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ElectricalElectrical Materials
PrevNext

At absolute zero temperature, an intrinsic semiconductor behaves as a

A

Conductor

B

n-type semiconductor

C

p-type semiconductor

D

insulator

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalElectrical Materials
Option D

insulator

Quick Summary:

At absolute zero temperature (0 K), an intrinsic semiconductor behaves as a perfect insulator. This is because there is insufficient thermal energy to excite electrons from the valence band to the conduction band.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

At absolute zero temperature (0 K), an intrinsic semiconductor behaves as a perfect insulator. This is because there is insufficient thermal energy to excite electrons from the valence band to the conduction band.

ЁЯФв Key Formulas

n=p=ni=A0T3/2eтИТEg2kTn = p = n_i = A_0 T^{3/2} e^{-\frac{E_g}{2kT}}n=p=niтАЛ=A0тАЛT3/2eтИТ2kTEgтАЛтАЛ тАФ intrinsic carrier concentration as a function of temperature TTT

nтЙИ0n \approx 0nтЙИ0 at T=0T = 0T=0 K тАФ no free carriers available

тЪЩя╕П Working Principle

In an intrinsic semiconductor, the Fermi level lies exactly in the middle of the forbidden energy gap. At T=0T = 0T=0 K, all valence electrons are tightly bound in covalent bonds, and the conduction band is completely empty. Since there are no free charge carriers available for conduction, the electrical conductivity is zero, making the material an ideal insulator.

ЁЯУМ Key Points
  • тЦ╕

    At 0 K, no covalent bonds are broken by thermal agitation.

  • тЦ╕

    The electrical conductivity ╧Г\sigma╧Г is directly proportional to carrier concentration.

  • тЦ╕

    The Fermi-Dirac distribution function f(E)f(E)f(E) becomes a step function at T=0T = 0T=0 K.

  • тЦ╕

    Semiconductors act as insulators at 0 K and conductors at higher temperatures.

тЬЕ Advantages
  • тЦ╕

    Useful for creating thermally stable electronic components at cryogenic temperatures.

  • тЦ╕

    Fundamental for understanding the temperature dependence of resistivity.

тЭМ Disadvantages / Limitations
  • тЦ╕

    No current flow possible at this state.

  • тЦ╕

    Not useful for practical device switching at 0 K.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Cryogenic sensors

  • тЦ╕

    Superconducting research

  • тЦ╕

    Theoretical condensed matter physics

ЁЯУД Additional Information
  • тЦ╕

    The forbidden energy gap EgE_gEgтАЛ prevents charge carriers from reaching the conduction band without thermal excitation.

  • тЦ╕

    Option A is incorrect because conductivity requires free electrons.

  • тЦ╕

    Options B and C are incorrect as they refer to extrinsic semiconductor properties which are absent at 0 K.

ЁЯУК Diagram / Illustration
Conduction Band(Empty at 0 K)Valence Band(Completely filled)E_g
тЬЕ

D is correct тАФ At absolute zero, all valence electrons are bound in covalent bonds, leaving the conduction band empty and resulting in zero conductivity.

Core Concepts Used
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Band Theory of Solids Intrinsic Semiconductors Fermi-Dirac Statistics
ЁЯТб EXAM TIP

Remember that conductivity in semiconductors increases with temperature (negative temperature coefficient), which is the exact opposite of metallic conductors.

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