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Question

A Ge semiconductor is doped with acceptor impurity concentration of $10^{15}$ atoms/cm$^3$. For the given hole mobility of $1800 \text{ cm}^2/\text{V-s}$, the resistivity of this material is

The correct answer is
$3.472 \text{ } \Omega \text{ cm}$

Semiconductor Resistivity Calculation

The problem asks for the resistivity ($\rho$) of a Germanium (Ge) semiconductor doped with an acceptor impurity.

Given Parameters

  • Dopant Type: Acceptor (making it a p-type semiconductor)
  • Acceptor Concentration ($N_A$): $1 \times 10^{15}$ atoms/cm$^3$
  • Hole Mobility ($\mu_p$): $1800 \text{ cm}^2/\text{V-s}$
  • Elementary Charge ($q$): $1.6 \times 10^{-19} \text{ C}$

Resistivity Formula

For a p-type semiconductor, the majority charge carriers are holes. The concentration of holes ($p$) is approximately equal to the acceptor concentration ($N_A$), i.e., $p \approx N_A$. The electrical conductivity ($\sigma$) is given by:

$ \sigma = q p \mu_p $

Resistivity ($\rho$) is the reciprocal of conductivity:

$ \rho = \frac{1}{\sigma} = \frac{1}{q p \mu_p} $

Since $p \approx N_A$, the formula becomes:

$ \rho = \frac{1}{q N_A \mu_p} $

Calculation

Substitute the given values into the resistivity formula:

$ \rho = \frac{1}{(1.6 \times 10^{-19} \text{ C}) \times (1 \times 10^{15} \text{ cm}^{-3}) \times (1800 \text{ cm}^2/\text{V-s})} $

First, calculate the denominator:

$ q N_A \mu_p = (1.6 \times 10^{-19}) \times (1 \times 10^{15}) \times 1800 $

$ q N_A \mu_p = (1.6 \times 1800) \times 10^{-19+15} $

$ q N_A \mu_p = 2880 \times 10^{-4} \text{ S/cm} $

$ q N_A \mu_p = 0.2880 \text{ S/cm} $

Now, calculate the resistivity:

$ \rho = \frac{1}{0.2880 \text{ S/cm}} $

$ \rho \approx 3.4722 \text{ } \Omega \text{ cm} $

Conclusion

The calculated resistivity is approximately $3.472 \text{ } \Omega \text{ cm}$, which matches Option C.

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Important Questions from Band Theory Effective Mass Holes

  1. For the energy dispersion of an electron in a one-dimensional solid $E(k) = E_0 - 2\gamma \cos(ka)$, the ratio of the effective mass of the electron in the solid to the free electron mass ($m_e$) at $k = 0$ is $R_0$. Taking $\gamma = 0.5 \text{ eV}$ and $a = 0.5 \text{ nm}$, the value of $R_0$ (rounded off to two decimal place) is _____
    ($\hbar = 1.054 \times 10^{-34} \text{ J.s}$, $m_e = 9.1 \times 10^{-31} \text{ kg}$, electron charge $= 1.6 \times 10^{-19} \text{ C}$)
  2. The dispersion ($E(k)$) of the conduction band (CB) and valence band (VB) for a semiconductor are shown schematically in the figure. Considering the possibility of an electron making a transition from the bottom of the CB to the top of the VB, which of the following options is/are correct?

  3. For nonrelativistic electrons in a solid, different energy dispersion relations (with effective masses $m_a^*$, $m_b^*$, and $m_c^*$) are schematically shown in the plots. Which one of the following options is CORRECT?

  4. The temperature dependence of the electrical conductivity ($\sigma$) of three intrinsic semiconductors A, B and C is shown in figure. 

    Let $E_A$, $E_B$ and $E_C$ be the bandgaps of A, B and C, respectively. Which one of the following relations is correct?

  5. The energy dispersion for electrons in one dimensional lattice with lattice parameter $a$ is given by $E(k) = E_0 - \frac{1}{2} W \cos ka$, where $W$ and $E_0$ are constants. The effective mass of the electron near the bottom of the band is
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