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Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

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Page 1: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

CRYSTALSTRUCTURES

LECTURE 5(18 slides)

Page 2: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

x y

z up

Constructing an FCC crystal lattice

Note how the FCC is justifiably called cubic close-packed (CCP).

Page 3: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

x

yz up

Homework 5: A base 2-D close-packed square lattice can be found in the both the SC and FCC lattices. The 3-D extension differs,Resulting in a close-packed cubic lattice for FCC but a much lessDense SC layout. BCC is also not close-packed. Can you find, in any plane of the BCC lattice, a 2D close-packed structure? Discuss the (111) plane in this regard. What is the plane that looks closest to the one below?

x

y

Page 4: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Building an FCC lattice in an obvious way

First layer Second layer Third layer

Note: certain planesclearly show HCPpatterns.

HOME: what plane is this?

Page 5: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Diamond and Zincblende Lattices

8-atom unit cellmade from FCC 4-atom unit cell by puttinganother atom ata/4+b/4+c/4 from each FCC atom

FCC

Zincblende lattice has different species in FCC sublattices: e.g. InP, GaAs

Page 6: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Analyzing the diamond lattice

FCC

BCC

Conclusion: the octantshown is an incompleteBCC lattice pattern. Use this in one of the HW’sRegarding packing fraction

Note: 4 bondshelps explain thatC forms a diamondlattice structure

Page 7: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Our favorite nine III-V binary semiconductors form zincblende lattices

As

Ga

Basic FCC lattice of Ga

FCC lattice for As

Page 8: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Again, thanks to some popsicle sticks, some Elmer’s glue anda bunch of Marbles from Michael’s Arts and Crafts Store, a digital camera and Photoshop software

HCP starting plane – builds up, but at each plane, one can choosedifferent sites for the triad – as shown above

Hexagonal Close Packing

Page 9: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

HCP and FCC contain HCP-type planes

Hexagonal Close-Packed Cubic (FCC) Close-Packed

Top

vie

w

In fact, these lattice types have the same packing fraction.

Open (seen from above) all layers Closed within 3 layers

Page 10: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Crystalline Element Lattice Types

Reference: http://www.uis.edu/~trammel/sci/unit_cells/sld30.htm

III IV V VIII VII

BCC has 8 nearest neighbors

diamond lattices

HCP has 12 nearest neighbors

Page 11: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Streetman and Banerjee

6) 1.47) 1.78) 1.109) 1.14

Assigned Problems 5-8.

Page 12: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

CRYSTALGROWTH

Page 13: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Czolchraski Crystal Growth Method

Ref: S&BFigs. 1.10,1.11

12” diameter by 1 meter Si bouleMade by pulling seed from Si melt

seed

Page 14: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Epitaxial Growth Methods

• LPE (Liquid Phase Epitaxy) – precipitation from liquid phase onto substrate, controlled by time and temperature

• VPE (Vapor Phase Epitaxy) – fast gas flow velocity over heated substrates; surface reaction of compounds releases desired atoms• MBE (Molecular Beam Epitaxy) – for monolayer-level control of stoichiometry – beams of elements to be deposited

Reference: Mandatory reading (hand out): E. D. Jungbluth, “Crystal Growth Methods Shape Communications Lasers,” Laser Focus World, vol. 29, pp. 61-72 (Feb., 1993).

Start with suitably oriented crystal substrate – grow layers of identical (homoepitaxy) or different material (heteroepitaxy) maintaining lattice type, orientation and lattice constant.

Page 15: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Epitaxial GrowthTechnologies

Reference: Mandatory reading (will hand out): E. D. Jungbluth, “Crystal Growth Methods Shape Communications Lasers,” Laser Focus World, vol. 29, pp. 61-72 (Feb., 1993).

LPE

VPE

MBE

Page 16: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Epitaxial Growth Methods

2” dia wafer cassette

InP-based laser substrate

Reference: E. D. Jungbluth, ibid.

Reference: G. P. Agrawal

2-D Lithography and etching at these stages

Page 17: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

A superlattice of MBE-Grown Layers

Ref:S&BFig. 1.16

Alternating layersof GaAs (dark)and AlAs (light)with 4-monolayerperiodicity:

SUPERLATTICE

CBVB

Page 18: Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)

Semiconductor Electronic Devices EECS 321 Spring 2002 CWRU Prof. Dave Smith

Assignment 10.

Read. E. D. Jungbluth, “Crystal Growth Methods Shape Communications Lasers,” Laser Focus World, vol. 29, pp. 61-72 (Feb., 1993).

a) What is an acceptable substrate defect density?b) How would you hook up a DC battery to make Jungbluth’s Fig 1’s device lase? How would you convert it into a detector instead?c) Compare substrate heating techniques in the cases of LPE, VPE and MBE.d) Several different bandgap-engineered devices types are mentioned and they are more suitable for some techniques than others. Name one type suitable for each fab method and why is that method preferred? E.g.: use the figure right bottom.