Copyright © Houghton Mifflin Company. All rights reserved. 16a–1 Figure 16.31: Two-dimensional representations of (a) a quartz crystal and (b) a quartz.

Slides:



Advertisements
Similar presentations
Physics: Principles with Applications, 6th edition
Advertisements

ECE G201: Introductory Material Goal: to give you a quick, intuitive concept of how semiconductors, diodes, BJTs and MOSFETs work –as a review of electronics.
Superconductors 2. Resistance falls to zero at the critical temperature 1. Electrical resistance falls as temperature increases 4. Superconductors repel.
E bb **. E Looking only at this region in the Rectangle:
Semiconductors What Is A Semiconductor? A semiconductor is a substance that has a lower conductivity than a metal and a higher conductivity than a non-metal.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Chemistry FIFTH EDITION by Steven S. Zumdahl University of Illinois.
Semiconductor Device Physics
Physics of Semiconductor Devices. Formation of PN - Junction When a P-type Semiconductor is joined together with an N-type Semiconductor a PN junction.
Integrated Circuit Devices
Conduction of Electricity in Solids
Semiconductor Light Detectors ISAT 300 Foundations of Instrumentation and Measurement D. J. Lawrence Spring 1999.
Mr Powell VI Characteristics Ohms Law Current/voltage characteristics For an ohmic conductor, a semiconductor diode and a filament lamp Candidates.
Doped Semiconductors Group IVA semiconductors can be “doped” by adding small amounts of impurities with more or fewer than 4 valence electrons. e.g. add.
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.
Lecture #3 OUTLINE Band gap energy Density of states Doping Read: Chapter 2 (Section 2.3)
P and n type semiconductors. Semiconductors Semiconductors are also referred to as metalloids. Metalloids occur at the division between metals and non-metals.
Copyright © Houghton Mifflin Company. All rights reserved. 16a–1 Figure 16.31: Two-dimensional representations of (a) a quartz crystal and (b) a quartz.
Unit-II Physics of Semiconductor Devices. Formation of PN Junction and working of PN junction. Energy Diagram of PN Diode, I-V Characteristics of PN Junction,
Lecture 2 OUTLINE Semiconductor Fundamentals (cont’d) – Energy band model – Band gap energy – Density of states – Doping Reading: Pierret , 3.1.5;
Lesson 23: Introduction to Solar Energy and Photo Cells ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson a.pptx.
Lecture 2 OUTLINE Important quantities Semiconductor Fundamentals (cont’d) – Energy band model – Band gap energy – Density of states – Doping Reading:
ECE685 Nanoelectronics – Semiconductor Devices Lecture given by Qiliang Li.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Figure 10.1 Schematic Representations of the Three States of Matter.
Chemistry XXI M2. Inducing Electron Transitions. M1. Controlling Electron Transfer Analyze electron transfer between coupled systems. Explore the effect.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Section 10.5 CARBON & SILICON: NETWORK ATOMIC SOLIDS NETWORK SOLIDS: SOLIDS CONTAINING.
Materials Conductive materials – valence band overlaps the conduction band Conductive materials – valence band overlaps the conduction band Non conductive.
The Science of Solar Cells May 15, Announcements.
Presentation on: ELECTROMAGNETISM Topic: SEMICONDUCTORS Presented to: SIR.TARIQ BHATTI Program: BsIT-3rd Department of Computer Science.
Gentle Intro to Semiconductors ENGN/PHYS 207. The ubiquitous LED.
1 Free Electron Model for Metals Metals are very good at conducting both heat and electricity. A lattice of in a “sea of electrons” shared between all.
Electromagnetism Lecture#6 Instructor: Engr. Muhammad Mateen Yaqoob.
29-1Bonding in Molecules *When atoms cling together as a single unit to achieve lower energy levels, this is a chemical bond. *Bonds occur as ionic an.
SEMICONDUCTORS Materials can be categorised into conductors, semiconductors or insulators by their ability to conduct electricity.conductorssemiconductorsor.
© 2008 Brooks/Cole 1 Chapter 20, section 20.3 Semiconductors and superconductors.
Solar panels A solar panel is made up of photovoltaic cells. A photovoltaic cell converts light energy into electricity. A conductor is something that.
Solar Cells Solar cells are made of two types of silicon Normal silicon has no free electrons N-type silicon has been doped with phosphorus to give it.
ELECTRONIC PROPERTIES OF MATTER - Semi-conductors and the p-n junction -
Free Electron Model for Metals
Energy of 3 π bonding orbitals lower than energy of 2p (isolated) orbitals on C from which they come. π antibonding are higher than isolated 2p. Find experimentally.
Introduction to Semiconductor Materials
Band Theory of Solids In isolated atoms the electrons are arranged in energy levels.
Extended Questions- The Answers
Conductors – many electrons free to move
1. Unit I: Semiconductor Diodes and Applications Before we start with Electronics Let us review the Basics of Electricity Q. What are the two main quantities.
1 Higher Physics Unit 3 Optoelectronics Semiconductors.
Solar panels are pretty expensive, but they are good to save money on electricity. They take something from the sun and do something with it to make it.
UNIT- IV SOLID STATE PHYSICS. 1)Electrical conductivity in between conductors & insulators is a) high conductors b) low conductors c) Semiconductors d)
Topic #1: Bonding – What Holds Atoms Together?
NEEP 541 Ionization in Semiconductors Fall 2002 Jake Blanchard.
Crystalline Solids, Band Theory, and Doping
Many solids conduct electricity
Problems All problems up to p.28 Q 4 can be done.
Solar Cell Semiconductor Physics
1 Semiconductor Devices  Metal-semiconductor junction  Rectifier (Schottky contact or Schottky barrier)  Ohmic contact  p – n rectifier  Zener diode.
Properties of metals Metals (75% of elements) Lustrous (reflect light)
Liquids and Solids (cont’d). Copyright © Houghton Mifflin Company. All rights reserved. 16c–2 Electrical Properties Metallic Conductors, e.g. Cu, Ag...
Semiconductors. O A Semiconductor is a material whose resistivity is between that of a good conductor and a good insulator. O Examples of materials which.
Band Theory of Electronic Structure in Solids
Overview of Silicon Device Physics
Intro to Semiconductors and p-n junction devices
COURSE NAME: SEMICONDUCTORS Course Code: PHYS 473.
Solids: Conductors, Insulators and Semiconductors
Energy of 3 π bonding orbitals lower than energy of 2p (isolated)
Covalent Bonding: Orbitals (cont’d)
Covalent Bonding: Orbitals (cont’d)
Covalent Bonding: Orbitals (cont’d)
Materials Conductive materials – valence band overlaps the conduction band Non conductive materials – valence band is separated from conduction.
Materials Conductive materials – valence band overlaps the conduction band Non conductive materials – valence band is separated from conduction.
First Brillouin zone of FCC lattice and the band diagram (Do you see any gaps?)
Presentation transcript:

Copyright © Houghton Mifflin Company. All rights reserved. 16a–1 Figure 16.31: Two-dimensional representations of (a) a quartz crystal and (b) a quartz glass.

Copyright © Houghton Mifflin Company. All rights reserved. 16a–2 Figure 16.28: The p orbitals (a) perpendicular to the plane of th carbon ring system in graphite can combine to form (b) an extensive pie bonding network.

Copyright © Houghton Mifflin Company. All rights reserved. 16a–3 The Electronic Configuration of a Magnesium Atom nlmlml msms 300+1/ /2 Mg: (Ne)3s 2 1s 2s 3s 2p 3p Empty 3p orbitals in Mg valence shell

Copyright © Houghton Mifflin Company. All rights reserved. 16a–4 Orbital energy levels

Copyright © Houghton Mifflin Company. All rights reserved. 16a–5 Figure 16.24: A representation of the energy levels (bands) in a magnesium crystal

Copyright © Houghton Mifflin Company. All rights reserved. 16a–6 Figure 16.27: Partial representation of the MO energies in (a) diamond and (b) a typical metal

Copyright © Houghton Mifflin Company. All rights reserved. 16a–7 Electron sea model for metals

Copyright © Houghton Mifflin Company. All rights reserved. 16a–8 Bonding in Solids Metallic Solids

Copyright © Houghton Mifflin Company. All rights reserved. 16a–9 Band structure of Semiconductors

Copyright © Houghton Mifflin Company. All rights reserved. 16a–10 Band Diagram: Semiconductor with No Doping At T = 0, lower valence band is filled with electrons and upper conduction band is empty, leading to zero conductivity. –Fermi energy E F is at midpoint of small energy gap (<1 eV) between conduction and valence bands. At T > 0, electrons thermally “excited” from valence to conduction band, leading to measurable conductivity. EFEF ECEC EVEV Conduction band (Partially Filled) Valence band (Partially Empty) T > 0

Copyright © Houghton Mifflin Company. All rights reserved. 16a–11 Silicon Crystal Doped with (a) Arsenic and (b) Boron

Copyright © Houghton Mifflin Company. All rights reserved. 16a–12 Figure 16.33: Energy-level diagrams for (a) an n-type semiconductor and (b) a p-type semiconductor.

Copyright © Houghton Mifflin Company. All rights reserved. 16a–13 pn junction

Copyright © Houghton Mifflin Company. All rights reserved. 16a–14 Figure 16.34: The p-n junction involves the contact of a p-type and an n-type semiconductor.

Copyright © Houghton Mifflin Company. All rights reserved. 16a–15 PN Junction - 7

Copyright © Houghton Mifflin Company. All rights reserved. 16a–16 PN Junction with Applied Potential No current, Barrier LargerCurrent Flows, Barrier Smaller

Copyright © Houghton Mifflin Company. All rights reserved. 16a–17 Herbert Kroemer

Copyright © Houghton Mifflin Company. All rights reserved. 16a–18

Copyright © Houghton Mifflin Company. All rights reserved. 16a–19 Light Amplification by Stimulated Emission Radiation

Copyright © Houghton Mifflin Company. All rights reserved. 16a–20 Solar Cells n-typep-type Photons Electron Hole Load p-n Junction under Illumination

Copyright © Houghton Mifflin Company. All rights reserved. 16a–21 Solar Panels – Photovoltaic Cells

Copyright © Houghton Mifflin Company. All rights reserved. 16a–22 Schematic of a Photovoltaic (solar) cell

Copyright © Houghton Mifflin Company. All rights reserved. 16a–23 A schematic of two circuits connected by a transistor.

Copyright © Houghton Mifflin Company. All rights reserved. 16a–24 Photolithography to make semiconductor integrated circuits

Copyright © Houghton Mifflin Company. All rights reserved. 16a–25 (a)-(h) The steps for forming a transistor in a crystal of initially pure silicon.

Copyright © Houghton Mifflin Company. All rights reserved. 16a–26 (a)-(h) The steps for forming a transistor in a crystal of initially pure silicon. (cont’d)

Copyright © Houghton Mifflin Company. All rights reserved. 16a–27 Semiconductors – key points to remember Band structure: Valence band – gap – conduction band DOPING: Group V  n type, Group III  p type n-p junctions Devices: (LED, laser, transistor, solar cell)

Copyright © Houghton Mifflin Company. All rights reserved. 16a–28 Figure 16.24: A representation of the energy levels (bands) in a magnesium crystal

Copyright © Houghton Mifflin Company. All rights reserved. 16a–29 Band structure of Semiconductors

Copyright © Houghton Mifflin Company. All rights reserved. 16a–30 Semiconductors – key points to remember Band structure: Valence band – gap – conduction band DOPING: Group V  n type, Group III  p type n-p junctions Devices: (LED, laser, transistor, solar cell)

Copyright © Houghton Mifflin Company. All rights reserved. 16a–31 Silicon Crystal Doped with (a) Arsenic and (b) Boron

Copyright © Houghton Mifflin Company. All rights reserved. 16a–32 Semiconductors – key points to remember Band structure: Valence band – gap – conduction band DOPING: Group V  n type, Group III  p type n-p junctions Devices: (LED, laser, transistor, solar cell)

Copyright © Houghton Mifflin Company. All rights reserved. 16a–33 pn junction

Copyright © Houghton Mifflin Company. All rights reserved. 16a–34 Semiconductors – key points to remember Band structure: Valence band – gap – conduction band DOPING: Group V  n type, Group III  p type n-p junctions Devices: (LED, laser, transistor, solar cell)

Copyright © Houghton Mifflin Company. All rights reserved. 16a–35 C 60 crystals

Copyright © Houghton Mifflin Company. All rights reserved. 16a–36 Ionic liquids