Solveeit Logo

Question

Question: Assume that the number of hole-electron pairs in an intrinsic semiconductor is proportional to \({{e...

Assume that the number of hole-electron pairs in an intrinsic semiconductor is proportional to eΔE2KT{{e}^{\dfrac{\Delta E}{2KT}}}. Here ΔE=\Delta E=energy gap and k=8.62×105eVK1k=8.62\times {{10}^{5}}eV{{K}^{-1}}. The energy gap for silicon is 1.1eV1.1eV. The ratio of electron hole pairs at 300K300K and 400K400Kis,
A.e5.104×108 B.e5 C.e D.e2 \begin{aligned} & A.{{e}^{5.104\times {{10}^{-8}}}} \\\ & B.{{e}^{-5}} \\\ & C.e \\\ & D.{{e}^{2}} \\\ \end{aligned}

Explanation

Solution

the number of hole-electron pairs in an intrinsic semiconductor is given as proportional to eΔE2KT{{e}^{\dfrac{\Delta E}{2KT}}}. Therefore substitute the given temperatures in this equation. So we can get the ratio of these two quantities. This ratio will be equal to the number of electron-hole pairs in the intrinsic semiconductor. Hope this will help you to solve this question.

Complete step by step answer:
it is already mentioned in the question that the energy gap of the silicon semiconductor is,
ΔE=1.1eV\Delta E=1.1eV
And also it is mentioned that,
k=8.62×105eVK1k=8.62\times {{10}^{5}}eV{{K}^{-1}}
As we know that the number of the electron- hole pair ratio is found to be proportional to eΔE2KT{{e}^{\dfrac{\Delta E}{2KT}}}.
eΔE2KT1eΔE2KT2=N1N2\dfrac{{{e}^{\dfrac{\Delta E}{2K{{T}_{1}}}}}}{{{e}^{\dfrac{\Delta E}{2K{{T}_{2}}}}}}=\dfrac{{{N}_{1}}}{{{N}_{2}}}
Therefore let us calculate this quantity instead of the other for the comparison.
For 300K300K, we can find the value of eΔE2KT{{e}^{\dfrac{\Delta E}{2KT}}} by substituting the other terms also,
eΔE2KT1=e(1.12(8.62×105)(300)){{e}^{\dfrac{\Delta E}{2K{{T}_{1}}}}}={{e}^{\left( \dfrac{1.1}{2\left( 8.62\times {{10}^{5}} \right)\left( 300 \right)} \right)}}
For 400K400K we can write that,
eΔE2KT2=e(1.12(8.62×105)(400)){{e}^{\dfrac{\Delta E}{2K{{T}_{2}}}}}={{e}^{\left( \dfrac{1.1}{2\left( 8.62\times {{10}^{5}} \right)\left( 400 \right)} \right)}}
Let us take the ratio of these quantities. This will be similar to taking the ratio of the number of electron-hole pairs. Therefore the ratio of this quantity can be written as,
number of electron holepair at 300Knumber of electron holepair at 400K=e(1.12(8.62×105)(300))e(1.12(8.62×105)(400))\dfrac{\text{number of electron holepair at 300K}}{\text{number of electron holepair at 400K}}=\dfrac{{{e}^{\left( \dfrac{1.1}{2\left( 8.62\times {{10}^{5}} \right)\left( 300 \right)} \right)}}}{{{e}^{\left( \dfrac{1.1}{2\left( 8.62\times {{10}^{5}} \right)\left( 400 \right)} \right)}}}
Simplifying the above equation will give,
N1N2=e(1.12(8.62×105))(13001400)\dfrac{{{N}_{1}}}{{{N}_{2}}}={{e}^{\left( \dfrac{1.1}{2\left( 8.62\times {{10}^{5}} \right)} \right)\left( \dfrac{1}{300}-\dfrac{1}{400} \right)}}
number of electron holepair at 300Knumber of electron holepair at 400K=e5.31×108\dfrac{\text{number of electron holepair at 300K}}{\text{number of electron holepair at 400K}}={{e}^{-5.31 \times 10^{-8}}}

So, the correct answer is “Option A”.

Note: The electron–hole pair is the basic unit for generation and recombination usually seen in the semiconductors. This corresponds to the transition of the electron between the valence band and the conduction band. Basically the generation of the electron is also a transition from the valence band to the conduction band. By the way, their recombination will lead to a transition in the reverse direction.