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Question #43790
The Question
Consider an n-type semiconductor at a low temperature (in the freeze-out regime) doped with a donor concentration . The donor electrons can be modeled as quasi-hydrogen atoms. The semiconductor has a relative permittivity and an effective electron mass . The ionization energy of a free hydrogen atom is , and the free electron mass is . In this regime, the conduction electron concentration is given by , where is the donor ionization energy and is the effective density of states in the conduction band. Assume and the electron mobility due to ionized impurity scattering scales as . Which of the following expressions correctly represents the temperature coefficient of resistivity, , of this semiconductor?
Options
- A.
- B.
- C.
- D.
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Correct Answer
Step-by-Step Solution
Explanation
How the Examiner Thinks
Multi-Concept_Bridge
Master problems that require linking physics and math concepts to solve complex competitive questions.
Concepts Behind This Question
Energy Level Scaling|Law of Mass Action|Temperature Coefficient (Alpha)
Why This Question Is Tricky
Common Mistakes
This question tests the integration of quantum energy level scaling with macroscopic transport properties and the Law of Mass Action.
Students must first correctly scale the Bohr model for a donor impurity using effective mass and dielectric constant.
The primary trap lies in the temperature coefficient calculation: students often memorize as a constant or calculate it for conductivity instead of resistivity (missing the overall negative sign).
Furthermore, they must correctly apply the square root from the Law of Mass Action to the temperature dependence of the effective density of states (), and combine it with the mobility temperature dependence to find the true scaling of resistivity before differentiating.
Quick Facts About This Question
Question Information
| Subject | Physics |
| Chapter | Atoms - Class 12 |
| Concept | Energy Level Scaling |
| Difficulty | 8 |
| Cognitive Load | 7 |
| Target Solve Time | 160 sec |
| Access | Free |