Estimate intrinsic electron and hole concentration from semiconductor band gap, temperature, and effective density of states.
Semiconductor carrier concentration
Enter consistent density-of-states values in inverse cubic centimeters.
About intrinsic carrier concentration
An intrinsic semiconductor is an ideal, chemically pure semiconductor whose mobile electrons and holes are created by thermal excitation rather than intentional dopants. At thermal equilibrium, every electron promoted into the conduction band leaves one hole in the valence band, so the electron concentration equals the hole concentration. That common value is called the intrinsic carrier concentration, usually written ni. It provides a fundamental scale for understanding conductivity, junction behavior, leakage current, and the limits of semiconductor devices.
This calculator evaluates the standard nondegenerate-semiconductor relation ni = sqrt(Nc × Nv) × exp(-Eg / (2kT)). Eg is the energy band gap in electronvolts, T is absolute temperature in kelvin, and k is the Boltzmann constant expressed as 8.617333262 × 10^-5 electronvolts per kelvin. Nc and Nv are the effective densities of available quantum states in the conduction and valence bands. Because the result uses the same volume unit as those density inputs, entering both in cm^-3 produces ni in cm^-3.
The exponential term makes carrier concentration extremely sensitive to both band gap and temperature. A narrow-gap material such as germanium has a much larger intrinsic concentration than silicon at the same temperature. A wide-gap material such as silicon carbide can maintain a much smaller intrinsic population at elevated temperature. Increasing temperature supplies more thermal energy, greatly increasing the probability that electrons cross the forbidden band gap. Effective densities of states also change with temperature, commonly in proportion to T raised to the three-halves power, so accurate comparisons should use Nc and Nv evaluated at the selected temperature.
The equation assumes Maxwell-Boltzmann statistics, thermal equilibrium, a spatially uniform material, and carrier populations far below the available state densities. These assumptions work well for many ordinary semiconductor calculations but can break down in heavily doped or degenerate material, under strong optical excitation, or far from equilibrium. The simple expression also does not model band-gap narrowing, traps, defects, strain, or quantum confinement. Material references may quote different effective masses and therefore slightly different density-of-states values.
Use this result as a physically meaningful estimate and keep all units consistent. For device-grade work, source band-gap and effective-mass data for the exact material composition and temperature. Intrinsic concentration connects directly to the mass-action law, where equilibrium electron concentration multiplied by hole concentration equals ni squared. It therefore helps engineers estimate minority carriers, reverse saturation current, resistivity trends, and the temperature range where intrinsic conduction begins to dominate doped behavior.
Intrinsic concentration examples
Material parameters
Calculated ni
Observation
Eg 1.12 eV, 300 K, Nc 2.8e19, Nv 1.04e19
6.6759e9 cm^-3
Representative silicon parameters using a fixed 1.12 eV gap.
Eg 0.66 eV, 300 K, Nc 1.04e19, Nv 6e18
2.2586e13 cm^-3
The narrower germanium-like gap produces many more intrinsic carriers.
Eg 1.12 eV, 350 K, Nc 3.53e19, Nv 1.31e19
1.8573e11 cm^-3
Higher temperature sharply increases the silicon-like carrier population.
How to calculate intrinsic concentration
Enter the semiconductor band gap in electronvolts.
Enter the absolute material temperature in kelvin.
Provide conduction- and valence-band effective densities of states in cm^-3.
Select Calculate Carrier Concentration to evaluate the equilibrium value.
Intrinsic carrier concentration FAQ
Why are intrinsic electron and hole concentrations equal?
Thermal excitation creates an electron and a hole as a pair. In a pure material at equilibrium, neither carrier type has a separate dopant source.
Why does ni increase so quickly with temperature?
The probability of crossing the band gap appears in an exponential Boltzmann factor. Density-of-states values also generally increase with temperature.
Can I enter densities in m^-3?
Yes, if both Nc and Nv use m^-3, the numerical result will also be in m^-3. The displayed unit says cm^-3, so convert the result or inputs for clarity.
Does doping change intrinsic carrier concentration?
Ideal ni is primarily a property of material and temperature, not ordinary doping. Heavy doping can alter the band structure and make the ideal relation less accurate.
Which band gap should I use?
Use the band gap at the calculation temperature and for the exact material composition. Band gap commonly decreases as semiconductor temperature rises.