The Architecture of Conduction: Band Theory and Semiconductors

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Vocabulary flashcards covering band theory, band gaps, thermal effect paradoxes, n-type and p-type semiconductor doping, and semiconductor junctions.

17 Terms

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<p>Diamond Structure</p>

Diamond Structure

A crystalline structure where each carbon atom forms four covalent bonds with four neighboring carbon atoms, creating a rigid tetrahedral framework.

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<p>Continuous Energy Bands</p>

Continuous Energy Bands

A continuous spectrum of allowed electron energy states formed when a large number of discrete atomic orbitals merge together as atoms assemble into a solid lattice (scaling up to 102310^{23} atoms).

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Valence Band

The lower, filled energy band in a solid material where electrons are anchored to their parent atoms.

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Conduction Band

The upper, normally empty energy band in a solid material that provides an open highway for the free movement of electrons.

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Band Gap

The forbidden energy zone situated between the valence band and the conduction band that electrons must jump across for electrical conduction to occur.

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Insulator Band Gap

A massive energy gap (such as 530530\,kJ/mol\text{kJ/mol} in diamond) that thermal energy cannot breach, trapping electrons in the valence band and preventing electrical flow.

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Semiconductor Band Gap

A small energy gap (such as 106106\,kJ/mol\text{kJ/mol} in silicon) that allows a small amount of thermal or external energy to promote electrons into the conduction band.

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Metal Conduction Band Gap

A band structure with zero gap where the valence band and conduction band overlap, allowing electrons to flow freely.

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Thermal Effect on Metal Conductivity

As temperature increases (from 750750\,K\text{K} to 15001500\,K\text{K}), thermal energy increases atomic vibrations in metals like tungsten, causing collisions that slow net electron motion and reduce conductivity.

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Thermal Effect on Semiconductor Conductivity

As temperature increases (from 750750\,K\text{K} to 15001500\,K\text{K}), heat provides kinetic energy that promotes more electrons across the band gap into the conduction band, increasing semiconductor conductivity.

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Doping

The process of deliberately injecting specific elemental impurities into a semiconductor (like Group 14 silicon) to precisely alter its electrical properties without changing its structural integrity.

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<p>n-Type Doping</p>

n-Type Doping

A doping process that adds an element with more valence electrons (such as phosphorus) to supply extra negative charge carriers and create a donor level near the conduction band.

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Donor Level

An energy level introduced near the empty conduction band via n-type doping, allowing donor electrons to easily jump into the conduction band.

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<p>p-Type Doping</p>

p-Type Doping

A doping process that adds an element with fewer valence electrons (such as gallium) to create an acceptor level, leaving positive electron holes in the valence band.

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Acceptor Level

An energy level created just above the valence band via p-type doping that accepts valence electrons, producing positive holes.

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Electron Holes

Positive charge carriers generated in the valence band during p-type doping that conduct electricity via a bucket-brigade mechanism as adjacent electrons shift to fill them.

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Transistor

A microscopic switch formed by joining n-type and p-type semiconductor materials at junctions, which executes logic functions in digital devices.