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Introduction to Materials Science and Engineering
Chapter 10: Electrical Properties Textbook Chapter 19
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Content Introduction Electrical Conduction Semiconductivity
Electrical Conduction in Ionic Ceramics and in Polymers 5. Dielectric Behavior Other Electrical Characteristics of Materials Electronic Devices and Fabrication
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Introduction ISSUES TO ADDRESS...
• How are electrical conductance and resistance characterized? • What are the physical phenomena that distinguish conductors, semiconductors, and insulators? • For metals, how is conductivity affected by imperfections, temperature, and deformation? • For semiconductors, how is conductivity affected by impurities (doping) and temperature?
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Content Introduction Electrical Conduction Semiconductivity
Electrical Conduction in Ionic Ceramics and in Polymers 5. Dielectric Behavior Other Electrical Characteristics of Materials Electronic Devices and Fabrication
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View of an Integrated Circuit
• Scanning electron microscope images of an IC: • A dot map showing location of Si (a semiconductor): --Si shows up as light regions. • A dot map showing location of Al (a conductor): --Al shows up as light regions.
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Electrical Conduction
Ohm’s Law
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Electrical Conductivity
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Important Unit
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Electronic vs. Ionic charge carrier electron (e=1.602x10-19 C)
electron/hole cation anion
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Energy Band:
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Band Structure of Solids
Valence band - The energy levels filled by electrons in their lowest energy states. Conduction band - The unfilled energy levels into which electrons can be excited to provide conductivity. Holes - Unfilled energy levels in the valence band. Because electrons move to fill these holes, the holes move and produce a current. Energy gap (Bandgap) - The energy between the top of the valence band and the bottom of the conduction band that a charge carrier must obtain before it can transfer a charge.
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Energy Band
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Formation of Energy Band
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Energy Band of Na
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Metal, Semiconductor, Insulator
Metal Insulator Semiconductor Ex) Cu (3d104s1) Mg(3s2) > 2eV < 2eV
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Energy band for Conductor
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Conduction in terms of Band and Atomic Bonding Models
metals insulators and semiconductors
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Electron Mobility Drift Velocity
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Electron Mobility conductivity For metals
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Electrical Resistivity of Metals
thermal scattering impurity scattering defect scattering
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Electrical Resistivity of Metals
temperature impurities
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Content Introduction Electrical Conduction Semiconductivity
Electrical Conduction in Ionic Ceramics and in Polymers 5. Dielectric Behavior Other Electrical Characteristics of Materials Electronic Devices and Fabrication
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Semiconductor Intrinsic semiconductor - A semiconductor in which properties are controlled by the element or compound that makes the semiconductor and not by dopants or impurities. Extrinsic semiconductor - A semiconductor prepared by adding dopants, which determine the number and type of charge carriers. Doping - Deliberate addition of controlled amounts of other elements to increase the number of charge carriers in a semiconductor. Thermistor - A semiconductor device that is particularly sensitive to changes in temperature, permitting it to serve as an accurate measure of temperature. Radiative recombination - Recombination of holes and electrons that leads to emission of light; this occurs in direct bandgap materials.
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Intrinsic Semiconductors
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Intrinsic Semiconductors
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Intrinsic Semiconductors
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Intrinsic Semiconductors
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Intrinsic Semiconductors
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Extrinsic Semiconductors
• Intrinsic: # electrons = # holes (n = p) • Extrinsic: --n ≠ p • N-type Extrinsic: (n >> p) • P-type Extrinsic: (p >> n)
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N-type Semiconductors
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N-type Semiconductors
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N-type Semiconductors
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P-type Semiconductors
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P-type Semiconductors
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P-type Semiconductors
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Temperature Dependence of Mobility
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Temperature Dependence of Mobility
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Hall Effect B=1kG wc=2.8GHz
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Hall Effect
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Hall Effect
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Semiconductor Devices
p-n junction
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Semiconductor Devices
transistor
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Semiconductor Devices
Junction transistor MOSFET
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Growth of Si crystal
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IC Fabrication Process
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Content Introduction Electrical Conduction Semiconductivity
Electrical Conduction in Ionic Ceramics and in Polymers 5. Dielectric Behavior Other Electrical Characteristics of Materials Electronic Devices and Fabrication
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Ionic Conduction nI: charge of ions
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Conducting Polymer temperature dependence of the conductivity
similar to that of semiconductor polymer- semicrystalline require modification of band model polyacetylene-prototype of a conducting polymer (conjugated organic polymer-alternating single and double bonds between carbons)
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Conducting Polymer conductivity
p-electrons in the double bond act as a carrier
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Content Introduction Electrical Conduction Semiconductivity
Electrical Conduction in Ionic Ceramics and in Polymers 5. Dielectric Behavior Other Electrical Characteristics of Materials Electronic Devices and Fabrication
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Dielectric Capacitance Capacitance ( ,F) e0:permittivity of a vacuum
e:permittivity of the medium er:relative permittivity (dielectric constant) where, e=ere0
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Polarization Electric dipole moment
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dielectric displacement
Polarization Surface charge density D, or quantity of charge per unit area is expressed as, (C/m2) dielectric displacement dipole
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Polarization ©2003 Brooks/Cole, a division of Thomson Learning, Inc. Thomson Learning™ is a trademark used herein under license.
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Types of Polarization Electronic Polarization (Pe)
Ionic Polarization (Pi) Orientation Polarization (Po)
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Frequency Response Dielectric Strength Dielectric Materials
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Content Introduction Electrical Conduction Semiconductivity
Electrical Conduction in Ionic Ceramics and in Polymers 5. Dielectric Behavior Other Electrical Characteristics of Materials Electronic Devices and Fabrication
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Ferroelectricity BaTiO3 Rochelle salt(NaKC4H4O6·4H2O) KH2PO4 KNbO3 PZT
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Piezoelectricity PbZrO3 NH4H2PO4 Quartz
©2003 Brooks/Cole, a division of Thomson Learning, Inc. Thomson Learning™ is a trademark used herein under license.
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Summary • Electrical conductivity and resistivity are:
-- material parameters. -- geometry independent. • Electrical resistance is: -- a geometry and material dependent parameter. • Conductors, semiconductors, and insulators... -- differ in accessibility of energy states for conductance electrons. • For metals, conductivity is increased by -- reducing deformation -- reducing imperfections -- decreasing temperature. • For pure semiconductors, conductivity is increased by -- increasing temperature -- doping (e.g., adding B to Si (p-type) or P to Si (n-type).
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