ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University

Slides:



Advertisements
Similar presentations
Semiconductor Device Physics
Advertisements

Fundamental Concepts Crystalline: Repeating/periodic array of atoms; each atom bonds to nearest neighbor atoms. Crystalline structure: Results in a lattice.
ECE : Nanoelectronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
Semiconductor Fundamentals OUTLINE General material properties Crystal structure Crystallographic notation Read: Chapter 1.
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
PRINCIPLES OF PRODUCTION ENGINEERING
Unit Cells Let’s look at two different ways to visualize the structure of a solid.
Lecture 4 The structure of crystalline solids L e a r n i n g O b j e c t i v es outcomes: 1.Describe the difference in atomic/molecular structure between.
S PHERE P ACKING Math Day 2015 Kristin DeVleming.
© 2013 Eric Pop, UIUCECE 340: Semiconductor Electronics ECE 340 Lecture 3 Crystals and Lattices Online reference:
THE “MOST IMPORTANT” CRYSTAL STRUCTURES. NOTE!! Much of the discussion & many figures in what follows was again constructed from lectures posted on the.
ENE 311 Lecture 3. Bohr’s model Niels Bohr came out with a model for hydrogen atom from emission spectra experiments. The simplest Bohr’s model is that.
Solid State Physics (1) Phys3710
2D Packing Examples hole Answer the following questions for both packing diagrams. 1.Find the smallest unit that, if repeated, would give you the entire.
Chapter 1 The Crystal Structure of Solids Describe three classifications of solids— amorphous, polycrystalline, and single crystal. Discuss the concept.
Cubic crystals: (a) simple cubic; (b) face-centered cubic, an atom in the center of every face, and (c) body-centered cubic. Figure
Structure of Solids Objectives By the end of this section you should be able to: Calculate atomic packing factors (HW) Compare bcc, fcc and hcp crystal.
Types of Solids Three general types 1. Amorphous ― with order only within a few atomonic and molecular dimensions (Fig. (a)) 2. Polycrystalline ― with.
WEEK 2 STRUCTURE OF MATERIALS MATERIALS SCIENCE AND MANUFACTURING PROCESSES.
Structure of crystalline solids
ECE : Nanoelectronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
Solid State Physics (1) Phys3710
Chapter 1 Crystal Structures. Two Categories of Solid State Materials Crystalline: quartz, diamond….. Amorphous: glass, polymer…..
2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt Surface Area of Irregular.
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
Bravais Lattices in 2D In 2D there are five ways to order atoms in a lattice Primitive unit cell: contains only one atom (but 4 points?) Are the dotted.
An Alternative Semiconductor Definition!
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices
ECE 875: Electronic Devices
Close-packed Spheres Units cells: point and space symmetry
ECE : Nanoelectronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
Lecture 1 OUTLINE Semiconductor Fundamentals – General material properties – Crystal structure – Crystallographic notation – Electrons and holes Reading:
PH0101 UNIT 4 LECTURE 4 RECIPROCAL LATTICE
ECE : Nanoelectronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
1 Solids. 2 Structures of Solids Crystalline vs. Amorphous Crystalline solid: well-ordered, definite arrangements of molecules, atoms or ions. –Most solids.
ECE 875: Electronic Devices
ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
1 Prof. Ming-Jer Chen Department of Electronics Engineering National Chiao-Tung University 02/24/ /24/2015 DEE3517 Solid State Physics (1) Lecture.
ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
Crystal lattice structure
Lecture 1 OUTLINE Important Quantities Semiconductor Fundamentals
ECE 875: Electronic Devices
Semiconductor Fundamentals
Groups: Fill in this Table for Cubic Structures
Next time: Diffraction
Chemistry 481(01) Spring 2017 Instructor: Dr. Upali Siriwardane
Lecture 1 OUTLINE Important Quantities Semiconductor Fundamentals
Chapter 3: Solid State Chemistry Week 7
Chapter 3: Solid State Chemistry
Crystallography and Structure
Crystal Structure of Solids
ECE 874: Physical Electronics
ECE 874: Physical Electronics
3-Dimensional Crystal Structure.
Lecture 1 OUTLINE Semiconductor Fundamentals
ECE 874: Physical Electronics
ECE 875: Electronic Devices
Prof. Virginia Ayres Electrical & Computer Engineering
ECE 874: Physical Electronics
3-Dimensional Crystal Structure
3-Dimensional Crystal Structure
Prof. Virginia Ayres Electrical & Computer Engineering
Solid Crystal Structures. (based on Chap
Solid Crystal Structures. (based on Chap
Crystal Structure Acknowledgement: This slides are largely obtained from Dr.Neoh Siew Chin UniMAP on the subject Material Engineering.
Solid Crystal Structures. (based on Chap
Presentation transcript:

ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University

VM Ayres, ECE874, F12 Lecture 02, 04 Sep 12

VM Ayres, ECE874, F12 Silicon crystallizes in the diamond crystal structure Fig. 1.5 (a): Notice real covalent bonds versus definition of imaginary cubic unit cell

VM Ayres, ECE874, F12

Corners: 8 x 1/8 = 1 Faces: 6 x ½ =3 Inside: 4 x 1 =4 Atoms in the Unit cell: 8

VM Ayres, ECE874, F12 What do you need to know to answer (b)? Size of a cubic Unit cell is a 3, where a is the lattice constant (Wurtzite crystal structure is not cubic)

VM Ayres, ECE874, F12

Which pair are nearest neighbors? O-1 O-2 O-3 O 1 2 3

VM Ayres, ECE874, F12 Which pair are nearest neighbors? O-1 O-2 O-3 O a/2 x z y

VM Ayres, ECE874, F12 (1/4, ¼, ¼) is given To get this from drawing would need scale marks on the axes

VM Ayres, ECE874, F12 Which pair are nearest neighbors? O-1 O-2 O-3 O a/2 x z y

VM Ayres, ECE874, F12 Directions for fcc (like Pr. 1.1 (b)): 8 atoms positioned one at each corner. 6 atoms centered in the middle of each face.

VM Ayres, ECE874, F12 The inside atoms of the diamond structure are all the ( ¼, ¼, ¼) locations that stay inside the box:

VM Ayres, ECE874, F12 All the ( ¼, ¼, ¼) locations are:

VM Ayres, ECE874, F12 You can match all pink atoms with a blue fcc lattice, copied from slide 12:

VM Ayres, ECE874, F12 You can match all bright and light yellow atoms with a green fcc lattice copied from slide 12:

VM Ayres, ECE874, F12 Therefore: the diamond crystal structure is formed from two interpenetrating fcc lattices

VM Ayres, ECE874, F12 But only 4 of the (¼, ¼, ¼) atoms are inside the cubic Unit cell.

VM Ayres, ECE874, F12 Now let the pink atoms be gallium (Ga) and the yellow atoms be arsenic (As). This is a zinc blende lattice. Compare with Fig. 1.5 (b)

VM Ayres, ECE874, F12 Note that there are 4 complete molecules of GaAs in the cubic Unit cell.

VM Ayres, ECE874, F12 Example problem: find the molecular density of GaAs and verify that it is: 2.21 x molecules/cm 3 = the value given on page 13.

VM Ayres, ECE874, F12

Increasing numbers of important compounds crystallize in a wurtzite crystal lattice: Hexagonal symmetry Fig. 1.3 forms a basic hexagonal Unit cell Cadmium sulfide (CdS) crystallizes in a wurtzite lattice Fig. 1.6 inside a hexagonal Unit cell Wurtzite: all sides = a

VM Ayres, ECE874, F12 Example problem: verify that the hexagonal Unit cell volume is: = the value given on page 13.

VM Ayres, ECE874, F12 a a c Hexagonal volume = 2 triangular volumes plus 1 rectangular volume a 120 o

VM Ayres, ECE874, F12

a a c Hexagonal volume = 2 triangular volumes plus 1 rectangular volume a 120 o

VM Ayres, ECE874, F12 Work out the parallel planes for CdS: 3 S 7 Cd 7 S 3 Cd 3 S 7 Cd Note: tetrahedral bonding inside

VM Ayres, ECE874, F12 3 S 7 S 3 S How many equivalent S atoms are inside the hexagonal Unit cell? Define the c distance as between S-S (see Cd-Cd measure for c in Fig. 1.6 (a) )

VM Ayres, ECE874, F12 How much of each S atom is inside: Hexagonal: In plane: 1/3 inside Therefore: vertex atoms = 1/3 X 1 = 1/3 inside 6 atoms x 1/3 each = 2 Hexagonal: Interior plane Top to bottom: all inside: 1 Also have one inside atom in the middle of the hexagonal layer: 1 Total atoms from the hexagonal arrangement = 3

VM Ayres, ECE874, F12 How much of each atom is inside: Note: the atoms on the triangular arrangement never hit the walls of the hexagonal Unit cell so no 1/3 stuff. But: they are chopped by the top and bottom faces of the hexagonal Unit cell: = ½ atoms. Therefore have: 3 S atoms ½ inside on each 3-atom layer layers: = 3/2 each layer Total atoms from triangular arrangements = 2 x 3/2 = 3

VM Ayres, ECE874, F12 3 S 7 S 3 S How many equivalent S atoms are inside the hexagonal Unit cell? Total equivalent S atoms inside hexagonal Unit cell = 6 3/2 3

VM Ayres, ECE874, F12 You are required to indentify N as the Cd atoms in Fig. 1.6 (a) Pr. 1.3 plus an extra requirement will be assigned for HW:

VM Ayres, ECE874, F12 Cd  N: 7 Cd 3 Cd 7 Cd So you’ll count the numbers of atoms for the red layers for HW, with c = the distance between Cd-Cd layers as shown.