edited by...1.5 concluding remarks 27 references 27 2 mechanics of twistable electronics 31 yewang...
TRANSCRIPT
Edited by
Takao Someya
Stretchable Electronics
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Stretchable Electronics
Edited by Takao Someya
The Editor
Prof. Takao SomeyaUniversity of TokyoDepartment of Electrical Engineering7-3-1 Hongo, Bunkyo-kuTokyo 113-8656Japan
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V
Contents
Preface XV ListofContributors XVII
PartI Theory 1
1 TheoryforStretchableInterconnects 3 JizhouSongandShuodaoWang1.1 Introduction 31.2 Mechanics of Stretchable Wavy Ribbons 51.2.1 Small-Deformation Analysis 51.2.2 Finite-Deformation Analysis 81.2.3 Ribbon Width Effect 121.3 Mechanics of Popup Structure 151.4 Mechanics of Interconnects in the Noncoplanar Mesh
Design 191.4.1 Global Buckling of Interconnects 191.4.2 Adhesion Effect on Buckling of Interconnects 211.4.3 Large Deformation Effect on Buckling of Interconnects 241.5 Concluding Remarks 27 References 27
2 MechanicsofTwistableElectronics 31 YewangSu,JianWu,ZhichaoFan,Keh-ChihHwang,YonggangHuang,
andJohnA.Rogers2.1 Introduction 312.2 Postbuckling Theory 312.3 Postbuckling of Interconnect under Twist 332.4 Symmetric Buckling Mode 342.5 Antisymmetric Buckling Mode 362.6 Discussion and Concluding Remarks 38 References 38
VI Contents
PartII MaterialsandProcesses 41
3 GrapheneforStretchableElectronics 43 ChaoYan,Seoung-KiLee,HoukJang,andJong-HyunAhn3.1 Introduction 433.2 Production of Graphene Films 443.2.1 Large-Area Graphene Synthesis by CVD 443.2.2 Exfoliation Methods 473.2.3 Epitaxial Growth Methods 483.3 Fabrication of Graphene Films on Substrates 503.3.1 Solution-Based Method 503.3.2 Transfer Printing 523.4 Applications in Flexible and Stretchable Electronics 543.4.1 Interconnect for Integrated Circuits 573.4.2 Flexible Electronics 603.4.2.1 Graphene Electrodes for Flexible FETs 603.4.2.2 Graphene Electrodes for Flexible OPVs 643.4.2.3 Graphene Electrodes for OLEDs 663.4.2.4 Graphene Film for Flexible Touch Screen Panels 703.4.3 Stretchable Electronics 713.5 Concluding Remarks 75 References 76
4 StretchableThin-FilmElectronics 81 StéphanieP.Lacour4.1 Introduction 814.2 Silicone Rubber as a Substrate 824.2.1 Elastomers 824.2.2 Silicone Rubber – Polydimethylsiloxane (PDMS) 834.2.2.1 PDMS Surface Chemistry 834.2.2.2 PDMS Mechanical Properties 844.2.2.3 Dielectric Properties 854.2.2.4 Other Properties 864.2.3 Photosensitive Silicones 864.3 Mechanical Architecture 874.3.1 Preserving the Mechanical Integrity of Thin-Film
Structures 884.3.1.1 Small Platforms (<500 µm Side) 894.3.1.2 Large Platforms (>500 µm Side) 904.3.2 Ensuring Smooth Strain Gradient across Interconnects 914.4 Stretchable Metallization 934.4.1 Morphology of Thin Gold Films on PDMS 944.4.2 Electromechanical Response 954.4.2.1 Uni-axial (1D) Stretching 964.4.2.2 Multi-axial (2D) Stretching 98
Contents VII
4.4.3 Printed Films on PDMS Substrate 994.5 Integrated Stretchable Thin-Film Devices 1004.5.1 Soft Neural Electrode Arrays 1004.5.2 Stretchable Capacitive Sensors 1014.5.3 Stretchable Antennas 1024.5.4 Stretchable Thin-Film Transistors 1034.5.5 Stretchable Organic Lasers 1054.6 Outlook 106 References 107
5 StretchablePiezoelectricNanoribbonsforBiocompatibleEnergyHarvesting 111
YiQi,ThanhD.Nguyen,PrashantK.Purohit,andMichaelC.McAlpine5.1 Energy Harvesting and Piezoelectric Materials 1115.1.1 Introduction to Biomechanical Energy Harvesting 1115.1.2 Piezoelectric Materials and Lead Zirconate Titanate (PZT) 1125.2 PZT Nanofabrication and Interfacing with Stretchable
Substrates 1165.2.1 Wafer-Scale PZT Nanowire Fabrication 1165.2.2 Transfer Printing onto Stretchable Substrates 1175.2.3 Stretchable Wavy and Buckled PZT Nanoribbons 1205.3 Piezoelectric Characterization and Electrical Measurements 1265.3.1 Piezoelectric Characterization 1265.3.2 Electrical Measurements 1305.4 Summary 133 References 134
PartIII CircuitBoards 141
6 ModelingofPrintedCircuitBoardInspiredStretchableElectronicSystems 143
MarioGonzalez,Yung-YuHsu,andJanVanfleteren6.1 Technology Development Considerations 1436.2 Modeling and Simulation 1456.2.1 Optimization of Metal Conductor Shape 1466.2.1.1 Description of the Model 1466.2.1.2 Material Properties 1466.2.1.3 Stress/Strain Comparison of Different Conductor Shapes 1476.2.1.4 Optimization of the Horseshoe Shape of Conductor 1496.2.2 Influence of Substrate Stiffness on the Plastic Strain of the
Conductor 1516.2.3 Induced Mechanical Interaction on Multitracks 1526.2.4 Polyimide-Supported Stretchable Interconnect 155 References 158
VIII Contents
7 MaterialsforStretchableElectronicsCompliantwithPrintedCircuitBoardFabrication 161
MatthiasAdler,RuthBieringer,ThomasSchauber,andJürgenGünther7.1 Introduction 1617.1.1 Silicones 1617.1.1.1 Fundamentals of Silicones 1617.1.1.2 Silicone Elastomers 1637.1.1.3 Durability 1667.1.1.4 Processing 1687.1.1.5 Fields of Application 1707.1.2 Polyurethanes 1717.1.2.1 Fundamentals of Polyurethanes 1717.1.2.2 Properties of Polyurethanes 1757.1.2.3 Thermoplastic Polyurethanes 1767.1.2.4 Cast Polyurethanes 1777.1.2.5 Commercial Raw Materials 1797.1.2.6 Applications of Polyurethanes 1817.1.2.7 Excursion Conductive Pastes (Developed during the STELLA
Project) 182 References 184 Further Reading 185
8 TechnologiesandProcessesUsedinPrintedCircuitBoardFabricationfortheRealizationofStretchableElectronics 187
FrederickBossuytandThomasLöher8.1 Lamination Technology 1878.1.1 Process Concept 1878.1.2 Polyurethane Films 1888.1.3 Printed Circuit Board Cu Foils 1898.1.4 Lamination of Copper Foils to Polyurethane Films 1898.1.5 Substrate Fabrication 1908.1.6 Component Assembly and Interconnection 1938.1.7 Encapsulation of Components 1948.1.8 Outline Cutting of Circuits on the Fabrication Board and Release 1958.1.9 Lamination to Textiles or Other Substrates 1958.2 Molding Technology 1968.2.1 General Introduction of the Process 1968.2.2 Copper as Electrical Conductor 1978.2.3 Polyimide as Mechanical Support 1998.2.4 Lamination of Polyimide–Copper Sheet on Rigid Substrate Using a
Temporary Adhesive 1998.2.5 Copper Patterning 2008.2.6 Solder Mask Application 2008.2.7 Copper Finish Application 2018.2.8 Assembly of Components 2018.2.9 Encapsulation by Molding 202
Contents IX
8.2.10 Application to Textiles 203 References 205
9 ReliabilityandApplicationScenariosofStretchableElectronicsRealizedUsingPrintedCircuitBoardTechnologies 207
JanVanfleteren,FrederickBossuyt,ThomasLöher,Yung-YuHsu,MarioGonzalez,andJürgenGünther
9.1 Application Considerations 2079.2 Reliability 2099.2.1 Results and Discussion of Single and Cyclic Elongation Tests 2099.2.2 One-Time Stretch Tests 2109.2.3 Cyclic Endurance Tests of Laminated and Molded Test Samples 2119.2.3.1 Pure Copper Tracks 2119.2.3.2 PDMS Encapsulated Parallel PI Supported Meander Tracks 2129.2.4 Failure Analysis 2149.2.4.1 In Situ Observation of the Deformation Behavior and Failure
Mechanism of Encapsulated/Nonencapsulated Stretchable Interconnects 214
9.2.4.2 In Situ Electromechanical Measurement for One-Time-Stretching Reliability 216
9.2.4.3 Correlation between Numerical and Experimental Results 2189.2.4.4 Fatigue Failure of Copper Meanders 2199.2.4.5 Lifetime Prediction by FEM 2219.2.5 Washability – An Introduction 2229.3 Application Scenarios 2239.3.1 Temperature Sensor 2239.3.2 Wireless Power Circuit 2249.3.3 Fitness Sensor 2259.3.4 Pressure Senors in a Shoe Insole 2269.3.5 Bandage Inlay for Compression Therapy 2279.3.6 Baby Respiration Monitor Demonstrator 2279.3.7 LED Matrix 2299.3.8 RGB Led Matrix (SMI by Laser) 2309.3.9 Thermoforming of Printed Conductors – Single Stretching 231 Reference 233 Further Reading 233
PartIV DevicesandApplications 235
10 StretchableElectronicandOptoelectronicDevicesUsingSingle-CrystalInorganicSemiconductorMaterials 237
Dae-HyeongKim,NanshuLu,andJohnA.Rogers10.1 Introduction 23710.1.1 Materials Selection for High-Performance Stretchable Electronics 237
X Contents
10.1.2 Monocrystalline Inorganic Semiconductors in Stretchable Designs 238
10.1.3 Bio-integrated Electronics 24010.2 Stretchable Circuits 24010.2.1 Wavy Electronic Devices and Circuits 24010.2.2 Noncoplanar Electronic Devices and Circuits 24210.2.3 Electronic Circuits with Serpentine Interconnects 24410.2.4 Stretchable Electronic Devices on Unconventional Substrates 24410.3 Application of Stretchable Designs to Microscale Inorganic Light
Emitting Diodes (µ-ILEDs) 24710.3.1 Stretchable µ-ILED Arrays 24710.3.2 Lighting Devices on Substrates of Unconventional Materials and
Shapes 24910.4 Biomedical Applications of Stretchable Electronics and
Optoelectronics 25310.4.1 Encapsulation Strategy 25310.4.2 Bio-applications of µ-ILEDs: Suture Threads and Proximity
Sensors 25310.4.3 Minimally Invasive Surgical Tools: Instrumented Balloon
Catheters 25610.4.4 Epidermal Electronic System (EES) 25910.5 Stretchable Digital Imagers and Solar Modules 26110.5.1 Hemispherical Electronic Eye Camera 26110.5.2 Curvilinear Imagers and Stretchable Photovoltaic Modules with High
Fill Factors 26310.5.3 Hemispherical Electronic Eye Camera with Adjustable Zoom
Magnification 26410.6 Conclusions 265 References 267
11 StretchableOrganicTransistors 271 TsuyoshiSekitaniandTakaoSomeya11.1 Introduction 27111.2 Perforated Organic Transistor Active Matrix for Large-Area,
Stretchable Sensors 27211.2.1 Simultaneous Sensing of Pressure and Temperature 27411.3 Rubber-Like Stretchable Organic Transistor Active Matrix Using
Elastic Conductors 27511.3.1 Integration of Elastic Conductors with Printed Organic
Transistors 27611.3.1.1 Integration Process 27611.3.2 Electrical and Mechanical Performances 27811.4 Rubber-Like Organic Transistor Active Matrix Organic Light-Emitting
Diode Display 28011.5 Future Prospects 283
Contents XI
Acknowledgments 283 References 283
12 PowerSupply,Generation,andStorageinStretchableElectronics 287
MartinKaltenbrunnerandSiegfriedBauer12.1 Introduction 28712.2 Radio Frequency Power Supplies 28712.3 Power Generation 28912.3.1 Dielectric Elastomer Generators 29012.3.2 Piezoelectric Energy Generation 29212.3.3 Solar Cells 29412.4 Power Storage 29712.4.1 Supercapacitors 29712.4.2 Batteries 29912.5 Summary 301 Acknowledgments 301 References 301
13 SoftActuators 305 KinjiAsaka13.1 Introduction 30513.2 Conducting Polymers 30613.3 Ionic Polymer Metal Composites (IPMCs) 30813.4 Nanocarbon Actuators 31013.4.1 Carbon Nanotube (CNT) Actuators 31013.4.2 CNT Actuators Based on Ionic-Liquid-Based Bucky-Gels 31113.4.3 Materials of Bucky-Gel Actuators 31313.4.4 Modeling of the Nanocarbon Actuators 31513.5 Applications 31913.6 Conclusion 319 References 320
14 Elastomer-BasedPressureandStrainSensors 325 BenjaminC.K.Tee,StefanC.B.Mannsfeld,andZhenanBao14.1 Introduction 32514.2 A Brief Elastomers Overview 32614.3 Important Sensor Characteristics 32714.3.1 Sensitivity 32814.3.2 Hysteresis 32914.3.3 Temporal Resolution 32914.3.4 Sensitivity to Environmental Factors 33014.3.5 Mechanical Durability 33014.4 Elastomeric Force Sensors 33014.4.1 Piezoresistive Sensors 331
XII Contents
14.4.1.1 Conductive Fillers in Elastomeric Composites 33114.4.2 Elastomer as a Dielectric Material 33514.4.2.1 Plain Elastomers 33614.4.2.2 Foam 33814.4.2.3 Microstructured Elastomers 33914.4.3 Piezoelectric Films 34114.4.4 Optical Pressure Sensors 34214.5 Active Pressure/Strain Sensors Systems 34314.6 Applications 34814.7 Outlook 348 References 350
15 ConformableActiveDevices 355 RobertA.StreetandAnaClaudiaArias15.1 Introduction 35515.2 Printing Processes for Organic TFTs 35615.2.1 Printing Considerations for Metals, Semiconductors, and
Dielectrics 35615.2.2 Printed Organic CMOS TFTs 35915.2.3 Alternative Material Choices 36015.2.4 Self-Assembly of TFTs from Solution 36115.3 Sensing and Memory Devices Based on Piezoelectric Polymer 36315.3.1 Pressure Sensor and Accelerometer 36315.3.2 Chemical Sensors 36415.3.3 Nonvolatile Printed Memory 36515.3.4 Printed Memristor 36615.3.5 Photodiodes and Other Devices 36715.4 Electronic Circuits 36815.4.1 All-Printed Organic TFT Display 36915.4.2 Inverter, Ring Oscillator, and Shift Register 37115.4.3 Self-Stabilized Amplifier Circuits 37215.5 Curved Conformal Devices by a Cut-and-Bend Approach 37415.6 Summary 375 Acknowledgments 376 References 376
16 StretchableNeuralInterfaces 379 WooHyeunKang,WenzheCao,SigurdWagner,andBarclayMorrison,III16.1 Introduction 37916.2 Overview of MEAs 38016.2.1 Advantages of Stretchable MEAs 38116.3 Classes of SMEAs 38216.3.1 Planar SMEAs 38216.3.2 Cuff SMEAs 38916.4 Common Limitations for All SMEAs 394
Contents XIII
16.5 Future Directions in Stretchable Neural Interfaces 39416.6 Conclusion 395 References 396
17 Bio-basedMaterialsasTemplatesforElectronicDevices 401 ChristianMüllerandOlleInganäs17.1 Introduction 40117.2 Polysaccharide-Based Templates 40217.2.1 Cellulose: Paper Substrates 40217.2.2 Cellulose: Nanofiber Networks 40317.2.3 Cellulose Fibers: Cotton, Lyocell, and Viscose 40717.2.4 Vascular Bundles 40717.2.5 Polysaccharide Hydrogels 40817.3 Protein-Based Templates 40917.3.1 Wool and Silk Fibers 40917.3.2 Silk Fibroin Films 41017.3.3 Protein Fibrils: Rhapidosomes, Microtubules, Actin Filaments, and
Amyloid Fibrils 41317.3.4 Collagen and Gelatin 41517.4 DNA Templates 41517.4.1 Intrinsic Electrical Properties of DNA 41517.4.2 Decorated DNA 41617.5 Virus Templates: Tobacco Mosaic Virus and M13 Bacteriophage 41817.6 Summary 419 References 420
18 OrganicIntegratedCircuitsforEMIMeasurement 431 MakotoTakamiya,KoichiIshida,TsuyoshiSekitani,TakaoSomeya,
andTakayasuSakurai18.1 Introduction 43118.2 Stretchable EMI Measurement Sheet 43218.2.1 Overview of Stretchable EMI Measurement Sheet 43218.2.2 2 V Organic CMOS Decoder 43418.2.3 Stretchable Interconnects with CNTs 43618.3 Silicon CMOS LSI for EMI Detection 43718.4 Experimental Results and Discussion 44018.4.1 Direct Silicon–Organic Circuit Interface 44018.4.2 Comparison of Conventional and Proposed EMI Measurements 44218.4.3 Calibration for EMI Measurement LSI 44318.5 Conclusion 446 Acknowledgments 447 References 447
Index 449
XV
Today’s electronics are bulky and rigid since they are manufactured on rigid sub-strates such as glass and/or silicon; however, the next-generation electronics will be manufactured on polymeric foils, subsequently going to be flexible and even stretchable.
Objects that surround our everyday life have very complicated shapes. In fact, most ambient tools are composed of round/curvy surfaces rather than flat glass/silicon wafers. Imagine overlaying a machine such as a humanoid robot with a skin-like sensor sheet. For a joint part of a robot, the sensor sheet needs to be extremely stretchable to accommodate the twisting or bending motion of the joint. In order to mask the sensor sheet to a surface with complex, intricate curves, “stretchability” is the key. As a result, electronics that are as flexible as films, and as stretchy as rubber sheets, will soon replace the traditional solid electronics. Future electronics will be highly deformable and will adapt their shapes by stretching, shrinking, and wrinkling as desired. Expectations are unlimited and abundant. Emerging applications will be realized when new elec-tronics adopt their stretchability.
This book, which has four parts, comprises 18 chapters. Part I introduces the theory of stretchable electronics and mechanics of twistable electronics. Here, deformation analysis and postbuckling theory are described. Part II puts together materials and processes. Graphene-based stretchable electrodes, polydimethyl-siloxane (PDMS) substrates, and stretchable piezoelectric nanoribbons are pre-sented as candidate materials for stretchable electronics. In Part III, stretchable circuit boards and related technologies ranging from modeling, materials, pro-cesses, device reliability, and applications are reported. Part IV covers novel stretchable applications of stretchable electronics which are made of inorganic and organic semiconductors. In addition to stretchable transistor integrated circuits and other conformable active devices, stretchable actuators, sensors, and stretch-able power sources are described. Bio-inspired and bio-medical applications are important and bio-based materials are introduced for electronics devices. Novel applications include stretchable systems to measure electromagnetic interference and signals from neurons.
Preface
XVI Preface
I would like to express my sincere gratitude to all our colleagues and friends involved in the realization of this book. I greatly appreciate them for agreeing to devote their time and effort to submitting and reviewing chapters to ensure its success. I am also indebted to Wiley-VCH for publication of this book.
Takao SomeyaTokyo, October 2012
XVII
Matthias AdlerFreudenberg Forschungsdienste SE & Co. KGHöhnerweg 2-469469 WeinheimGermany
Jong-Hyun AhnSungkyunkwan UniversitySchool of Advanced Materials Science and EngineeringSuwon, 440-746Korea
Ana Claudia AriasUniversity of CaliforniaEECS DepartmentBerkeley, CA 94720USA
Kinji AsakaNational Institute of Advanced Industrial Science and Technology (AIST)Health Research Institute1-8-31 MidorigaokaIkedaJapan
ListofContributors
Zhenan BaoStanford UniversityDepartment of Chemical Engineering381 North South MallStanford, CA 94305USA
Siegfried BauerJohannes Kepler University LinzSoft Matter PhysicsAltenbergerstraße 694040 LinzAustria
Ruth BieringerFreudenberg Forschungsdienste SE & Co. KGHöhnerweg 2-469469 WeinheimGermany
Frederick BossuytUniversity Ghent9052 Gent-ZwijnaardeBelgium
Frederick BossuytCentre for Microsystems TechnologyGhent University and Interuniversity Microelectronics CentreTechnology Park, Building 914-A9052 Gent-ZwijnaardeBelgium
XVIII ListofContributors
Wenzhe CaoPrinceton UniversityDepartment of Electrical Engineering and Princeton Institute for the Science and Technology of MaterialsF310 Engineering QuadOlden StreetPrinceton, NJ 08544USA
Zhichao FanTsinghua UniversityDepartment of Engineering MechanicsBeijing, 100084China
Mario GonzalezThe Interuniversity Microelectronics Center IMECKapeldreef 753001 LeuvenBelgium
Jürgen GüntherFreudenberg Forschungsdienste SE & Co. KGHöhnerweg 2-469469 WeinheimGermany
Yung-Yu HsuThe Interuniversity MicroElectronics Center IMECKapeldreef 753001 LeuvenBelgiumPresent address: MC10 Inc.36 Cameron Ave.MA 02140USA
Yonggang HuangNorthwestern UniversityDepartments of Civil and Environmental Engineering and Mechanical EngineeringEvanston, IL 60208USA
Keh-Chih HwangTsinghua UniversityDepartment of Engineering MechanicsBeijing, 100084China
Olle InganäsLinköping UniversityBiomolecular and Organic ElectronicsDepartment of Physics, Chemistry and Biology58183 LinköpingSweden
Koichi IshidaUniversity of TokyoTokyo 153-8505Japan
Houk JangSungkyunkwan UniversitySchool of Advanced Materials Science and EngineeringSuwon, 440-746Korea
Martin KaltenbrunnerJohannes Kepler University LinzSoft Matter PhysicsAltenbergerstraße 694040 LinzAustria
ListofContributors XIX
Woo Hyeun KangColumbia UniversityDepartment of Biomedical Engineering351 Engineering TerraceMC 89041210 Amsterdam AvenueNew York, NY 10027USA
Dae-Hyeong KimSeoul National UniversitySchool of Chemical and Biological EngineeringSeoul, 151-744Korea
Stéphanie P. LacourCenter for NeuroprostheticsEPFL | STI | IMT/IBI | LSBI Station 17CH-1015 Lausanne Switzerland
Seoung-Ki LeeSungkyunkwan UniversitySchool of Advanced Materials Science and EngineeringSuwon, 440-746Korea
Thomas LöherFraunhofer IZMGustav-Meyer-Allee 2513355 BerlinGermany
Nanshu LuDepartment of Aerospace Engineering and Engineering MechanicsUniversity of Texas at Austin405 N Mathews St.Austin, TX 78712USA
Stefan C.B. MannsfeldStanford UniversityDepartment of Chemical Engineering381 North South MallStanford, CA 94305USA
Michael C. McAlpinePrinceton UniversityDepartment of Mechanical and Aerospace EngineeringEngineering QuadOlden StreetPrinceton, NJ 08544USA
Barclay Morrison, IIIColumbia UniversityDepartment of Biomedical Engineering351 Engineering TerraceMC 89041210 Amsterdam AvenueNew York, NY 10027USA
Christian MüllerDepartment of Chemical and Biological Engineering/Polymer TechnologyChalmers University of Technology41296 GöteborgSweden
Thanh D. NguyenPrinceton UniversityDepartment of Mechanical and Aerospace EngineeringEngineering QuadOlden StreetPrinceton, NJ 08544USA
XX ListofContributors
Prashant K. PurohitUniversity of Pennsylvania Department of Mechanical Engineering and Applied Mechanics220 South 33rd Street Philadelphia, PA 19104-6391USA
Yi QiPrinceton UniversityDepartment of Mechanical and Aerospace EngineeringEngineering QuadOlden StreetPrinceton, NJ 08544USA
John A. RogersUniversity of IllinoisDepartment of Materials Science and EngineeringUrbana, IL 61801USA
John A. RogersUniversity of Illinois at Urbana-ChampaignDepartment of Materials Science and EngineeringBeckman Institute for Advanced Science and Technology and Frederick Seitz Materials Research LaboratoryUrbana, IL 61801USA
Takayasu SakuraiUniversity of TokyoTokyo 153-8505Japan
Thomas SchauberFreudenberg Forschungsdienste SE & Co. KGHöhnerweg 2-469469 WeinheimGermany
Tsuyoshi SekitaniThe University of Tokyo Department of Electrical Engineering and Information Systems 7-3-1 Hongo Bunkyo-ku Tokyo 113-8656Japan
Takao SomeyaThe University of TokyoDepartment of Electrical Engineering and Information Systems 7-3-1 HongoBunkyo-kuTokyo 113-8656Japan
Jizhou SongUniversity of MiamiDepartment of Mechanical and Aerospace EngineeringCoral Gables, FL 33146USA
Robert A. StreetPalo Alto Research Center3333 Coyote Hill RoadPalo Alto, CA 94304USA
Yewang SuTsinghua UniversityDepartment of Engineering MechanicsBeijing, 100084China
ListofContributors XXI
Makoto TakamiyaUniversity of TokyoTokyo 153-8505Japan
Benjamin C.K. TeeStanford UniversityDepartment of Electrical EngineeringDavid Packard Building350 Serra MallStanford, CA 94305USA
Jan VanfleterenCentre for Microsystems TechnologyGhent University and Interuniversity Microelectronics CentreTechnology Park, Building 914-A9052 Gent-ZwijnaardeBelgium
Thomas VervustCentre for Microsystems TechnologyGhent University and Interuniversity Microelectronics CentreTechnology Park, Building 914-A9052 Gent-ZwijnaardeBelgium
Sigurd WagnerPrinceton UniversityDepartment of Electrical Engineering and Princeton Institute for the Science and Technology of MaterialsB422 Engineering QuadOlden StreetPrinceton, NJ 08544USA
Shuodao WangNorthwestern UniversityDepartment of Mechanical EngineeringEvanston, IL 60208USA
Jian WuTsinghua UniversityDepartment of Engineering MechanicsBeijing, 100084China
Chao YanSungkyunkwan UniversitySchool of Advanced Materials Science and EngineeringSuwon, 440-746Korea
Part ITheory
1
3
Theory for Stretchable InterconnectsJizhouSongandShuodaoWang
1.1 Introduction
A rapidly growing range of applications demand electronic systems that cannot be formed in the conventional manner on semiconductor wafers. The most prominent example is stretchable electronics, which has a performance equal to established technologies that use rigid semiconductor wafers, but in formats that can be stretched and compressed. It enables many application possibilities such as flexible displays [1], electronic eye camera [2–4], conformable skin sensors [5], smart surgical gloves [6], and structural health monitoring devices [7]. There are primarily two directions to make stretchable electronics. One is to use intrinsically stretchable materials such as organic materials [8–13]. However, the electrical performance of organic semiconductor materials is relatively poor comparing with the welldeveloped, highperformance inorganic electronic materials. The other direction to achieve stretchable electronics is to use conventional semiconductors, such as silicon, and make the system stretchable. The main challenge here is to make siliconbased structures stretchable since the brittleness of silicon makes it almost impossible to be stretched. Many researches bypassed this difficulty by using stretchable interconnects [14–22].
One of the most intuitive approaches to develop stretchable interconnects is to exploit outofplane deflection in thin layers to accommodate strains applied in the plane. Figure 1.1 illustrates some examples of this concept. In the first case (Figure 1.1a) [17, 24, 25] of stretchable wavy ribbons, the initially flat ribbons are bonded to a prestrained elastomeric substrate. The prestrain can be induced by mechanical (or thermal) stretch along the ribbon directions. Releasing the prestrain causes a compression in the ribbon, and this compression leads to a nonlinear buckling response and results in a wavy profile. When the wavy structure is subject to stretches, the amplitudes and periods of the waves change to accommodate the deformation. In the second case (Figure 1.1b) of popup structure [26], the ribbons can be designed to bond the prestretched elastomeric substrate only at certain locations. When the prestrain is released, the ribbon on the nonbonded regions delaminates from the substrate and forms popup profile. Compared to Figure 1.1a,
1
Stretchable Electronics, First Edition. Edited by Takao Someya.© 2013 WileyVCH Verlag GmbH & Co. KGaA. Published 2013 by WileyVCH Verlag GmbH & Co. KGaA.
4 1 TheoryforStretchableInterconnects
this layout has the advantage that the wavelengths can be defined precisely with a level of engineering control to have higher stretchability.
Combining the stretchable interconnects in Figure 1.1a (or Figure 1.1b) with rigid device islands, an interconnectisland structure [16, 19, 20, 22] can be developed to accommodate the deformations. Mechanical response to stretching or compression involves, primarily, deformations only in these interconnects, thereby avoiding unwanted strains in the regions of the active devices. Lacour et al. [16] and Kim et al. [19] developed a coplanar mesh design by using the wavelike interconnects, which are bonded with the substrate. Although such a coplanar mesh design can improve the stretchability to around 40%, the stretchability is still small for certain applications. Kim et al. [20] developed a noncoplanar mesh design (Figure 1.1c), consisting of device islands linked by popup interconnects for stretchable circuits, which can be stretched to rubberlike levels of strain (e.g., up to 100%). To further increase the stretchability, serpentine interconnects [14, 15, 19–22] can be used. Compared to the straight interconnects, the serpentine ones can accommodate larger deformation because they are much longer and can involve large twist to reduce the strains in the interconnects.
Figure 1.1 SEM images of (a) stretchable wavy ribbons, (b) popup structure, (c) noncoplanar mesh design with straight interconnects, and (d) noncoplanar mesh design with serpentine interconnects.
(Reprinted with permission from Ref. [15] Copyright 2007 American Institute of Physics and Ref. [23] Copyright 2009 American Vacuum Society).
(a) (b)
(c) (d)
1.2MechanicsofStretchableWavyRibbons 5
Figure 1.1d shows a SEM image of serpentine interconnects used in the noncoplanar mesh design.
For serpentine interconnects, there are no theoretical work, and many researchers have developed numerical models to study their deformations due to their complex geometries [14, 15, 19–22]. The related review is not the focus of this chapter. Here, we will review the theoretical aspects related to the designs in Figure 1.1a–c. Mechanics of stretchable wavy ribbons (Figure 1.1a) is described in Section 1.2. Analysis for small and large strains and width effect are discussed in this section. Section 1.3 describes the mechanics of popup structure (Figure 1.1b). Section 1.4 reviewed the mechanics of interconnects in the noncoplanar mesh design (Figure 1.1c). Interfacial adhesion and large deformation effect are also discussed in this section.
1.2 Mechanics of Stretchable Wavy Ribbons
The fabrication of stretchable wavy ribbons is illustrated in Figure 1.2. The flat ribbon is first chemically bonded to a prestrained compliant substrate. When the prestrain is released, the ribbon is compressed to generate the wavy layout through a nonlinear buckling response. These wavy layouts can accommodate external deformations through changes in wavelength and amplitude, which is also shown in Figure 1.2.
1.2.1 Small-Deformation Analysis
Several models [28, 29] have been developed to explain the mechanics of stretchable wavy ribbons under small deformations. For example, Huang et al. [29] developed an energy method to determine the buckling profile. The thin ribbon is modeled as an elastic nonlinear von Karman beam since its thickness is much smaller compared with other characteristic lengths (e.g., wavelength). The substrate is modeled as a semiinfinite solid because its thickness (∼mm) is much larger than that (∼µm) of film. The total energy consists of the bending energy Ub and membrane energy Um in the thin film and strain energy Us in the substrate.
For a stiff thin film (ribbon) with thickness hf, Young’s modulus Ef and Poisson’s ratio vf on a prestrained compliant substrate with prestrain εpre, Young’s modulus Es, and Poisson’s ratio vs, the wavy profile forms with the outofplane displacement:
w A kx Ax= ( ) =
cos cos1
12πλ
(1.1)
when the prestrain is released. Here, x1 is the coordinate along the ribbon direction, A is the amplitude, λ is the wavelength, and k = 2π/λ is the wave number.
6 1 TheoryforStretchableInterconnects
A and λ (or k) are to be determined by minimizing the total energy. The bending energy Ub can be obtained by
U LE h w
xx
E h ALb
f f f fd
dd=
=∫0
3 2
2
2
0
4 3 2
4 01
24 3λπ
λ
λ
(1.2)
where L0 and E Ef f f= −( )1 2ν are the length and planestrain modulus of the thin film, respectively.
The membrane strain ε11, which determines the membrane energy in the ribbon, is related to the inplane displacement u1 and outofplane displacement w by εmembrane = du1/dx1 + (dw/dx1)2/2 − εpre. The membrane force Nmembrane is given by N E hmembrane f f membrane= ε . The interfacial shear is negligible [29] and the force equilibrium equation becomes dN11/dx1 = 0, which gives a uniform membrane force and therefore a uniform membrane strain:
ε πλ
εmembrane pre= −2 2
2
A (1.3)
Figure 1.2 Schematic illustration of the process for fabricating buckled, or “wavy,” single crystal Si ribbons on a PDMS substrate. (Reprinted with permission from Ref. [27] Copyright 2009 American Vacuum Society).
Bond Si nanoribbons to prestrained PDMS
L+dLSi
PDMS
Release prestrain
L
StretchableSi device
Compress Stretch