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- Hint: The term gap in a general sense means there is a space which is empty between two regions. Here we are talking about the energy gap. We must have a clear idea about how temperature enables electrons from a lower energy level to get to higher energy levels.
Complete step-by-step solution -
First, we need to understand what is a forbidden energy gap. The forbidden energy band gap of a semiconductor is the energy difference (in eV) between the top of the conduction band and the bottom of the valence band in any materials whether it be a metal, an insulator or a semiconductor.
For easy understanding, we can say that the gap is a region where there are no states available for an electron to occupy.
In semiconductors, the conduction band and the valence band are separated by a small energy difference of about 1 eV. This is a small energy difference and can be overcome by thermal agitation.
The energy gap of a semiconductor material is dependent on the temperature. So as the temperature increases from room temperature there is a decrease in the forbidden energy gap. The relation between the forbidden energy gap and temperature is given by the equation,
$E_{g}(T)=E_{g}(0)-\dfrac{\alpha T^{2}}{T+\beta}$
Where,
$E_{g}(T)$ is the forbidden energy gap of the semiconductor at a temperature T.
$E_{g}(0)$ is the intrinsic forbidden energy gap of the semiconductor.
$\alpha$ and $\beta$ are constants.
Hence, Option (B) is correct.
Note: In the case of metals, the conduction band and valence band overlap each other. In insulators, the conduction band and the valence band are separated by a high energy difference (greater than 10 eV).
Complete step-by-step solution -
First, we need to understand what is a forbidden energy gap. The forbidden energy band gap of a semiconductor is the energy difference (in eV) between the top of the conduction band and the bottom of the valence band in any materials whether it be a metal, an insulator or a semiconductor.
For easy understanding, we can say that the gap is a region where there are no states available for an electron to occupy.
In semiconductors, the conduction band and the valence band are separated by a small energy difference of about 1 eV. This is a small energy difference and can be overcome by thermal agitation.
The energy gap of a semiconductor material is dependent on the temperature. So as the temperature increases from room temperature there is a decrease in the forbidden energy gap. The relation between the forbidden energy gap and temperature is given by the equation,
$E_{g}(T)=E_{g}(0)-\dfrac{\alpha T^{2}}{T+\beta}$
Where,
$E_{g}(T)$ is the forbidden energy gap of the semiconductor at a temperature T.
$E_{g}(0)$ is the intrinsic forbidden energy gap of the semiconductor.
$\alpha$ and $\beta$ are constants.
Hence, Option (B) is correct.
Note: In the case of metals, the conduction band and valence band overlap each other. In insulators, the conduction band and the valence band are separated by a high energy difference (greater than 10 eV).
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