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OE_50200: Compound Semiconductors

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OE_50200: Compound Semiconductors. Jim Y. Chi(???) ????????. National Dong-hua University, ... What is the Moor's law for Compound Semiconductor technology? ... – PowerPoint PPT presentation

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Title: OE_50200: Compound Semiconductors


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OE_50200 Compound Semiconductors Jim Y.
Chi(???) ???????? National Dong-hua
University, Hualian, Taiwan 2007. 02. 22
2
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Course reference MIT OpenCourseWare
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Outline
  • Crystal Structures
  • Bulk crystal growth
  • Band structures
  • Properties of Semiconductors Si and compounds

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  • Points to be covered in Lecture 1
  • The families (III-V's, II-VI's, IV-VI's,
    IV-IV's), Eg vs a
  • Band structures (E vs k G, L, X minima direct
    vs. indirect gaps)
  • Crystal lattices, electrical properties, optical
    properties trends in properties and the periodic
    table. The useful compounds.

7
Worldwide Semiconductor Revenue
Worldwide Compound Semiconductor Forecast
Worldwide Compound Semiconductor Revenue
BCC Inc.
Worldwide semiconductor revenue will rise to
255.7 B in 2006, up from 237 B in 2005,
according to iSuppli
8
mm
  • The number of transistors that can be
    inexpensively placed on an integrated circuit is
    increasing exponentially, doubling approximately
    every two years
  • Moore's Law describes this driving force of
    technological and social change in the late 20th
    and early 21st centuries.
  • Self-fulfilling prophecy for the industry!
  • What is the Moors law for Compound Semiconductor
    technology?
  • Whats the Post-Moores law technologies?

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Crystal Structures
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  • 4 inches are still used for MEMs and Photonic
    circuits
  • GaAs wafers are up to eight inches-one step
    behind Si

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Outline
  • Crystal Structures
  • Bulk crystal growth
  • Band structures
  • Properties of Semiconductors Si and compounds

34
Band Structures for Electrons and Holes
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Band Structures of Semiconductors Ge, Si, GaAs
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Properties of Common Semiconductors
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Bandstructure of GaN
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Direct and Indirect Bandgap
  • Because of the small momentum of photons, the
    optical transition are vertical.
  • Direct bandgap materials are more efficient light
    emitter and absorber than indirect bandgap
    material. This properties has consequence on the
    LEDs, solar cells
  • hv -gt e h
  • Si, Ge, C or their combinations are indirect
    bandgap materials.
  • III-V and III-N tend to be direct bandgap
    materials, the exceptions are GaP and AlAs

39
Band structure of Diamond Structures (sp3
hybridization)
Angular part of the atomic s and p orbitals
  • Conduction band at k0 is S-like with spherical
    symmetry and and the valence band are linear
    combination of P-like states.
  • The split-off band (SO), are due to the
    spin-obital interaction of the electrons and the
    nucleus
  • The effective mass is

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Why Si is indirect and GaAs direct?
http//www.designers-guide.org/Forum/YaBB.pl?num1
150452919
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Outline
  • Crystal Structures
  • Bulk crystal growth
  • Band structures
  • Properties of Semiconductors Si and compounds

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First - ever LED Report
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Outlines
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Si is science and GaAs is the art!!!
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Diamond and Zinc Blend Structures
  • Si, Ge, C or their combinations are indirect
    bandgap materials
  • III-V and III-N tend to be direct bandgap
    materials, the exceptions are GaP and AlAs
  • Different crystal direction will have different
    chemical and physcial properties.
  • Orientation dependent etching
  • Channeling for ion implantation and diffusion

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Hexagonal Structure -GaN
Zince Blend
Wurtzite
?- Wurzite ?- Zinc Blend
  • Wurtzite structure has one axis of the tetrahedra
    longer.
  • Wurtzite material does not have central symmetry
    leads to piezo-electric effect in the
    C-direction.
  • Miller indices of Wurtzite structure?

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Substrates for Epigrowth
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Epitaxy is the Key for Optoelectronic
Semiconductor Devices
Lattice Constants, Å
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Wavelength Range for Epitaxy Materials
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650
807
400
980
780
1310
1550
GaInAs/InP
InP
AlInGaAs/InP
GaAsSb/GaAs
InGaNAs/GaAs
GaAs
InGaAs/GaAs
hu
AlGaAs/GaAs
Hole levels
QDs
AlGaInP/GaAs
GaInN/GaN
200 400 600 800
1000 1200 1400 1600
Wavelength, nm
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  • Points to be covered in Lecture 1
  • The families (III-V's, II-VI's, IV-VI's,
    IV-IV's), Eg vs a
  • Band structures (E vs k G, L, X minima direct
    vs. indirect gaps)
  • Crystal lattices, electrical properties, optical
    properties trends in properties and the periodic
    table. The useful compounds.
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