13 Jul 2026

Four-Probe Resistance of a Semiconductor and Determination of Band Gap

practical pg-iv cmp four-probe semiconductor band-gap

Aim

To measure the resistance of a semiconductor by the four-probe method at different temperatures and determine its energy gap.

Apparatus

Four-probe semiconductor unit, constant-current source, microvoltmeter, heater, thermometer, and regulated power supply.

Experimental arrangement

Four-probe semiconductor resistance arrangement
Current is passed through the outer probes and the voltage drop is measured between the inner probes while the sample temperature is varied.

Theory

The four-probe method separates the current contacts from the voltage contacts. A known current enters through the outer probes and the inner probes draw negligible current, so contact resistance and lead resistance do not enter the measured voltage significantly. For a long thin sample, the resistivity is obtained from the measured voltage $V$, current $I$, and geometrical correction factor $G$:

\[\rho=G\frac{V}{I}.\]

For an intrinsic semiconductor, thermal excitation creates electron-hole pairs across the gap. The conductivity varies approximately as $\sigma=\sigma_0e^{-E_g/(2kT)}$. Hence a plot of $\log_{10}\sigma$ against $1/T$ is linear and

\[E_g=-2.303k\frac{d(\log_{10}\sigma)}{d(1/T)}.\]

Observations

Temperature (K) Current (mA) Probe voltage (mV) Resistivity (ohm m)
303 2.0 18.2 0.91
313 2.0 12.8 0.64
323 2.0 8.8 0.44
333 2.0 6.0 0.30
343 2.0 4.0 0.20

For this trial sheet, the geometrical correction factor is $G=0.10\,\text{m}$.

Graph

Log conductivity versus inverse temperature graph for band gap
The negative slope of $\log_{10}\sigma$ versus $1000/T$ gives the energy gap.

Calculation

For the first reading,

\[\rho=G\frac{V}{I}=0.10\frac{18.2\times10^{-3}}{2.0\times10^{-3}}=0.910\,\Omega\,\text{m}.\]

Therefore,

\[\sigma=\frac{1}{\rho}=\frac{1}{0.910}=1.10\,\text{S m}^{-1}.\]

The graph is plotted against $1000/T$. Its slope is approximately $-3.36$ per unit of $1000/T$, which corresponds to $-3360$ K when the horizontal variable is $1/T$. Hence

\[E_g=-2.303(8.617\times10^{-5})(-3360)=0.67\,\text{eV}.\]

Result

The semiconductor shows decreasing resistivity with increasing temperature, and the energy gap obtained from the graph is

\[\boxed{E_g\approx0.67\,\text{eV}}.\]

Viva Questions

  1. Why are four probes used? The voltage contacts carry negligible current, so contact resistance has little effect.
  2. Why is the sample heated gradually? To maintain thermal equilibrium and avoid temperature gradients.
  3. What indicates semiconductor behaviour? Its resistance decreases as temperature increases.

Maxima Code

Download the PG-IV calculation file.

© Rajesh Kumar, SKMU · Physics Lecture Notes · rajeshphy.github.io

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