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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Semiconductors and Semiconductor Devices

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Semiconductors and Semiconductor Devices

A semiconducting material possesses a band gap of 1 eV . It is...

A semiconducting material possesses a band gap of 1 eV1 \text{ eV}. It is doped with acceptor impurities that establish acceptor levels 1 meV1 \text{ meV} above the valence band. Suppose that a transition from one energy level to another is practically forbidden if kTkT is less than 1/501/50 of the energy gap. Furthermore, if kTkT exceeds twice the gap, the upper levels achieve maximum population. The temperature of the semiconductor is raised from 0 K0 \text{ K}. Initially, the hole concentration increases with temperature before becoming approximately constant. Upon further heating, the hole concentration begins to increase again at a specific temperature. Determine the approximate temperature range over which the hole concentration remains roughly constant.

Options

  1. A12 K12 \text{ K} to 11600 K11600 \text{ K}
  2. B10 K10 \text{ K} to 115 K115 \text{ K}
  3. C40 K40 \text{ K} to 460 K460 \text{ K}
  4. D20 K20 \text{ K} to 230 K230 \text{ K}

Correct answer

D. 20 K20 \text{ K} to 230 K230 \text{ K}

Step-by-step solution

The energy required to excite an electron from the valence band to the acceptor level is ΔEa=1 meV=10−3 eV\Delta E_a = 1 \text{ meV} = 10^{-3} \text{ eV}.

The acceptor levels achieve maximum population when kT1=2ΔEa=2×10−3 eVkT_1 = 2 \Delta E_a = 2 \times 10^{-3} \text{ eV}.

Using the Boltzmann constant k≈111600 eV/Kk \approx \dfrac{1}{11600} \text{ eV/K}, we get:

T1=2×10−3×11600=23.2 KT_1 = 2 \times 10^{-3} \times 11600 = 23.2 \text{ K}

At this temperature, all acceptor levels are occupied by electrons, meaning the hole concentration in the valence band reaches a constant value.

The hole concentration remains constant until electrons from the valence band start getting excited to the conduction band. The band gap is Eg=1 eVE_g = 1 \text{ eV}.

This intrinsic transition begins when kT2=150Eg=150×1 eV=0.02 eVkT_2 = \dfrac{1}{50} E_g = \dfrac{1}{50} \times 1 \text{ eV} = 0.02 \text{ eV}.

T2=0.02×11600=232 KT_2 = 0.02 \times 11600 = 232 \text{ K}

Thus, the hole concentration remains roughly constant in the temperature range of approximately 23.2 K23.2 \text{ K} to 232 K232 \text{ K}, which best matches 20 K20 \text{ K} to 230 K230 \text{ K}.
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