Ch.1 Introduction Optoelectronic devices: - devices deal with interaction of electronic and optical processes Solid-state physics: - study of solids, through.

Slides:



Advertisements
Similar presentations
Semiconductor Devices 21
Advertisements

Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com.
Another “Periodic” Table!. Growth Techniques Ch. 1, Sect. 2, YC Czochralski Method (LEC) (Bulk Crystals) –Dash Technique –Bridgeman Method Chemical Vapor.
Semiconductor Device Physics
Electronics.
Department of Electronics Introductory Nanotechnology ~ Basic Condensed Matter Physics ~ Atsufumi Hirohata.
CHAPTER 3 Introduction to the Quantum Theory of Solids
Chapter 1 The Crystal Structure of Solids Describe three classifications of solids— amorphous, polycrystalline, and single crystal. Discuss the concept.
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Lecture #14 ANNOUNCEMENTS OUTLINE Reading
1 Motivation (Why is this course required?) Computers –Human based –Tube based –Solid state based Why do we need computers? –Modeling Analytical- great.
Dr. Jie ZouPHY Chapter 43 Molecules and Solids.
Semiconductor Physics (Physique des semi-conducteurs)
Lecture #3 OUTLINE Band gap energy Density of states Doping Read: Chapter 2 (Section 2.3)
9. Semiconductors Optics Absorption and gain in semiconductors Principle of semiconductor lasers (diode lasers) Low dimensional materials: Quantum wells,
Lecture Jan 31,2011 Winter 2011 ECE 162B Fundamentals of Solid State Physics Band Theory and Semiconductor Properties Prof. Steven DenBaars ECE and Materials.
Lecture 2 OUTLINE Semiconductor Fundamentals (cont’d) – Energy band model – Band gap energy – Density of states – Doping Reading: Pierret , 3.1.5;
INTEGRATED CIRCUITS Dr. Esam Yosry Lec. #5.
Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc
Semiconductor Devices 22
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Figure 10.1 Schematic Representations of the Three States of Matter.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Intermolecular Forces Forces between (rather than within) molecules.  dipole-dipole.
1. Crystal Properties and Growth of Semiconductors
MSE 576 Thin Films 1 of xx Molecular Beam Epitaxy 09/26/2008 MSE 576: Thin Films Deepak Rajput Graduate Research Assistant Center for Laser Applications.
Yoon kichul Department of Mechanical Engineering Seoul National University Multi-scale Heat Conduction.
Carrier Mobility and Velocity
M.H.Nemati Sabanci University
John E. McMurry Robert C. Fay Lecture Notes Alan D. Earhart Southeast Community College Lincoln, NE General Chemistry: Atoms First Chapter 10 Liquids,
Chapter 10 Liquids and Solids Intermolecular Forces Forces between (rather than within) molecules.  dipole-dipole attraction: molecules with dipoles orient.
ECE 250 – Electronic Devices 1 ECE 250 Electronic Device Modeling.
ECEE 302 Electronic Devices Drexel University ECE Department BMF-Lecture Page -1 Copyright © 2002 Barry Fell 23 September 2002 ECEE 302: Electronic.
Crystal Growth Techniques
Basic Electronics By Asst Professor : Dhruba Shankar Ray For B.Sc. Electronics Ist Year 1.
ME 381R Fall 2003 Micro-Nano Scale Thermal-Fluid Science and Technology Lecture 3: Microstructure of Solids Dr. Li Shi Department of Mechanical Engineering.
Solid-State Electronics
Impurities & Defects, Continued More on Shallow Donors & Acceptors Amusing Answers to Exam Questions Given by Public School Students!
English ability would save life English ability gives you opportunities e.g. Job opening in TSMC
ECE 340 Lecture 6 Intrinsic Material, Doping, Carrier Concentrations
Computational Solid State Physics 計算物性学特論 第3回
ELECTRON AND PHONON TRANSPORT The Hall Effect General Classification of Solids Crystal Structures Electron band Structures Phonon Dispersion and Scattering.
Reminders Quiz#2 and meet Alissa and Mine on Wednesday –Quiz covers Bonding, 0-D, 1-D, 2-D, Lab #2 –Multiple choice, short answer, long answer (graphical.
Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)
EE105 - Spring 2007 Microelectronic Devices and Circuits
Many solids conduct electricity
Thin Film Deposition. Types of Thin Films Used in Semiconductor Processing Thermal Oxides Dielectric Layers Epitaxial Layers Polycrystalline Silicon Metal.
President UniversityErwin SitompulSDP 2/1 Dr.-Ing. Erwin Sitompul President University Lecture 2 Semiconductor Device Physics
Nanoelectronics Chapter 5 Electrons Subjected to a Periodic Potential – Band Theory of Solids
Semiconductor Conductivity Ch. 1, S It is well-known that in semiconductors, there are Two charge carriers! Electrons  e - & Holes  e + What is a hole?
Introduction to Semiconductors CSE251. Atomic Theory Consists of Electron, proton, neutron Electron revolve around nucleus in specific orbitals/shells.
LECTURE 5 BASICS OF SEMICONDUCTOR PHYSICS. SEMICONDUCTOR MATERIALS.
A semiconductor material cannot be viewed as a collection of non interacting atoms, each with its own individual energy levels. Because of the proximity.
Overview of Silicon Device Physics
Deposition Techniques
Chapter Energy Bands and Charge Carriers in Semiconductors
Conductivity, Energy Bands and Charge Carriers in Semiconductors
“Semiconductor Physics”
Today’s objectives- Semiconductors and Integrated Circuits
Lecture 2 OUTLINE Important quantities
Introduction to Semiconductors
Another “Periodic” Table!
Read: Chapter 2 (Section 2.3)
Atomic Picture of Crystal Surfaces
EECS143 Microfabrication Technology
Lecture 2 OUTLINE Semiconductor Fundamentals (cont’d)
Basic Semiconductor Physics
Semiconductor crystals
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Lecture 1 OUTLINE Basic Semiconductor Physics Reading: Chapter 2.1
Epitaxial Deposition
Presentation transcript:

Ch.1 Introduction Optoelectronic devices: - devices deal with interaction of electronic and optical processes Solid-state physics: - study of solids, through methods such as quantum mechanics, crystallography, electromagnetism and metallurgy Elemental semiconductors: - Si, Ge,..etc. - indirect bandgap, low electric-optics conversion efficiency Compound semiconductors - III-V (e.g. GaN, GaAs), II-VI - direct bandgap, high electric-optics conversion efficiency GaAs, InP - higher mobility than Si, Ge, - energy band gap, Eg: 1.43 (GaAs), 1.35 (InP) - most common substrate, used to grow up compound semiconductors

Periodic Table

Band structure Band structure: - results of crystal potential that originates from equilibrium arrangement of atoms in lattice - directed from potential model and electron wave equation (Schrodinger equation) time-dependent Schrodinger equation E: electron energy, φ:wave equation, m: electron mass, ħ: Plank constant

Electron energy band diagram v.s. wave number

Energy bandgap v.s. lattice constant

Bonding in solids Van der Waals bonding: formation of dipoles between atoms and their electrons e.g.: inert gas, like Ar Ionic bonding: electron exchange between atoms produces positive and negative ions which attract each other by Coulomb-type interactions e.g. NaCl, KCl covalent bonding sharing of electrons between neighboring atoms e.g.: elemental and compound semiconductors Metallic bonding: valence electrons are shared by many atoms (bonding not directional, electron free or nearly free contributed to conductivity) e.g.: Zn

Body-Centered Cubic (BCC) structure e.g. iron, chromium, tungsten, niobium

Face-Centered Cubic (FCC) structure e.g.: aluminum, copper, gold, silver

Diamond Cubic (FCC) structure

Zincblende structure Diamond structure, Zincblende structure e.g.: aluminum, GaAse.g.: Si, Ge

Atomic arrangement in different solids

Dislocation & strain Dislocation occurs if - epitaxial layer thickness > h c (critical thickness), or - epitaxial layer thickness < h c, but with large mismatch Strain occurs if - epitaxial layer thickness < hc, and with small mismatch

Strain semiconductor a) lattice match b) compressive strain c) tensile strain Strain offer flexibility for restriction of lattice mismatch

Crystal Growth Bulk growth: - furnace growth - pulling technique Epitaxial growth: - Liquid Phase Epitaxy (LPE) - Vapor Phase Epitaxy (VPE), or termed Chemical Vapor Deposition (CVD) - Molecular Beam Epitaxy (MBE)

Epitaxy epi means “above” taxis means “in order manner” epitaxy can be translated to “to arrange upon” with controlled thickness and doping subtract acts as a seed crystal, deposited film takes on a lattice structure and orientation identical to the subtract different from thin film deposition that deposit polycrystalline or amorphous film - homoepitaxy: epi and subtract are with the same material epi layer more pure than subtract and have different doping level - hetroepitaxy: used for - Si-based process for BJT and CMOS, or - compound semiconductors, such as GaAs

Epitaxy Material Growth Methods Liquid Phase Epitaxy Vapor Phase Epitaxy (VPE), or termed Chemical Vapor Deposition (CVD) - formation of condensed phase from gas of different chemical composition - distinct from physical vapor deposition (PVD) such as sputtering, e-beam deposition, MBE (condensation occurs without chemical change) - gas stream through a reactor and interact on a heated subtract to grow epi layer Molecular Beam Epitaxy

Doping of Semiconductors Intrinsic materials: undoped - Undoped materials by epitaxy technology have more carriers than in intrinsic material. e.g. GaAs: /cm 3 (instrinsic carrier concentration: 1.8x10 6 /cm 3 ) - impurity comes from source materials, carrier gases, process equipment, or subtract handle Extrinsic materials: - n-type: III sub-lattice of III-V compound is substituted by V elements: impurity terms “donor” - p-type: V sub-lattice of III-V compound is substituted by III elements: impurity terms “acceptor”

Optical fiber - lowest loss at 1.55 um - lowest dispersion” 1.3 um

Energy band theory