Solid-state materials and band theory — match each item to its band-structure characteristic List I (Material / dopant) A. Copper (a good conductor) B. Rubber (an electrical insulator) C. Antimony doped into Si/Ge (Group V donor) D. Boron doped into Si/Ge (Group III acceptor) List II (Band-structure effect) 1. Produces a discrete energy level just above the valence band (acceptor level) 2. Produces a discrete energy level just below the conduction band (donor level) 3. Large forbidden energy gap (typical of insulators) 4. Valence and conduction bands overlap (typical of good conductors)

Electronics and Communication Engineering Matching Questions Difficulty: Easy
Choose an option
  • A
    A-4, B-3, C-2, D-1
  • B
    A-4, B-1, C-2, D-3
  • C
    A-3, B-4, C-2, D-1
  • D
    A-4, B-3, C-1, D-2

Answer

Correct Answer: A-4, B-3, C-2, D-1

Explanation

Introduction / Context:This matching question tests fundamental solid-state physics as used in electronics: how intrinsic materials and dopants shape band structures and hence conductivity. Conductors, insulators, and doped semiconductors can be recognized by simple band diagrams and the placement of donor/acceptor energy levels relative to the conduction and valence bands.

Given Data / Assumptions:

  • Copper represents a metallic conductor.
  • Rubber represents an insulating polymer with a large band gap.
  • Antimony (Sb, Group V) acts as a donor in Si/Ge.
  • Boron (B, Group III) acts as an acceptor in Si/Ge.

Concept / Approach:In metals, the valence and conduction bands overlap or a partially filled band exists, so electrons move freely. Insulators show a large forbidden gap between valence and conduction bands, limiting carrier excitation. In semiconductors, doping introduces discrete energy levels: donors (Group V) add levels just below the conduction band; acceptors (Group III) add levels just above the valence band, easing promotion of carriers with modest thermal energy.

Step-by-Step Solution:

Copper → overlapping bands → maps to statement 4.Rubber → large forbidden gap → maps to statement 3.Antimony (donor) → discrete level just below E_c → maps to statement 2.Boron (acceptor) → discrete level just above E_v → maps to statement 1.

Verification / Alternative check:Introductory band diagrams for metals, insulators, and doped semiconductors consistently show these placements. Device physics texts use the same donor/acceptor level locations to explain n-type and p-type behavior and the ease of thermal ionization at room temperature.

Why Other Options Are Wrong:

  • Assigning rubber to donor/acceptor levels confuses intrinsic insulation with doped semiconductor behavior.
  • Placing “overlap” on rubber or dopants contradicts their basic roles.
  • Swapping donor/acceptor positions in energy band diagrams reverses n-type vs p-type physics.

Common Pitfalls:Mixing up “discrete level near E_c” (donor) and “near E_v” (acceptor); assuming all good conductors simply have tiny gaps rather than true band overlap; forgetting that polymers like rubber are wide-gap insulators.

Final Answer:A-4, B-3, C-2, D-1

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