White Paper: Transparent High Dielectric Nanocomposite

Similar documents
White Paper: Resistivity and Dielectric Strength of Nanocomposites

White Paper: Low Chromatic Aberration Nanocomposite

Elizabethtown College Department of Physics and Engineering PHY104

CHAPTER 6 DIELECTRIC AND CONDUCTIVITY STUDIES OF ZIRCONIUM TIN TITANATE (ZST)


Supporting Information

The Dielectric Properties of (PVA-PEG-PVP-MgO) and (PVA-PEG-PVP-CoO) Biomaterials

DEPARTMENT OF ELECTRICAL ENGINEERING DIT UNIVERSITY HIGH VOLTAGE ENGINEERING

Institute for Electron Microscopy and Nanoanalysis Graz Centre for Electron Microscopy

Dielectric Properties of Composite Films Made from Tin(IV) Oxide and Magnesium Oxide

Technology Brief 9: Capacitive Sensors

White Paper: Compatibility of ZrO2 Nanocrystals in Acrylic Monomers

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

Plasmonics. The long wavelength of light ( μm) creates a problem for extending optoelectronics into the nanometer regime.

Chapter 10. Nanometrology. Oxford University Press All rights reserved.

Variable capacitor energy harvesting based on polymer dielectric and composite electrode

SUPPLEMENTARY INFORMATION

MAGNETIC FIELDS & UNIFORM PLANE WAVES

True Room Temperature Bonding a novel process for the creation of health tech consumables ATB. ir. Richard Bijlard Technogation - Invenios

Introducing the RoVaCBE Flagship project: Roll-to-roll Vacuum-processed Carbon Based Electronics. Dr Hazel Assender, University of Oxford

Effect of Filler Surface Modification on the Dielectric Properties of High-k Composite Materials

Optimization of MnO2 Electrodeposits using Graphenated Carbon Nanotube Electrodes for Supercapacitors

Laser Processing of 3-D Structures for Embedded and Integrated Components: An Application of Flexible and Printable Nanomaterials in Microelectronics

EE 4345 Chapter 6. Derek Johnson Michael Hasni Rex Reeves Michael Custer

Supporting Online Material for

White Paper: Lumen Gain with Zirconia-Silicone Nanocomposites for LED Encapsulation

Nanofabrication Lab Process Development for High-k Dielectrics

Evaluation of Capacitance in Motor Circuit Analysis Findings. Howard W Penrose, Ph.D., CMRP President, SUCCESS by DESIGN

CHARACTERIZATION OF MAGNETICALLY LOADED MICROWAVE ABSORBERS

Short-Term Dielectric Performance Assessment of BOPP Capacitor Films: A Baseline Study

Lecture contents Review: Few concepts from physics Electric field

Improving the dielectric and piezoelectric properties of screen-printed Low temperature PZT/polymer composite using cold isostatic pressing

Dielectric constant measurement of P3HT, polystyrene, and polyethylene

Graphene Fundamentals and Emergent Applications

Graphene-Rubber Composites

Experiment FT1: Measurement of Dielectric Constant

Transmission-Reflection Method to Estimate Permittivity of Polymer

Gold Nanoparticles Floating Gate MISFET for Non-Volatile Memory Applications

Supplementary information

DIELECTRIC AND AC CONDUCTION STUDIES OF LEAD PHTHALOCYANINE THIN FILM

Supplementary Information for. Effect of Ag nanoparticle concentration on the electrical and

The Basic Capacitor. Dielectric. Conductors

TC 412 Microwave Communications. Lecture 6 Transmission lines problems and microstrip lines

Characterization of electric charge carrier transport in organic semiconductors by time-of-flight technique

Session V: Graphene. Matteo Bruna CAMBRIDGE UNIVERSITY DEPARTMENT OF ENGINEERING

Technical Data Sheet

Scalable Nanomaterials and Nanostructures for Energy and Flexible Electronics

ELECTROMAGNETIC MODELING OF THREE DIMENSIONAL INTEGRATED CIRCUITS MENTOR GRAPHICS

High speed vacuum deposition of organic TFTs in a roll-to-roll facility

Chapter 2: Capacitor And Dielectrics

AM11: Diagnostics for Measuring and Modelling Dispersion in Nanoparticulate Reinforced Polymers. Polymers: Multiscale Properties.

Outline. ECE 477 Digital Systems Senior Design Project. Module 7 Capacitor Selection Guidelines. Film Ceramic Electrolytic Miscellaneous

Nano-mechatronics. Presented by: György BudaváriSzabó (X0LY4M)

Metal nanoparticle-doped coloured films on glass and polycarbonate substrates

MICROWAVE SURFACE IMPEDANCE OF A NEARLY FERROELECTRIC SUPERCONDUCTOR

Enhanced Nonlinear Optical Response from Nano-Scale Composite Materials

INORGANIC NANOFILLER EFFECTS ON RESISTIVITY AND ABSORPTION CURRENTS IN LOW DENSITY POLYETHYLENE NANOCOMPOSITES

SCB10H Series Pressure Elements PRODUCT FAMILY SPEFICIFATION. Doc. No B

Supporting Information

Quantum Mechanical Simulation for Ultra-thin High-k Gate Dielectrics Metal Oxide Semiconductor Field Effect Transistors

PHYSICS nd TERM Outline Notes (continued)

INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012

The Science and Engineering of Materials, 4 th ed Donald R. Askeland Pradeep P. Phulé. Chapter 2 Atomic Structure

High Performance, Low Operating Voltage n-type Organic Field Effect Transistor Based on Inorganic-Organic Bilayer Dielectric System

Transient Photocurrent Measurements of Graphene Related Materials

Quantum Dots for Advanced Research and Devices

User s Manual. STUDY OF DIELECTRIC CONSTANT Model: DEC-01

Frequency dispersion effect and parameters. extraction method for novel HfO 2 as gate dielectric

Thermal-Mechanical Decoupling by a Thermal Interface Material

The Basic Capacitor. Water Tower / Capacitor Analogy. "Partnering With Our Clients for Combined Success"

Supplementary material for High responsivity mid-infrared graphene detectors with antenna-enhanced photo-carrier generation and collection

6.012 Electronic Devices and Circuits

FEATURES AND APPLICATIONS OF POLYMER THIN FILM MULTI-LAYER CAPACITOR PML CAP

Chapter 12. Nanometrology. Oxford University Press All rights reserved.

Steric stabilization. Dispersions in liquids: suspensions, emulsions, and foams ACS National Meeting April 9 10, 2008 New Orleans

5. Building Blocks I: Ferroelectric inorganic micro- and nano(shell) tubes

DIELECTRIC STUDIES IN THE DEVELOPMENT OF HIGH ENERGY DENSITY PULSED POWER CAPACITORS *

High-resolution Characterization of Organic Ultrathin Films Using Atomic Force Microscopy

Variation of Refractive Index of PMMA with temperature and different doping % of Tio 2

Temperature Dependent Current-voltage Characteristics of P- type Crystalline Silicon Solar Cells Fabricated Using Screenprinting

ALL-POLYMER FET BASED ON SIMPLE PHOTOLITHOGRAPHIC MICRO-PATTERNING OF ELECTRICALLY CONDUCTING POLYMER

DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD

THE INFLUENCE OF CARBON NANOTUBES ON THE ELECTRICAL PROPERTIES OF INJECTION MOLDED THERMOPLASTIC POLYMER MATRIX. Jan VÁCHA, Jiří HABR

Supporting Information. Metallic Adhesion Layer Induced Plasmon Damping and Molecular Linker as a Non-Damping Alternative

Thermo-Mechanical Analysis of a Multi-Layer MEMS Membrane

Chapt ha e pt r e r 9 Capacitors

CH676 Physical Chemistry: Principles and Applications. CH676 Physical Chemistry: Principles and Applications

Introduction to Electric Circuit Analysis

Carbon Nanotube Thin-Films & Nanoparticle Assembly

Solutions for Assignment-8

Thin Film Bi-based Perovskites for High Energy Density Capacitor Applications

Supplementary Figures

Metallurgical and Materials Engineering Department MME 2509 Materials Processing Laboratory SOL-GEL DIP COATING

Enhancing the Performance of Organic Thin-Film Transistor using a Buffer Layer

Xin Zhang, Weiwei Chen, Jianjun Wang, Yang Shen*, Yuanhua Lin, and Ce-Wen

Evaluation of Epoxy Nanocomposites for High Voltage Insulation

ESO 205 Nature and Properties of Materials

Microwave Absorption Enhancement of RGO/ Ni Nanocomposites

On-Wafer Characterization of Electromagnetic Properties of Thin-Film RF Materials

Lecture ) Electrical, Magnetic 2) Optical Properties of Nanomaterials (C4)

Transcription:

Zhiyun (Gene) Chen, Ph.D., Vice President of Engineering Pixelligent Technologies 64 Beckley Street, Baltimore, Maryland 2224 Email: zchen@pixelligent.com February 205 Abstract High dielectric constant materials have a wide array of applications. Most high dielectric constant materials are inorganic, which are typically difficult to process. Polymer materials are gaining popularity due to their processability and flexibility. They, however, has relatively low dielectric constant. Pixelligent s transparent ZrO2 nanocrystal/polymer nanocomposite provides a new class of high dielectric constant material that can be applied to many novel applications. Because of our proprietary surface capping technology, the nanocrystals can be incorporated into the polymer up to 80 wt% loading, corresponding to a dielectric constant of 8, without losing optical transparency and processability. Background on Dielectric Materials Dielectric materials have very broad applications in the electronic industry, including capacitors, gate dielectrics for transistors, and electrostatic dissipation (ESD) coatings. A non-magnetic dielectric material is defined by real and imaginary components of the Complex Permittivity: Normalization of ε* with respect to the Dielectric Permittivity of Free Space ε o = 0 9 /36π [f/m] gives the Complex Relative Permittivity: k and k indicate capability of storage of electric field energy and dissipative characteristics for nonmagnetic dielectrics. Dielectric Constant k is the relative permittivity or dielectric constant. It is the quantity generally referred to as Dielectric Constant in the literature. It is a dimensionless quantity since it

is relative to free space. Dissipation Factor (D), also called Loss Tangent or tan δ, is usually reported to indicate the energy loss characteristic of a material. It is also dimensionless and is defined as follows: Lossy dielectrics are characterized by a dissipation factor greater than 0.. They may or may not exhibit DC electrical conductivity. Dielectric properties usually vary with frequency; in general, the higher the DC conductivity, the greater the frequency sensitivity. Dielectrics with a dissipation factor less than 0.0 are considered low-loss materials and good electrical insulators. In general, dielectric properties show relatively little variation with frequency in the microwave range. Table shows the dielectric constant and dissipation factor for common dielectric materials. Various combinations of dielectric constant and dissipation factor are used in different applications. For example, a high dielectric constant and a low dissipation factor are desired for gate oxide integrated circuit applications. A high dielectric constant and a high dissipation factor are desired for ESD coatings. Table illustrates that most high dielectric constant materials are inorganic materials. As a result dielectric materials are traditionally made from inorganic substances. However, these materials are difficult to process, usually requiring high temperature process conditions, and are brittle and inflexible. Polymers are gaining wider use as dielectric materials for many applications such as flexible and printable electronics. This is due to increased processability, greater flexibility, and improved chemical resistance.. However, most polymers have a dielectric constant between and 4 [], severely limiting their use in many applications. 2

Table : Properties of common materials [] (The green cells indicate polymeric materials. The blue area indicates the range of properties that can be developed from Pixelligent s nanocomposites). 0.000 0.0002 0.0003 0.0004 0.0005 0.0006 0.0007 0.0008 0.0009 0.00 0.002 0.005 0.0 0.05 0. 2 2 2. 2.2 Teflon Natural Rubber 2. 2.2 2.3 2.4 Polyethlylene Fluropolymer 2.3 2.4 Dielectric Constant 2.5 3 4 5 6 7 8 Polystyrene Fused Silica Boron Nitride Mica Berrylium Borosilicate Glass Mylar Lexan Pyrex Nitirle Rubber Epoxy Silicone Soda lime Glass PMMA Zinc Molybdenum Sulfide 2.5 3 4 5 6 7 8 9 0 5 Sapphire Magnesium Aluminum Magnisium Titante 9 0 5 20 50 00 >00 0.000 0.0002 0.0003 0.0004 0.0005 0.0006 Strontium Titante 0.0007 0.0008 0.0009 0.00 0.002 0.005 Dissipation Factor Titanium Dioxide Zirconia Barium Titanate 0.0 0.05 0. 20 50 00 >00 Pixelligent s High-Dielectric Constant Nanocomposites Nanocomposites composed of inorganic nanocrystals and polymer matrices offer a greater range of dielectric properties without sacrificing other properties of the polymer. Nanocomposites are a rapidly developing family of materials. They have a wide array of applications. A nanocomposite is a synthetic material composed of one or more types of nanocrystals (i.e. fillers), usually embedded in a polymeric binder. A nanocomposite is an effective way to combine the advantages of the constitute materials. Nanocrystals are particles of a material, typically tens of nanometers or smaller, that retain the stoichiometry and crystal structure of their bulk counterpart. Nanocrystals have been the focus of accelerated scientific studies for the past two decades because they often demonstrate novel properties as a result of the reduced sizes. Moreover, nanocrystals can be surface treated with various capping agents and dispersed into polymer matrices to form nanocomposites that can be used in applications where bulk materials are impractical or when novel and integrated functionalities are required. When nanocrystals are dispersed into an optically transparent polymer, the dielectric constant of the resulting 3

nanocomposite can be described using effective medium theory, for example, Maxwell Garnett theory: [2] ε ε eff eff ε + ε i ε m = δi ( ) ε + 2ε m 2ε m i m where ε eff is the effective dielectric constant of the medium, ε i is the one of the inclusions and ε m is the one of the matrix δ i is the volume fraction of the nano-filler. Figure. Dielectric constant of the ZrO 2/Acrylic Nanocomposites with different loadings. For reference, silicon dioxide, a commonly used dielectric material for gate oxide, has a dielectric constant of 3.9. The small (< 0 nm) and uniform size of Pixelligent s nanocrystals, and our proprietary surface modification technology ensure that when the nanocrystals are loaded into a polymer matrix, they are entirely agglomeration free with superb homogeneity. The quality of the nanocomposite and film is demonstrated in Figure 2. The high quality of Pixelligent s nanocomposite provides low dielectric loss and high optical transparency. To demonstrate the impact of the ZrO 2 nanocrystals inclusion on the dielectric constant, a ZrO 2/acrylic system was used as a model system. The nanocomposite formulation with different ZrO 2 loadings were spin-coated on a conductive silicon wafers, with ~ 2 µm in thickness, then gold electrodes are deposited on top of the film to form a metal-insulator-metal configuration. The capacitance was 4

measured using a LCR meter and the dielectric constant was calculated. The results are shown in Figure. Dielectric constant of ~ 8 can be achieved with ~ 80 wt% nanocrystal loading. The measured value is larger than predicted by Maxwell Garnett model, which assumes that there is no interaction between the matrix and filler. Similar results based on ZrO 2 nanocrystals were also observed in the literature, the large dielectric constant was attributed to interfacial polarization as a result of the mixed valency of Zr ions on the nanocrystal surface. [4] a) b) Figure 2. TEM images of the nanocomposite films measured. a) shows the uniform film thickness and excellent smoothness; and b) is a high magnification image showing individually dispersed ZrO 2 nanocrystals. Figure 3a shows the testing structure for the dielectric constant measurements. The films were deposited on a highly conductive silicon substrate, placing gold contacts on top of the film for an array of capacitors. Figure 3b shows a typical capacitance and dissipation factor of a nanocomposite with 80 wt% ZrO 2 nanocrystals. ZrO 2 nanocrystals loading. The dissipation factor of the material is very low even at high frequency. Considering the low thickness of the film, this indicates that the device made with the nanocomposite film will have very low leakage current. 5

a) b) Figure 3. a) Testing structure for the dielectric constant measurements; b) a typical capacitance and dissipation factor of a nanocomposite with 80 wt% ZrO 2 nanocrystals. The dielectric constant can be calculated from the capacitance. The optical transmittance of these films were also measured, these films are deposited on quartz substrates with similar process conditions. All the films showed good optical transmittance in the entire visible range, as shown in Figure 4. Figure 4. Optical transmittance of two of the Pixelligent s high dielectric nanocomposites. Note: The transmittance were measured without a reference, which means the reflection from the front surface was not taken into account and the actual transmittance is higher than what were shown in the figure. 6

Pixelligent is capable of dispersing the nanocrystals into a large variety of polymers, such as acrylics, epoxies, silicones, and siloxanes. A similar trend in improving dielectric constant is expected as nanocrystal loading increases in the nanocomposite based on Equation. Pixelligent s ZrO 2 nanocrystal/polymer nanocomposite combines the high dielectric constant of ZrO 2 with the processability of polymeric materials to provide a flexible, and high dielectric nanocomposite that can be easily applied with a thin film coating process such as spin-coating or roll-to-roll printing. Our nanocomposites significantly expand the range of available dielectric constants for polymeric dielectric materials, as illustrated by the blue rectangle in Table. Furthermore, Pixelligent s nanocomposites are highly transparent as well as solution processable, allowing them to be used in a broad array of applications such as displays, touch screens, smart windows, optical sensors and printable electronics. Acknowledgment We thank Dr. Pooran Joshi from Oakridge National Labs for performing the dielectric constant measurement and transmission electron microscopy. The measurement is work is partly funded by DOE Corporate Research and Development Agreement (CRADA) # NFE-4-05086. Bibliography [] Data cited from Technical Reports AFML-TR-72-39 and 74-250 Laboratory for Insulation Research, Massachusetts Institute of Technology. Measurements are 25 C and -0 GHz. Properties vary with frequency and temperature.. [2] H. Nalwa, Handbook of Low and High Dielectric Constant Materials and Their Applications, London: Academic Press, 999. [3] T. C. Choy, Effective Medium Theory, Oxford: Clarendon Press, 999. [4] S. G. T. &. D. S. K. Manna, "Room temperature stabilized cubic zirconia nanocrystal: a giant dielectric material," Journal Of Physics D: Applied Physics, vol. 43, no. 29, p. 295403, 200. 7