Novel Soft Materials: Organic Semiconductors

Similar documents
Plastic Electronics. Joaquim Puigdollers.

Organic Electronic Devices

Surface Transfer Doping of Diamond by Organic Molecules

Introduction. Fang-Chung Chen Department of Photonics and Display Institute National Chiao Tung University. Organic light-emitting diodes

Introduction to semiconductor nanostructures. Peter Kratzer Modern Concepts in Theoretical Physics: Part II Lecture Notes

Electron Spectroscopy

Initial Stages of Growth of Organic Semiconductors on Graphene

Classification of Solids

Graphene. Tianyu Ye November 30th, 2011

ESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor

Conductivity and Semi-Conductors

X-Ray Photoelectron Spectroscopy (XPS)

Quantum Dots for Advanced Research and Devices

Chapter 7. Solar Cell

Introduction to Organic Solar Cells

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960

Flexible Organic Photovoltaics Employ laser produced metal nanoparticles into the absorption layer 1. An Introduction

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7

Physics of Organic Semiconductor Devices: Materials, Fundamentals, Technologies and Applications

Photodiodes and other semiconductor devices

Chemistry Instrumental Analysis Lecture 8. Chem 4631

KATIHAL FİZİĞİ MNT-510

Paper Review. Special Topics in Optical Engineering II (15/1) Minkyu Kim. IEEE Journal of Quantum Electronics, Feb 1985

Methods of surface analysis

Electrons are shared in covalent bonds between atoms of Si. A bound electron has the lowest energy state.

E L E C T R O P H O S P H O R E S C E N C E

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu

Optical Spectroscopies of Thin Films and Interfaces. Dietrich R. T. Zahn Institut für Physik, Technische Universität Chemnitz, Germany

In a metal, how does the probability distribution of an electron look like at absolute zero?

Appendix 1: List of symbols

Semiconductor Polymer

X-Ray Photoelectron Spectroscopy (XPS)

Stepwise Solution Important Instructions to examiners:

Semiconductors and Optoelectronics. Today Semiconductors Acoustics. Tomorrow Come to CH325 Exercises Tours

ORGANIC SEMICONDUCTOR 3,4,9,10-Perylenetetracarboxylic dianhydride (PTCDA)

Supporting Information

Sébastien FORGET. Laboratoire de Physique des Lasers Université Paris Nord P13. www-lpl.univ-paris13.fr:8088/lumen/

Solid State Device Fundamentals

Basic cell design. Si cell

Observation of electron injection in an organic field-effect transistor with electroluminescence *

e - Galvanic Cell 1. Voltage Sources 1.1 Polymer Electrolyte Membrane (PEM) Fuel Cell

PHYSICS nd TERM Outline Notes (continued)

Lecture 5. X-ray Photoemission Spectroscopy (XPS)

FYS 3028/8028 Solar Energy and Energy Storage. Calculator with empty memory Language dictionaries

Electronic properties of organic semiconductors and their interfaces. Devices of "Organic & Hybrid Electronics"

Real-time and in-line Optical monitoring of Functional Nano-Layer Deposition on Flexible Polymeric Substrates

Supporting Information

OPTICAL PROPERTIES AND SPECTROSCOPY OF NANOAAATERIALS. Jin Zhong Zhang. World Scientific TECHNISCHE INFORMATIONSBIBLIOTHEK

Organic semiconductor heterointerfaces containing bathocuproine

Supplementary material: Nature Nanotechnology NNANO D

Towards a deeper understanding of polymer solar cells

Electronics go everywhere

Review of Optical Properties of Materials

Supporting Information

CME 300 Properties of Materials. ANSWERS: Homework 9 November 26, As atoms approach each other in the solid state the quantized energy states:

2D MBE Activities in Sheffield. I. Farrer, J. Heffernan Electronic and Electrical Engineering The University of Sheffield

Making OLEDs efficient

The Electromagnetic Properties of Materials

X-ray Photoelectron Spectroscopy (XPS)

Local Anodic Oxidation of GaAs: A Nanometer-Scale Spectroscopic Study with PEEM

Crystal Properties. MS415 Lec. 2. High performance, high current. ZnO. GaN

Energy Spectroscopy. Ex.: Fe/MgO

Temperature Dependent Optical Band Gap Measurements of III-V films by Low Temperature Photoluminescence Spectroscopy

Transparent Electrode Applications

Basic Principles of Light Emission in Semiconductors

Microscopic Ohm s Law

MSE 321 Structural Characterization

Chapter Modern Physics

MS482 Materials Characterization ( 재료분석 ) Lecture Note 2: UPS

Triplet state diffusion in organometallic and organic semiconductors

This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and

Bonds in molecules are formed by the interactions between electrons.

A. OTHER JUNCTIONS B. SEMICONDUCTOR HETEROJUNCTIONS -- MOLECULES AT INTERFACES: ORGANIC PHOTOVOLTAIC BULK HETEROJUNCTION DYE-SENSITIZED SOLAR CELL

Solar Cell Materials and Device Characterization

Abstract. Introduction

Photovoltaics. Lecture 7 Organic Thin Film Solar Cells Photonics - Spring 2017 dr inż. Aleksander Urbaniak

EEE4106Z Radiation Interactions & Detection

Matti Laan Gas Discharge Laboratory University of Tartu ESTONIA

Photonic Communications Engineering Lecture. Dr. Demetris Geddis Department of Engineering Norfolk State University

Ch/ChE 140a Problem Set #3 2007/2008 SHOW ALL OF YOUR WORK! (190 Points Total) Due Thursday, February 28 th, 2008

Two-dimensional lattice

Energy Spectroscopy. Excitation by means of a probe

Metal Organic interfaces

Solid State Device Fundamentals

PHOTOVOLTAICS Fundamentals

Supplementary Materials for

Session 5: Solid State Physics. Charge Mobility Drift Diffusion Recombination-Generation

Two-dimensional lattice

Unit IV Semiconductors Engineering Physics

X-Ray Photoelectron Spectroscopy (XPS) Auger Electron Spectroscopy (AES)

Organic solar cells. State of the art and outlooks. Gilles Horowitz LPICM, UMR7647 CNRS - Ecole Polytechnique

Lecture 15: Optoelectronic devices: Introduction

Chapter 4 Scintillation Detectors

n N D n p = n i p N A

MSE 310/ECE 340: Electrical Properties of Materials Fall 2014 Department of Materials Science and Engineering Boise State University

Photoelectron spectroscopy Instrumentation. Nanomaterials characterization 2

Transparent TiO 2 nanotube/nanowire arrays on TCO coated glass substrates: Synthesis and application to solar energy conversion

EE 446/646 Photovoltaic Devices I. Y. Baghzouz

Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis

Lecture 10 Charge Carrier Mobility

Transcription:

JSPS Science Dialogue Novel Soft Materials: Organic Semiconductors X.T. HAO Prof. UENO s Lab Faculty of Engineering, Chiba University 21 st Century Center of Excellence Program

The route to research Transparent oxide semiconductors: Shandong University, China Organic light emitting devices: Institute of Materials Research and Engineering, Singapore Surface and interface of organic semiconductors: Prof. UENO s Lab, Faculty of Engineering, Chiba University, Japan

9.6million km 2, 1300 millions people Spring City--Jinan Bao Tu Spring

Transparent oxide semiconductors Shan Dong University Send out, Take in

Organic light emitting devices: Institute of Materials research & Engineering Transparent cathode Polymer layers Anode Substrate

Surface and interface of organic semiconductors: Prof. UENO s Lab

The route to research Find problems solve problems Improvement? More places more experiences Knowledgeable?

Novel Soft Materials: Organic Semiconductors

Outline Introduction Basic concepts in organic semiconductors Surface/interface of organic semiconductors Organic devices Summary

Resistivity difference 10 24 =1,000,000,000,000,000,000,000,000 Discovery of organic semiconductors Japan, 1950 Pioneers: Akamatu and Inokuchi,

Current Research Status OLED Organic soft device Application Fundamental Synthesis of Organic Semiconductors A B C A Unified organic Device metal organic. Nanoscale structure and properties; electronic and electrical properties etc Pb Pb - Pb Pb Pb Nanoscale control of organic film growth Theory and experiment Molecular Scalpel/ Syn. Rad. h π Electron Electronic states and dynamics σ

One electron in one orbital Metal & Insulator [Quantum Effect] Two electrons in one orbital Animation contributed by Prof. H. FUKUYAMA

Motion of holes and electrons

Transport of charge carriers Motion of ball E E = 1 2 mv 2 = 2 P 2m P E Motion of electron E = E( P) P

Fermi Level The behavior of water in bucket and electrons in solid E F

E F φ VL Fermi Sea of electrons Metal Vacuum Bandgap E Conduction band E F φ VL Ionization energy Valence band Intrinsic semicond. Insulator Vacuum

Conductivity Ohm s Law V = IR σ =neµ R = ρl S σ 1 = ρ R = l σ S Carrier concentration Mobility

Conductivity Mobility Charge transfer rate k CT σ =neµ a µ = ea2 k B T k CT k CT = 2π h 1 t 2 4πλ reorg k B T exp λ reorg 4k B T µ We need smaller λ for higher µ t : Transfer integral (intermolecular interaction) λ reorg : Reorganization energy (hole-vibration coupling) λ reorg J. Cornil et al. Adv. Mater. 14, 726 (2002). Coropceanu et al.,theor. Chem. Acc. 110, 59 (2003). J.L.Bredas group, Chem.Rev.104, 4971 (2004).

Electronic interaction at surface/interface cathode e- transfer recombination h + transfer anode

Electron exchange Electron Organic molecule Metal atoms

Energy level alignment at interface Metal Organic Interface Molecular orientation reaction with metal distortion of electronic distribution existence of electric dipole

Contact between metal and molecular solid Electron transfer Fermi level

Nobel Prize, 1921 Photoelectric effect

Photoelectric effect Photon Electron(E K )

E=hν-Φ Kinetic energy of photoelectron hν Binding energy (work function /metal) Solid Vacuum

e - velocity v hν + Potential is acting on photoelectron

v e - velocity v > v After the potential disappears, photoelectron travels without reducing its velocity.

Excited / vacuum level e - Work function (φ) E F e - E F Ionization potential IP E K = hv -IP e - hv Secondary electrons hv Secondary electrons E vac E F Fermi level E F Ionization potential UPS for metal UPS for organic film

High-resolution UPS -I Preparation chamber/organic He reefer He* X-ray Analyzer Preparation chamber/metal LEED/Auger Polarized VUV photon

High-resolution UPS -II Analyzer (R=300mm) (A-1, MBS-Toyama) Cleaning chamber (SPA-LEED) STM Spectrometer (M-1, MBS-Toyama) + He source (L-1, MBS) Preparation chamber

He* (MAES) source Chamber PIES/UPS Instrument and Characteristics of of PIES colddischarge type DP with L-N2Trap system TMP Q-MASS Measurment Chamber SP sample holder inlet for L-N2 Transfer Rod 180* hemi-spherical deflection type analyzer Sample Preparation Chamber Introduction Chamber DP with L-N2Trap system He I (UPS) source Chamber

PIES: Penning Ionization Electron Spectroscopy 2s 1s

Molecular orientation can be detected: PIES study P O Ti He*(2 3 S) MAES Intensity (arb. units) Gr(σ*) π Gr(π) n (O) state π π annealed as grown O Ti e - e - O Ti O Ti O Ti e - He* O Ti He* HOPG O Ti Ti O O Ti Ti O O Ti 15 10 Binding Energy from E F sub (ev) 5 0

Organic devices: Organic light emitting devices Organic solar cells Organic thin film transistors etc Soft organic materials Flexible bendable devices

Organic light emitting diodes ~100nm (~0.0001mm) ~0.1-1mm 1mm =1,000,000nm

Organic solar cell

Basic structure of Organic LED Cathode Light Emitting Layer Hole Transport Layer Anode Substrate Cathode: metal material Emitter: organic materials Anode: metal, semiconductors Substrate: Rigid & flexible

cathode e- transfer recombination h + transfer anode Working Mechanism of OLED e- transfer h + transfer Luminescence E F HOMO + + + + + + + + + - + - - - - - - LUMO - - E F - - - - - - - - + + + + + + +

60 6 Sheet resistance resistivity Sheet resistance (Ω/sq) 50 40 30 5 4 3 Resistivity (Ω cm) 20 0.0 0.5 1.0 1.5 2.0 Hydrogen flow rate (sccm) 2

Conventional Flexible OLED approach Ag Ca EL ITO PET/barrier layer

Variable color OLEDs Non-cavity Top OLED Transparent cathode Organic stack ITO anode Transparent cathode Organic stack ITO anode Cavity Top OLED Substrate Mirror Mirror Substrate Non-cavity OLED Cathode mirror Organic stack ITO anode Substrate Cathode mirror Organic stack ITO anode Semitransparent mirror Substrate Cavity OLED

Variable color OLEDs Φ1+ Φ2+2ndλ=m2π λ1 λ2 λ3 λ1 λ2 λ3 ITO thickness: 21.7nm 43.3nm 65nm 86.7nm 108.3nm 130nm 151.1nm 173.3nm

High contrast OLED Cathode Organic stack TCO anode Optical destructive anode n(x) Transparent substrate Sunlight readable OLED display

Cathode Emitting layer HTL ITO glass

Technology and Advantages Rigid device Flexible device paper-like appearance high brightness low voltage etc ultra-thin, lightweight conformable shape low cost etc

Samsung s 21-inch and 40-inch OLED TV resolution :1920x1200 contrast ratio: 5000:1 resolution :1280 x 800 contrast ratio: 5000:1

Summary

Acknowledgement Japan Society for the Promotion of Science (JSPS) UENO s Lab: Prof. Ueno, Prof. Okudaira, Prof. Sakamoto, Dr. Kera, Other members

Thank you for your attention!