---
title: "Temperature effect on carrier concentration"
subject: "Electrical Engineering Material"
chapter: 6
key: "semester_3/electrical_engineering_material:temperature-carrier-concentration"
source: https://www.bctengineer.com/q/semester_3/electrical_engineering_material/temperature-carrier-concentration
site: BCT Engineering
---

# Temperature effect on carrier concentration

Electrical Engineering Material · Chapter 6: Semiconductors

- Asked in: 2079 Bhadra, 6 marks; 2073 Chaitra, 6 marks (asked 2 times)
- Video: [Solid State Electronics | Temperature Dependence of Carrier Concentration (Extrinsic)](https://www.youtube.com/watch?v=H2L6N-HKAA4) — India Engineered
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_3/electrical_engineering_material/temperature-carrier-concentration
- Whole chapter: https://www.bctengineer.com/md/semester_3/electrical_engineering_material/chapter-6

## Question

Explain how does temperature affects the formation of carrier concentration in semiconductor.

## Short answer

In intrinsic semiconductors, carrier concentration rises exponentially with temperature: ni ∝ T^(3/2) exp(-Eg/2kT). In doped semiconductors, three regions emerge: at low T ionisation gives n ∝ exp(-ΔE/2kT); at medium T saturation n ≈ Nd constant; at high T intrinsic generation dominates, n ≈ ni again.

## Answer

The carrier concentration in a semiconductor depends strongly on temperature because carriers are created thermally, either by ionising impurities or by breaking covalent bonds across the band gap.

#### Intrinsic semiconductor
Electron-hole pairs are created when thermal energy lifts electrons across $E_g$:

$$
n_i = \sqrt{N_cN_v}\,\exp\left(-\frac{E_g}{2kT}\right), \quad N_c, N_v \propto T^{3/2}
$$

so $n_i \propto T^{3/2}e^{-E_g/2kT}$. The exponential dominates: for Si, $n_i$ roughly doubles for every 8 to 10 K rise near room temperature.

#### Extrinsic (n-type) semiconductor
A plot of $\ln n$ against $1/T$ shows three regions:

1. **Low temperature (ionisation or freeze-out region):** only some donors are ionised.

$$
n = \left(\frac{1}{2}N_cN_d\right)^{1/2}\exp\left(-\frac{\Delta E}{2kT}\right), \quad \Delta E = E_c - E_d
$$

2. **Medium temperature (extrinsic or saturation region):** all donors are ionised, $n \approx N_d$, nearly constant. This range (about 150 K to 500 K for Si with $N_d = 10^{15}$ cm$^{-3}$) is where devices work. It begins at the saturation temperature $T_s$, where the donors become fully ionised.

3. **High temperature (intrinsic region):** thermal generation across $E_g$ exceeds $N_d$; $n \approx n_i$ and the material behaves as intrinsic. The changeover temperature $T_i$ is where $n_i \approx N_d$.

```text
 ln n
   |\
   | \   intrinsic region
   |  \  slope -Eg/2k
   |   \
   |    \____________________  n = Nd
   |       extrinsic region  \
   |                          \   ionisation region
   |                           \  slope -ΔE/2k
   +-----|--------------------|-------- 1/T
        1/Ti                 1/Ts
   (high T at left, low T at right)
```

#### Fermi level
As $T$ rises, $E_F$ moves from near $E_d$ (low $T$) towards mid-gap (high $T$), because the extrinsic carriers become a smaller fraction of the total.

The upper limit of device operation is set by $T_i$; wide band gap materials (GaAs, SiC) have higher $T_i$ and can work at higher temperatures.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What mainly controls the rise of n_i with temperature?
   A. The T^(3/2) factor in Nc and Nv
   B. The exponential factor exp(-Eg/2kT)
   C. A change in the mobility
   D. A change in donor concentration
   Answer: B. n_i is proportional to T^(3/2) exp(-Eg/2kT), and the exponential dominates, so n_i doubles every 8 to 10 K near room temperature. (Key point: Intrinsic temperature dependence)

2. What is the electron concentration in the medium-temperature (extrinsic) region of an n-type sample?
   A. n is about ni and rises steeply
   B. n is about Nd, nearly constant
   C. n is zero
   D. n falls exponentially
   Answer: B. All donors are ionised and intrinsic generation is still small, so n is about Nd; devices operate here. (Key point: Saturation region)

3. What happens at high temperature above Ti?
   A. Donors freeze out
   B. n stays constant at Nd
   C. Holes disappear
   D. Thermal generation across Eg exceeds Nd, so n is about ni and the material becomes intrinsic
   Answer: D. Band-to-band generation dominates and the slope of ln n versus 1/T becomes -Eg/2k. (Key point: High temperature region)

## Related in Electrical Engineering Material

- [n-type carrier concentration versus temperature](https://www.bctengineer.com/question.md?key=semester_3%2Felectrical_engineering_material%3Antype-concentration-temperature) — Electrical Engineering Material, chapter 6, asked 2×
- [Temperature dependence of carrier concentration and mobility](https://www.bctengineer.com/question.md?key=semester_3%2Felectrical_engineering_material%3Atemperature-carrier-mobility) — Electrical Engineering Material, chapter 6, asked 2×
- [Electron concentration in an extrinsic semiconductor](https://www.bctengineer.com/question.md?key=semester_3%2Felectrical_engineering_material%3Aextrinsic-electron-concentration) — Electrical Engineering Material, chapter 6
- [Intrinsic concentration and its temperature dependence](https://www.bctengineer.com/question.md?key=semester_3%2Felectrical_engineering_material%3Aintrinsic-concentration-derivation) — Electrical Engineering Material, chapter 6
- [Intrinsic Fermi level of pure semiconductor](https://www.bctengineer.com/question.md?key=semester_3%2Felectrical_engineering_material%3Aintrinsic-fermi-level) — Electrical Engineering Material, chapter 6
- [Compensated semiconductor concentrations and conductivity](https://www.bctengineer.com/question.md?key=semester_3%2Felectrical_engineering_material%3Acompensated-conductivity) — Electrical Engineering Material, chapter 6

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