Step 1: Recall the formula for intrinsic carrier concentration (\(n_i\)).
The intrinsic carrier concentration in a semiconductor is a function of temperature \(T\) and the energy bandgap \(E_g\). The standard formula is:
\[
n_i = A T^{3/2} \exp\left(-\frac{E_g}{2k_B T}\right)
\]
where \(A\) is a material-specific constant and \(k_B\) is the Boltzmann constant.
Step 2: Analyze the temperature dependence.
The formula shows that \(n_i\) depends on temperature in two ways: through the \(T^{3/2}\) term and the exponential term \(\exp(-E_g / 2k_B T)\). The exponential term describes the dominant temperature dependence, but the question asks how the concentration *varies with* T, and the pre-exponential factor \(T^{3/2}\) is a key part of this variation.
Step 3: Compare with the given options.
The options provided are power-law dependencies on \(T\). The pre-exponential factor in the expression for \(n_i\) is \(T^{3/2}\), which matches option (3).