Question Video: Recalling the Relationship between Doped and Undoped Charge Carrier Densities | Nagwa Question Video: Recalling the Relationship between Doped and Undoped Charge Carrier Densities | Nagwa

Question Video: Recalling the Relationship between Doped and Undoped Charge Carrier Densities Physics • Third Year of Secondary School

In a doped semiconductor that is at thermal equilibrium, the density of free electrons in the semiconductor is represented by 𝑛, and the density of vacancies in the semiconductor is represented by 𝑝. The density of either free electrons or vacancies in pure silicon is represented by 𝑛ᵢ. Which of the following formulas correctly models the semiconductor? [A] 𝑝𝑛 = 𝑛_(𝑖) ^(2) [B] 𝑝𝑛 = (𝑛_𝑖)^1/2 [C] 𝑝𝑛 = 𝑛_𝑖 [D] 𝑝𝑛 = 2𝑛_𝑖 [E] 𝑝𝑛 = (𝑛_𝑖)/2

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Video Transcript

In a doped semiconductor that is at thermal equilibrium, the density of free electrons in the semiconductor is represented by 𝑛, and the density of vacancies in the semiconductor is represented by 𝑝. The density of either free electrons or vacancies in pure silicon is represented by 𝑛 sub 𝑖. Which of the following formulas correctly models the semiconductor? (A) The vacancy density times the electron density equals the undoped density squared. (B) The vacancy density times the electron density equals the undoped density to the power of one-half. (C) The vacancy density times the electron density equals the undoped density. (D) The vacancy density times the electron density equals two times the undoped density. (E) The vacancy density times the electron density equals the undoped density divided by two.

To begin, recall that in a pure semiconductor such as pure silicon, free electrons and vacancies are created in pairs, so the density of free electrons must be equal to the density of vacancies. This is why the quantity 𝑛 sub 𝑖 is capable of modeling the concentration of either free electrons or vacancies in a pure sample. If we know the undoped density equals the electron density, then because of this relationship, we also know the undoped density equals the vacancy density.

Now we wanna find out what happens when we multiply the vacancy density and the electron density and state their product in terms of the undoped density. Luckily, the math is pretty simple at this point. On the right-hand side of our formula, let’s make these two substitution, and we have 𝑛 sub i times 𝑛 sub i, or 𝑛 sub i squared. This might seem redundant in the case of a pure semiconductor, but it’s an interesting result that this formula actually holds true for any semiconductor at thermal equilibrium whether it’s pure or doped.

Recall that as we dope a semiconductor, the densities of electrons and vacancies change so that they’re no longer equal. However, they change in such a way that the quantity 𝑛 sub i squared remains constant, which makes this formula really versatile and useful.

So answer choice (A) is correct. A doped semiconductor at thermal equilibrium is correctly modeled using the formula the vacancy density times the electron density equals the undocked density squared.

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