Bio-Microsystems 고려대학교 Center for MNB Sensor Technology Nam Ki Min 02-3290-3991

Slides:



Advertisements
Similar presentations
Semiconductor Device Physics
Advertisements

Electronics.
Conduction in Metals Atoms form a crystal Atoms are in close proximity to each other Outer, loosely-bound valence electron are not associated with any.
Energy Band View of Semiconductors Conductors, semiconductors, insulators: Why is it that when individual atoms get close together to form a solid – such.
Lecture 2 OUTLINE Semiconductor Basics Reading: Chapter 2.
P461 - Semiconductors1 Semiconductors Filled valence band but small gap (~1 eV) to an empty (at T=0) conduction band look at density of states D and distribution.
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Semiconductor Physics (Physique des semi-conducteurs)
Lecture #3 OUTLINE Band gap energy Density of states Doping Read: Chapter 2 (Section 2.3)
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;
Lecture 3. Intrinsic Semiconductor When a bond breaks, an electron and a hole are produced: n 0 = p 0 (electron & hole concentration) Also:n 0 p 0 = n.
An Introduction to Semiconductor Materials
SEMICONDUCTOR PHYSICS. BAND THEORY OF SOLIDS  Ge and Si are pure semiconductors  Electronic configuration of Si is  1S 2, 2S 2, 2P 6, 3S 2, 3P 2.
SEMICONDUCTORS.
Lecture 2 OUTLINE Important quantities Semiconductor Fundamentals (cont’d) – Energy band model – Band gap energy – Density of states – Doping Reading:
SEMICONDUCTORS Semiconductors Semiconductor devices
Semiconductor Devices 22
Electronics Principles & Applications Sixth Edition Chapter 2 Semiconductors (student version) ©2003 Glencoe/McGraw-Hill Charles A. Schuler.
OBJECTIVE Objective of this practical is to learn about diode and identify its terminals.
Semiconductor Fundamentals. Objectives –After completing this unit, the student should be able to: Identify materials that act as semiconductors. Define.
INTRODUCTION TO SEMICONDUCTORS MATERIAL Chapter 1 (Week 2)
Chapter 2 Semiconductor Materials and Diodes
ECE 250 – Electronic Devices 1 ECE 250 Electronic Device Modeling.
Taklimat UniMAP Universiti Malaysia Perlis WAFER FABRICATION Hasnizah Aris, 2008 Lecture 2 Semiconductor Basic.
Impurities & Defects, Continued More on Shallow Donors & Acceptors Amusing Answers to Exam Questions Given by Public School Students!
McGraw-Hill © 2013 The McGraw-Hill Companies, Inc. All rights reserved. 2-1 Electronics Principles & Applications Eighth Edition Chapter 2 Semiconductors.
By Squadron Leader Zahid Mir CS&IT Department, Superior University PHY-BE -03 Semiconductors (Continued)
ECE 340 Lecture 6 Intrinsic Material, Doping, Carrier Concentrations
BASIC ELECTRONICS Module 1 Introduction to Semiconductors
LECTURE OUTLINE Electronic Properties 2 Electronic Properties 2.
Extrinsic Semiconductors ECE Definitions Intrinsic ▫Pure ▫There are an equal number of electrons and holes Extrinsic ▫Contains impurities (donors,
1 EE 2 Fall 2007 Class 9 slides. 2 Outline 1.Review of last class 2.Extrinsic semiconductors 3.Donor and acceptor impurities 4.Majority and minority carries.
Lecture 1 OUTLINE Semiconductors, Junction, Diode characteristics, Bipolar Transistors: characteristics, small signal low frequency h-parameter model,
Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
Silicon.  Occurs as silica (SiO 2 ) & other silicates.  Hard & Brittle.
Properties of metals Metals (75% of elements) Lustrous (reflect light)
CANKAYA UNIVERSITY ECE-246 Fundamental of Electronics
President UniversityErwin SitompulSDP 2/1 Dr.-Ing. Erwin Sitompul President University Lecture 2 Semiconductor Device Physics
Introduction to Semiconductors CSE251. Atomic Theory Consists of Electron, proton, neutron Electron revolve around nucleus in specific orbitals/shells.
INTRODUCTION TO SEMICONDUCTORS
INTRINSIC SEMICONDUCTOR  A pure semiconductor.  Its conductivity is low.  It has thermally generated current carries.  Examples of pure or intrinsic.
Manipulation of Carrier Numbers – Doping
© Electronics ECE 1312 EECE 1312 Chapter 2 Semiconductor Materials and Diodes.
Operational Amplifier
“Semiconductor Physics”
Today’s objectives- Semiconductors and Integrated Circuits
Lecture 2 OUTLINE Important quantities
Impurities & Defects, Continued More on Shallow Donors & Acceptors
N-TYPE AND P-TYPE SEMICONDUCTORS
Manipulation of Carrier Numbers – Doping
Introduction to Semiconductors
Read: Chapter 2 (Section 2.3)
EECS143 Microfabrication Technology
Lecture 2 OUTLINE Semiconductor Fundamentals (cont’d)
Semiconductor Fundamentals
Electronic Devices & Circuits
Basic Semiconductor Physics
Fouad N. Ajeel Lecture 1, Slide 1 Second class– semester 1 College of Science University of Sumer Analog Electronics Second class: semester 1.
Electronic Fundamental Muhammad Zahid
Electronic Circuits-1(CNET-112) Level 4th Department of CNET
ECE 340 Lecture 6 Intrinsic Material, Doping, Carrier Concentrations
Impurities & Defects, Continued More on Shallow Donors & Acceptors
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Lecture 1 OUTLINE Basic Semiconductor Physics Reading: Chapter 2.1
Types of Semiconductor Materials By Dr
ELECTRICAL PROPERTIES
Solid State Electronics ECE-1109
Ashutosh Barua ECE - ASET
Unit-2 Dr.A.L.Jerald Antony Raj, M.Sc.,M.Ed.,M.Phil(Che).,M.Phil(Edn).,Ph.D.,NET.,D.Acu Associate Professor, Pope John Paul II College of Education.
Presentation transcript:

Bio-Microsystems 고려대학교 Center for MNB Sensor Technology Nam Ki Min

Microfabrication 민 남 기민 남 기 Chapter 2

What is Microfabrication ?

고려대학교 Center for MNB Sensor Technology 4 What is Microfabrication? Historically the earliest micromanufacturing was used for semiconductor devices in integrated circuit fabrication and these processes have been covered by the term "semiconductor device fabrication," "semiconductor manufacturing," etc. Practical advances in MEMS and other nanotechnology, where the technologies from IC fabrication are being re-used, adapted or extended have led to the extension of the scope and techniques of microfabrication. Microfabrication (or micromanufacturing) is the design and creation of devices whose size can be measured in micrometers(10 -6 meters) or microns. Microfabrication typically uses methods and techniques developed by the semiconductor industry for creating IC, as well as new processes developed specifically for MEMS.

고려대학교 MNB Sensor Lab 5 What is Microfabrication? IC MESM

고려대학교 MNB Sensor Lab 6 Basic Microfabrication Steps

What are Semiconductors ?

Korea University MNB Sensor Lab 8 What are Semiconductors ? A group of materials having conductivities between those of metals and insulators. InsulatorConductor Semiconductor Very sensitive to temperature and light. Extremely minute traces of impurity atoms (routinely less than one atom per 10 9 Si atoms) can have a drastic effect on the electrical properties of semiconductors.  Semiconductor Properties

Korea University MNB Sensor Lab What are Semiconductors ?  General classifications of semiconductors Elemental semiconductors - Si(Silicon), Ge(Germanium) Compound semiconductors - IV-IV : SiC - III-V : GaAs(Gallium arsenide), GaN(Gallium nitride) - II-VI : ZnO(Zinc Oxide) - IV-VI : PbS(Lead sulfide), PbSe(Lead selenide) Alloys - Binary : Si 1-x Ge x - Ternary : Al x Ga 1-x As

Korea University MNB Sensor Lab 10  Atomic structure +14 Atomic core Valence electrons Silicon

Korea University MNB Sensor Lab 11  Covalent bond Si Shared electrons Silicon

Korea University MNB Sensor Lab 12  Silicon crystal Si Silicon

Korea University MNB Sensor Lab 13  Energy Levels : Hydrogen  Energy band EnEn eV eV eV 0 eV n=1 n=2 n=o o n=3 +1 n=1 n=2 n=3 Silicon

Korea University MNB Sensor Lab 14 (a)The splitting of the energy levels when two atoms are brought together. (b) The splitting when six atoms are brought together.  Energy band formation Silicon

Korea University MNB Sensor Lab 15 (c) If we consider the total number of atoms (N=10 23 atoms/cm 3 ), we find a very large number of levels (determined by N) spaced within the width ΔE, so the levels may be regard as a continuous band of energy levels. Silicon

Korea University MNB Sensor Lab 16  Energy band formation Silicon

Korea University MNB Sensor Lab 17  Silicon energy band Band Model Si Conduction band (Empty of electrons at T=0 K) Electron energy Valence band (Full of electrons at T=0 K) Band Model Bonding Model Silicon

Korea University MNB Sensor Lab 18 Carrier Generation in Semiconductors At T>0K, a few valence band electrons may gain enough thermal energy to break the covalent bond. Free electron Hole Conduction band Valence band Si Band Model Bond Model

Korea University MNB Sensor Lab 19 Electrical Conduction in Semiconductors Both electrons and holes contribute electric current in a semiconductor.

Korea University MNB Sensor Lab 20 Electrical Conduction in Semiconductors Current density and Conductivity semiconductor metal

Korea University MNB Sensor Lab 21 The techniques of adding controlled amounts of impurity atoms to a semiconductor material in order to change its conductivity. -Pentavalent impurity (5 valence electron) : P, As, Sb -Trivalent impurity (3 valence electron ) : B, Ga, Al Extrinsic (Impurity) Semiconductors  Doping of Semiconductor

Korea University MNB Sensor Lab 22 The addition of pentavalent impurity contributes free electrons, greatly increasing the conductivity of the intrinsic semiconductor. Extrinsic (Impurity) Semiconductors  N-type Semiconductor Si free electron P Si

Korea University MNB Sensor Lab 23 This type of impurity atom donates an electron to the conduction band and so is called a donor impurity atom. The resulting material is referred to as an n-type semiconductor. P Si Free electron generated by donor ionization Donor ions Free electrons Donor level Extrinsic (Impurity) Semiconductors

Korea University MNB Sensor Lab 24 The addition of trivalent impurity to an intrinsic semiconductor creates deficiencies of valence electrons, called "holes".  P-type Semiconductor Extrinsic (Impurity) Semiconductors Si hole B Si

Korea University MNB Sensor Lab 25 The group III atom accepts an electron from the valence band and so is referred to as an acceptor impurity atom. This type of semiconductor material is referred to as a p-type material. What are Semiconductors? B Si hole generated by acceptor ionization Acceptor ions Acceptor level

Korea University MNB Sensor Lab 26 Intrinsic n-type p-type n : electron p: hole n i =intrinsic carrier concentration n : majority carrier : p p : minority carrier : n  Summary n = p n >>p n <<p What are Semiconductors?