they interact with a thin specimen. Low-loss EELS can provide information about electronic excitations and, with appropriate analysis, can be used to investigate a material's band-gap region.

  2. Computational Methods

    Electronic-structure calculations can also be used to estimate semiconductor band structures and band gaps. Density functional theory (DFT) is widely used to calculate electronic structure, but common semilocal DFT approximations often underestimate semiconductor band gaps.

    More advanced approaches, including hybrid functionals and the GW approximation, can provide improved predictions in many materials, although they generally require greater computational resources and expertise. Calculated values depend on the theoretical method, structural model, and material conditions used in the calculation.

Because each technique measures somewhat different aspects of a material's electronic or optical response, researchers may use several complementary methods when accurate band-gap characterization is required.

FAQs About Band Gaps in Semiconductors

What is a band gap in a semiconductor?
The band gap is the energy difference between the valence-band maximum and the conduction-band minimum. It determines the minimum energy required for band-to-band electronic excitation and strongly influences a material's electrical and optical properties.
Which materials are wide-bandgap semiconductors?
Important wide-bandgap semiconductors include silicon carbide (SiC) and gallium nitride (GaN). Their relatively large band gaps, together with properties such as high critical electric fields, make them useful for many high-power, high-voltage, high-temperature, and high-frequency applications. Fused silica and quartz also have large electronic band gaps, but they are normally classified as electrical insulators rather than wide-bandgap semiconductors.
Why is band gap important in solar cells?
The semiconductor band gap influences which photon energies can generate electron-hole pairs and affects the balance between solar-cell current and voltage. A smaller band gap allows absorption of lower-energy, longer-wavelength photons and can increase potential photocurrent, but it generally lowers the maximum attainable voltage. A larger band gap can support a higher voltage but leaves more low-energy photons unabsorbed. Therefore, photovoltaic design involves optimizing the band gap rather than simply choosing the smallest possible value.
Does a smaller band gap make a semiconductor more conductive?
For an intrinsic semiconductor at a given temperature, a smaller band gap generally produces a higher intrinsic carrier concentration and therefore higher intrinsic electrical conductivity. In real semiconductor wafers, however, conductivity also depends strongly on dopant concentration, carrier mobility, temperature, defects, impurities, and material quality.

Low-Bandgap Semiconductors for Solar Cells and Photovoltaic Research

A graduate research assistant requested help with the following:

Can you please let me know if you have a low-bandgap semiconductor that can be used to fabricate a solar or photovoltaic cell ? We would also like to know whether the doping profile of the material can be customized.

I can provide a research paper that we would like to follow to fabricate an InAs photodiode. The doping profile discussed in the paper is described below.

The InAs wafer studied in the referenced work was grown by metalorganic vapor-phase epitaxy (MOVPE) on a 2-inch p-type InAs substrate. The epitaxial structure consisted of a 2 µm p+ InAs layer doped with Zn at a nominal concentration of approximately 1 × 1018 cm−3, followed by an 8 µm nominally intrinsic InAs layer and a 2 µm n+ InAs layer doped with Si at approximately 1 × 1018 cm−3.

Band Gaps of Common Low-Bandgap Semiconductors

Representative room-temperature band-gap values for several common semiconductor materials are listed below. Exact values can vary with temperature, crystal quality, composition, strain, and other material conditions.

  • Silicon (Si): approximately 1.12 eV
  • Germanium (Ge): approximately 0.66 eV
  • Indium Arsenide (InAs): approximately 0.35 eV
  • Indium Antimonide (InSb): approximately 0.17 eV

Based on these values, low-bandgap materials such as InAs and InSb are especially useful for infrared optoelectronics, photodetectors, and other applications requiring sensitivity to lower-energy, longer-wavelength photons.

Depending on current inventory and specifications, these materials may be available in different diameters, conductivity types, doping levels, and crystallographic orientations. Availability should be confirmed for the required wafer diameter, orientation, carrier concentration, thickness, surface finish, and doping type.

We can also produce epitaxial structures using MOCVD or related epitaxial-growth techniques. Epitaxial structures can be designed with specified layer thicknesses, compositions, and doping profiles, subject to material-system and growth-process limitations.

Band-gap engineering is generally achieved by changing alloy composition, strain, heterostructure design, or quantum confinement. Doping is primarily used to control carrier concentration and electrical properties and does not by itself allow arbitrary control of the fundamental band gap of bulk InAs.

Example InAs Epitaxial Structure

Proposed structure:

Item   Qty.   Description
GG04.   1/10   Epitaxial wafers, 2" diameter × 500 ± 25 µm, two flats
Substrate: p-type InAs:Zn, (100) ± 0.5°, carrier concentration approximately 1 × 1018 to 3 × 1018 cm−3, EPD < 10,000 cm−2, one-side polished, backside alkaline etched
Epi Layer 1: 2.0 µm p-type InAs:Zn, approximately 1 × 1018 cm−3
Epi Layer 2: 8.0 µm nominally undoped InAs, carrier concentration < 1 × 1016 cm−3
Epi Layer 3: 2.0 µm n-type InAs:Si, approximately 1 × 1018 cm−3

The epitaxial-growth facility would need to verify process capability, layer specifications, and pricing for the requested structure. Required InAs substrate availability should also be confirmed at the time of quotation.

Before finalizing the structure, it may be useful to determine whether thinner epitaxial layers could satisfy the device requirements and whether a separate p-type InAs:Zn epitaxial layer is necessary when the substrate itself is already p-type InAs:Zn.

Reference #228706 for specs and pricing.

Diagram comparing the band structure of conductors, semiconductors, and insulators

What Are the Effects of a Smaller Band Gap Than Silicon?

A semiconductor with a smaller band gap than silicon generally requires less energy to excite electrons from the valence band into the conduction band. In an intrinsic semiconductor, a smaller band gap generally produces a higher intrinsic carrier concentration at a given temperature and therefore higher intrinsic electrical conductivity.

However, band gap alone does not determine the conductivity or resistivity of a real semiconductor wafer. Electrical conductivity also depends strongly on dopant concentration, electron and hole mobility, temperature, defects, impurities, crystal quality, and other material properties.

How Does Band Gap Affect Intrinsic Carrier Concentration?

Thermal energy can excite a fraction of electrons across the semiconductor band gap. The intrinsic carrier concentration depends strongly on both band-gap energy and temperature. Materials with smaller band gaps generally have much larger intrinsic carrier concentrations than wider-bandgap materials at the same temperature.

This is one reason narrow-bandgap semiconductors such as InAs and InSb can exhibit significant intrinsic carrier populations even near room temperature, while wider-bandgap semiconductors maintain lower intrinsic carrier concentrations.

How Does Temperature Affect a Semiconductor Band Gap?

Temperature and band-gap energy should not be directly compared because they are different physical quantities. Temperature is normally expressed in kelvin (K), while band-gap energy is expressed in electron volts (eV).

The relevant thermal-energy scale is kBT, where kB is the Boltzmann constant and T is absolute temperature. As temperature rises, more carriers can be thermally excited across the band gap, increasing the intrinsic carrier concentration.

The band gap itself also usually changes with temperature. For many semiconductors, including silicon, the band gap decreases gradually as temperature increases.

A narrower band gap does not inherently cause a material to become hotter. Device temperature depends on electrical power dissipation, thermal conductivity, cooling, packaging, operating conditions, and device design.

How Does a Smaller Band Gap Affect Optical Absorption?

The band gap determines the approximate minimum photon energy required for band-to-band excitation. Photon energy and wavelength are related approximately by:

E (eV) ≈ 1240 / λ (nm)

A smaller band gap allows a semiconductor to respond to lower-energy, longer-wavelength photons. This is why low-bandgap semiconductors such as InAs and InSb are useful for infrared detectors, infrared imaging, spectroscopy, and other optoelectronic applications.

Direct versus indirect band structure also matters. Direct-bandgap semiconductors generally exhibit stronger near-band-edge optical absorption and more efficient radiative emission than indirect-bandgap semiconductors such as silicon.

Does a Smaller Band Gap Make a Better Solar Cell?

Not necessarily. A smaller band gap allows a photovoltaic material to absorb lower-energy, longer-wavelength photons, which can increase the potential photocurrent. However, reducing the band gap also generally reduces the maximum achievable voltage.

A larger band gap can support a higher output voltage, but photons with energies below the band gap cannot generate electron-hole pairs through ordinary band-to-band absorption. Photons with energy far above the band gap also lose excess energy through carrier thermalization.

Solar-cell efficiency therefore involves a tradeoff between photon absorption, photocurrent, voltage, recombination, thermalization losses, and other device-level factors. There is no general rule that either the smallest or largest possible band gap produces the highest efficiency.

Multi-junction photovoltaic cells address this tradeoff by combining semiconductor materials with different band gaps. Higher-bandgap junctions absorb higher-energy photons, while lower-bandgap junctions can absorb lower-energy photons that pass through the upper layers.

How Are Semiconductor Band Gaps Measured?

Semiconductor band gaps can be investigated using several experimental methods, including optical absorption spectroscopy, photoluminescence, photoconductivity, temperature-dependent electrical measurements, spectroscopic ellipsometry, and electron energy-loss spectroscopy.

The appropriate analysis depends on the semiconductor and whether its fundamental transition is direct or indirect. For example, optical absorption data are often analyzed differently for direct- and indirect-bandgap materials.

Temperature-dependent conductivity measurements can also provide information about activation energies, but the slope of a conductivity-versus-temperature plot should not automatically be interpreted as the fundamental band gap without considering doping, defect levels, conduction mechanisms, and the temperature range being studied.

What Does the k-Vector Mean in a Band Structure?

The k-vector, or crystal wave vector, describes an electron state in reciprocal space. It is not a measurement of band-gap energy.

A semiconductor band structure plots electron energy as a function of k. The band gap is the energy difference between the valence-band maximum and the conduction-band minimum.

If these extrema occur at the same k-value, the semiconductor has a direct band gap. If they occur at different k-values, as in silicon, the material has an indirect band gap.

Smaller vs. Larger Band Gaps

Neither a smaller nor a larger band gap is universally better. The appropriate material depends on the application.

  • Narrow-bandgap semiconductors generally have higher intrinsic carrier concentrations and can detect longer-wavelength radiation.
  • Moderate-bandgap semiconductors such as silicon and GaAs are widely used in electronics and photovoltaics because they provide useful combinations of electrical, optical, and manufacturing properties.
  • Wide-bandgap semiconductors such as SiC and GaN generally have lower intrinsic carrier concentrations and high critical electric fields, making them useful for high-voltage, high-temperature, high-frequency, and high-power devices.

Material selection should therefore consider band gap together with carrier mobility, breakdown field, thermal conductivity, doping capability, optical response, crystal quality, fabrication requirements, and intended operating conditions.

Watch: Semiconductor Band Gap Explanation

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