A-444. Adaptive PolCarr carriers for novel applications in life sciences. Heidemarie Schmidt

Size: px
Start display at page:

Download "A-444. Adaptive PolCarr carriers for novel applications in life sciences. Heidemarie Schmidt"

Transcription

1 A-444 Adaptive PolCarr carriers for novel applications in life sciences Heidemarie Schmidt Nano-Spintronics Group Department of Materials for Nanoelectronics Chemnitz University of Technology

2 Outlook Polarizable materials and electrostatic forces Charge-patterned silicon wafers Detection of surface-near electrostatic forces (SNEF) Carriers for nonlocal and local adsorption of polarizable materials PolCarr carriers for novel applications in life sciences Summary 2

3 Collaborations & Acknowledgments K. Wiesenhütter, I. Skorupa, U. Wiesenhütter, A. Kolitsch, W. Skorupa, J. Raff/ Helmholtz-Zentrum Dresden-Rossendorf O.G. Schmidt/ TU Chemnitz, IFW Dresden M. Rüb/ EAH Jena A.-D. Müller/ Anfatec Instruments AG J. Meyer, D. Teichmann, S. Friedrich-Löbelt, K. Rosenkranz, T. Förster/ Ascenion GmbH M. Müller, P. Uhlmann/ IPF Dresden A.-K. Meyer/ Klinik für Neurologie, TU Dresden J. Pahnke/ Section of Neuropathology, University of Oslo O. Deschaumes, C.Bartic/ Soft Matter and Biophysics, KU Leuven G. Ettenberger/ Pharma, Medizinprodukte und Hygiene, OFI Wien F.W. Falkenberg / CIRES GmbH 3

4 Polarizable materials and electrostatic forces

5 Polarizable materials with electric dipole p Molecule where electrons are concentrated in one place has instantaneous dipole p Molecule with two atoms with different electronegativity has permanent dipole p Molecule where electrons are repelled by permanent dipole of another molecule has induced dipole p Water molecule in vapour, p=1.85 D Cis isomer, p=1.90 D Trans isomer, p=0 D 5 5

6 Electrostatic forces F Charges create electric field E. Long-range ( nm) Coulomb force F between charges + - Dipole moment p tends to align in an electric field E p E No labeling of polarizable material needed. Many molecules and biomaterials are polarizable. 6

7 Electrostatic forces between molecules Attractive force - Repulsive force + + Anionic polymer Cationic polymer Cationic polymer Advances in Polymer Science 255 & 256 (Ed.: Martin Müller), Springer,

8 Charge-patterned silicon wafers 8

9 Small charge/area concentration Frictional electrostatic generator negative (-) charge on rasps positive (+) charge on glass plate Bottle battery consisting of 25 Leyden jars (inside (+) & outside (-) metal-coated glas) (Deutsches Museum München, Inv. Nr. 3920) Leyden jar (battery) Charges/area: e/m 2 1 e/(100 nm x100 nm) 9

10 Large charge/area concentration F F kv DANFYSIK 1090, High current ion implanter 500 kv ion implanter Length scale:1 mm - 1 mm - 1 nm Implanted silicon wafer Charges/area: e/m 2 1 e/(1 nm x1 nm) 10

11 Detection of surface-near electrostatic forces (SNEF) 11

12 Probing SNEF by KPFM Kelvin probe force microscopy (KPFM) Minimization of electrostatic forces acting on the cantilever (vibration amplitude f ac ) by applying the appropriate KPFM bias U K to the sample backside. Topography (resonance frequency f r, vibration amplitude ~10 nm) and KPFM bias U K (operation frequency f ac, vibration amplitude < 20 pm) probed simultaneously. 12

13 Probing SNEF by KPFM Minimization of the SNEF by accumulation of mobile majority charge carriers in the surface region of the doped semiconductor KPFM bias applied to sample backside is related with energy difference between Fermi energy E F and respective band edge [2] Picture: Sander Münster, Kunstkosmos Doped Si cantilevers (NSC15, k=46 N/m): f ac =5 khz-130 khz < f r =265 khz-400 khz C. Baumgart, M. Helm, H. Schmidt, Phys. Rev. B 80 (2009) 13

14 Carriers for nonlocal and local adsorption of polarizable materials: 3 Proof-of-Concept (PoC) 14

15 Nonlocal adsorption of polarizable material Carrier A: Si substrate with polyelectrolyte coating T.J. Günther, M. Suhr, J. Raff, K. Pollmann, Immobilization of microorganisms for AFM studies in liquids, RCS Adv. 4 (2014)

16 PoC with microorganisms on carrier A A Viridibacillus arvi JG-B58 B Lysinibacillus sphaericus JG-B53, OD 600 =0.05 C E.coli, OD 600 =0.10 D E.coli, OD 600 =0.05 OD 600 : optical density of cells in a 600 nm Successful immobilization for AFM studies in liquids T.J. Günther, M. Suhr, J. Raff, K. Pollmann, RCS Adv. 4 (2014) 16

17 Nonlocal adsorption of polarizable material Carrier B: Si cantilever with SiO 2 coating O. Bäumchen et al., Vom Photolack zum Gecko, Physik Journal 14 (2015)

18 Frequency in percent Frequency in percent PoC with bacteria on carrier B Hydrophilic surface Hydrophobic surface Adhesive power in nn Adhesive power in nn Force F increases with decreasing SiO 2 thickness O. Bäumchen et al., Vom Photolack zum Gecko, Physik Journal 14 (2015)

19 Local adsorption of polarizable material Carrier C: PolCarr carrier Charge-patterned silicon wafer Dipping/spin-coating in/of solution with polarizable material Local attachment of polarizable material on PolCarr carrier H. Schmidt, S. Habicht, S. Feste, A.-D. Müller, O.G. Schmidt, Appl. Surf. Sci. 281 (2013) 19

20 Local adsorption of polarizable material Diethylaminoethyl-Dextran-FITC (DEAE-FITC) (Ø=10-20 nm (ph=9), l=200 nm (ph=4)) Local P-implantation of n + -Si stripes (5 mm width, 15 mm periodicity) into n-si Dipping at ph=11 (1 mg/ml) ph=9 ph=4 Rinsing (5 min, dest. water) Drying (10 min, 50 C) Advances in Polymer Science 255 & 256 (Ed.: Martin Müller), Springer, 2014 H. Schmidt, S. Habicht, S. Feste, A.-D. Müller, O.G. Schmidt, Appl. Surf. Sci. 281 (2013) 20

21 Positively charged molecule (DEAE-FITC) Cationic polymer diethylaminoethyl-dextran-fitc (DEAE-FITC) + ph=9 ph=4 + Monomer molar mass: 231g/mol Polymer molar mass: g/mol Charges per monomer unit: 0.5 Branched topology, Labeled with Fluoresceinisothiocyanat/FITC Coiled chain (ph=9): Ø=10-20 nm Elongated chain (ph=4): l=200 nm Advances in Polymer Science 255 & 256 (Ed.: Martin Müller), Springer,

22 PoC with DEAE-FITC on carrier C 10 mm 100% coating of n + -Si-stripes with DEAE-FITC Standard Si wafer: <20% coating 22

23 PolCarr for novel applications in life sciences 23

24 Fabrication of PolCarr carriers Design of photolithography mask Selection of implantation parameters Ion implantation Dopant activation Deposition of biocompatible thin film 24

25 Microwell plates with PolCarr bottom plate 25

26 Microwell plates with PolCarr bottom plate Charge-pattern in PolCarr bottom plate (implanted Si wafer) for local attachment of polarizable biomaterials and for adherent cell growth is defined by implantation pattern and by species of implanted ions. 26

27 Summary Charges in implanted silicon wafers create SNEF SNEF probed by Kelvin probe force microscopy PolCarr carriers with SNEF pattern for local attachment of polarizable materials retaining functionality during: Autoclaving for sterilization (+121 C, high pressure steam, min) Incubation for cell growth (+37 C, ph, CO 2, O 2, N 2, hours-days) Cryogenic applications for shock freezing (-196 C, days-weeks-months) 27

28 Thank you for your attention. PD Dr. Heidemarie Schmidt Nano-Spintronics Group Department of Materials for Nanoelectronics Chemnitz University of Technology Phone:

Basic Laboratory. Materials Science and Engineering. Atomic Force Microscopy (AFM)

Basic Laboratory. Materials Science and Engineering. Atomic Force Microscopy (AFM) Basic Laboratory Materials Science and Engineering Atomic Force Microscopy (AFM) M108 Stand: 20.10.2015 Aim: Presentation of an application of the AFM for studying surface morphology. Inhalt 1.Introduction...

More information

Deposition of exchange-coupled dinickel complexes. on gold substrates utilizing ambidentate mercaptocarboxylato

Deposition of exchange-coupled dinickel complexes. on gold substrates utilizing ambidentate mercaptocarboxylato Deposition of exchange-coupled dinickel complexes on gold substrates utilizing ambidentate mercaptocarboxylato ligands Martin Börner 1, Laura Blömer 1, Marcus Kischel 1, Peter Richter 2, Georgeta Salvan

More information

Lecture 12: Biomaterials Characterization in Aqueous Environments

Lecture 12: Biomaterials Characterization in Aqueous Environments 3.051J/20.340J 1 Lecture 12: Biomaterials Characterization in Aqueous Environments High vacuum techniques are important tools for characterizing surface composition, but do not yield information on surface

More information

Atomic Force Microscopy imaging and beyond

Atomic Force Microscopy imaging and beyond Atomic Force Microscopy imaging and beyond Arif Mumtaz Magnetism and Magnetic Materials Group Department of Physics, QAU Coworkers: Prof. Dr. S.K.Hasanain M. Tariq Khan Alam Imaging and beyond Scanning

More information

Scanning Probe Microscopy (SPM)

Scanning Probe Microscopy (SPM) Scanning Probe Microscopy (SPM) Scanning Tunneling Microscopy (STM) --- G. Binnig, H. Rohrer et al, (1982) Near-Field Scanning Optical Microscopy (NSOM) --- D. W. Pohl (1982) Atomic Force Microscopy (AFM)

More information

General concept and defining characteristics of AFM. Dina Kudasheva Advisor: Prof. Mary K. Cowman

General concept and defining characteristics of AFM. Dina Kudasheva Advisor: Prof. Mary K. Cowman General concept and defining characteristics of AFM Dina Kudasheva Advisor: Prof. Mary K. Cowman Overview Introduction History of the SPM invention Technical Capabilities Principles of operation Examples

More information

Scanning Tunneling Microscopy

Scanning Tunneling Microscopy Scanning Tunneling Microscopy Scanning Direction References: Classical Tunneling Quantum Mechanics Tunneling current Tunneling current I t I t (V/d)exp(-Aφ 1/2 d) A = 1.025 (ev) -1/2 Å -1 I t = 10 pa~10na

More information

INTRODUCTION TO BIOPHYSICS. II semester, week /2015

INTRODUCTION TO BIOPHYSICS. II semester, week /2015 INTRODUCTION TO BIOPHYSICS II semester, week 3 2014/2015 INTRODUCTION TO ELECTRICITY Electricity phenomena associated with interaction between electrically charged objects PARTICLES AND ELECTRIC CHARGE

More information

Contents. Preface XI Symbols and Abbreviations XIII. 1 Introduction 1

Contents. Preface XI Symbols and Abbreviations XIII. 1 Introduction 1 V Contents Preface XI Symbols and Abbreviations XIII 1 Introduction 1 2 Van der Waals Forces 5 2.1 Van der Waals Forces Between Molecules 5 2.1.1 Coulomb Interaction 5 2.1.2 Monopole Dipole Interaction

More information

AFM Imaging In Liquids. W. Travis Johnson PhD Agilent Technologies Nanomeasurements Division

AFM Imaging In Liquids. W. Travis Johnson PhD Agilent Technologies Nanomeasurements Division AFM Imaging In Liquids W. Travis Johnson PhD Agilent Technologies Nanomeasurements Division Imaging Techniques: Scales Proteins 10 nm Bacteria 1μm Red Blood Cell 5μm Human Hair 75μm Si Atom Spacing 0.4nm

More information

Intermittent-Contact Mode Force Microscopy & Electrostatic Force Microscopy (EFM)

Intermittent-Contact Mode Force Microscopy & Electrostatic Force Microscopy (EFM) WORKSHOP Nanoscience on the Tip Intermittent-Contact Mode Force Microscopy & Electrostatic Force Microscopy (EFM) Table of Contents: 1. Motivation... 1. Simple Harmonic Motion... 1 3. AC-Mode Imaging...

More information

Scanning Probe Microscopy. Amanda MacMillan, Emmy Gebremichael, & John Shamblin Chem 243: Instrumental Analysis Dr. Robert Corn March 10, 2010

Scanning Probe Microscopy. Amanda MacMillan, Emmy Gebremichael, & John Shamblin Chem 243: Instrumental Analysis Dr. Robert Corn March 10, 2010 Scanning Probe Microscopy Amanda MacMillan, Emmy Gebremichael, & John Shamblin Chem 243: Instrumental Analysis Dr. Robert Corn March 10, 2010 Scanning Probe Microscopy High-Resolution Surface Analysis

More information

Imaging Methods: Scanning Force Microscopy (SFM / AFM)

Imaging Methods: Scanning Force Microscopy (SFM / AFM) Imaging Methods: Scanning Force Microscopy (SFM / AFM) The atomic force microscope (AFM) probes the surface of a sample with a sharp tip, a couple of microns long and often less than 100 Å in diameter.

More information

Module 26: Atomic Force Microscopy. Lecture 40: Atomic Force Microscopy 3: Additional Modes of AFM

Module 26: Atomic Force Microscopy. Lecture 40: Atomic Force Microscopy 3: Additional Modes of AFM Module 26: Atomic Force Microscopy Lecture 40: Atomic Force Microscopy 3: Additional Modes of AFM 1 The AFM apart from generating the information about the topography of the sample features can be used

More information

CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS. Chemistry 1411 Joanna Sabey

CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS. Chemistry 1411 Joanna Sabey CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS Chemistry 1411 Joanna Sabey Forces Phase: homogeneous part of the system in contact with other parts of the system but separated from them by a

More information

Intermolecular Forces and Liquids and Solids Chapter 11

Intermolecular Forces and Liquids and Solids Chapter 11 Intermolecular Forces and Liquids and Solids Chapter 11 A phase is a homogeneous part of the system in contact with other parts of the system but separated from them by a well defined boundary. Phases

More information

MEEN Nanoscale Issues in Manufacturing. Lithography Lecture 1: The Lithographic Process

MEEN Nanoscale Issues in Manufacturing. Lithography Lecture 1: The Lithographic Process MEEN 489-500 Nanoscale Issues in Manufacturing Lithography Lecture 1: The Lithographic Process 1 Discuss Reading Assignment 1 1 Introducing Nano 2 2 Size Matters 3 3 Interlude One-The Fundamental Science

More information

Instrumentation and Operation

Instrumentation and Operation Instrumentation and Operation 1 STM Instrumentation COMPONENTS sharp metal tip scanning system and control electronics feedback electronics (keeps tunneling current constant) image processing system data

More information

L8: The Mechanics of Adhesion used by the Gecko

L8: The Mechanics of Adhesion used by the Gecko L8: The Mechanics of Adhesion used by the Gecko With help from Bo He Overview Gecko s foot structure Intermolecular force Measurement: 2-D MEMS sensor Gecko s adhesive mechanism Measurement results discussion

More information

Review of Semiconductor Fundamentals

Review of Semiconductor Fundamentals ECE 541/ME 541 Microelectronic Fabrication Techniques Review of Semiconductor Fundamentals Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Page 1 Semiconductor A semiconductor is an almost insulating material,

More information

ECE 340 Lecture 39 : MOS Capacitor II

ECE 340 Lecture 39 : MOS Capacitor II ECE 340 Lecture 39 : MOS Capacitor II Class Outline: Effects of Real Surfaces Threshold Voltage MOS Capacitance-Voltage Analysis Things you should know when you leave Key Questions What are the effects

More information

Abstract. The principles and applicability of surface structure and hydrophobicity of polymers (PS, PDMS),

Abstract. The principles and applicability of surface structure and hydrophobicity of polymers (PS, PDMS), Contact Angle Goniometer: Hydrophobicity of Biomaterial Surfaces and Protein Coatings Eman Mousa Alhajji North Carolina State University Department of Materials Science and Engineering MSE 255 Lab Report

More information

Ecole Franco-Roumaine : Magnétisme des systèmes nanoscopiques et structures hybrides - Brasov, Modern Analytical Microscopic Tools

Ecole Franco-Roumaine : Magnétisme des systèmes nanoscopiques et structures hybrides - Brasov, Modern Analytical Microscopic Tools 1. Introduction Solid Surfaces Analysis Group, Institute of Physics, Chemnitz University of Technology, Germany 2. Limitations of Conventional Optical Microscopy 3. Electron Microscopies Transmission Electron

More information

Atomic and molecular interactions. Scanning probe microscopy.

Atomic and molecular interactions. Scanning probe microscopy. Atomic and molecular interactions. Scanning probe microscopy. Balázs Kiss Nanobiotechnology and Single Molecule Research Group, Department of Biophysics and Radiation Biology 27. November 2013. 2 Atomic

More information

Nanotechnology Fabrication Methods.

Nanotechnology Fabrication Methods. Nanotechnology Fabrication Methods. 10 / 05 / 2016 1 Summary: 1.Introduction to Nanotechnology:...3 2.Nanotechnology Fabrication Methods:...5 2.1.Top-down Methods:...7 2.2.Bottom-up Methods:...16 3.Conclusions:...19

More information

Electrochemically Exfoliated Graphene as Solution-Processable, Highly-Conductive Electrodes for Organic Electronics

Electrochemically Exfoliated Graphene as Solution-Processable, Highly-Conductive Electrodes for Organic Electronics Supporting Information Electrochemically Exfoliated Graphene as Solution-Processable, Highly-Conductive Electrodes for Organic Electronics Khaled Parvez, Rongjin Li, Sreenivasa Reddy Puniredd, Yenny Hernandez,

More information

Supplementary Figure 1 Dark-field optical images of as prepared PMMA-assisted transferred CVD graphene films on silicon substrates (a) and the one

Supplementary Figure 1 Dark-field optical images of as prepared PMMA-assisted transferred CVD graphene films on silicon substrates (a) and the one Supplementary Figure 1 Dark-field optical images of as prepared PMMA-assisted transferred CVD graphene films on silicon substrates (a) and the one after PBASE monolayer growth (b). 1 Supplementary Figure

More information

CNPEM Laboratório de Ciência de Superfícies

CNPEM Laboratório de Ciência de Superfícies Investigating electrical charged samples by scanning probe microscopy: the influence to magnetic force microscopy and atomic force microscopy phase images. Carlos A. R. Costa, 1 Evandro M. Lanzoni, 1 Maria

More information

Magnetic Nanowires inside. carbon nanotubes

Magnetic Nanowires inside. carbon nanotubes Leibniz Institute for Solid State and Materials Research IFW Dresden Magnetic Nanowires inside Carbon Nanotubes Magnetic force microscopy sensors using ironfilled carbon nanotubes Thomas Mühl Outline Introduction

More information

Magnetic Force Microscopy (MFM) F = µ o (m )H

Magnetic Force Microscopy (MFM) F = µ o (m )H Magnetic Force Microscopy (MFM) F = µ o (m )H 1. MFM is based on the use of a ferromagnetic tip as a local field sensor. Magnetic interaction between the tip and the surface results in a force acting on

More information

Supporting Information

Supporting Information Supporting Information Analysis Method for Quantifying the Morphology of Nanotube Networks Dusan Vobornik*, Shan Zou and Gregory P. Lopinski Measurement Science and Standards, National Research Council

More information

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

High-resolution Characterization of Organic Ultrathin Films Using Atomic Force Microscopy High-resolution Characterization of Organic Ultrathin Films Using Atomic Force Microscopy Jing-jiang Yu Nanotechnology Measurements Division Agilent Technologies, Inc. Atomic Force Microscopy High-Resolution

More information

Contents. What is AFM? History Basic principles and devices Operating modes Application areas Advantages and disadvantages

Contents. What is AFM? History Basic principles and devices Operating modes Application areas Advantages and disadvantages Contents What is AFM? History Basic principles and devices Operating modes Application areas Advantages and disadvantages Figure1: 2004 Seth Copen Goldstein What is AFM? A type of Scanning Probe Microscopy

More information

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

Metallurgical and Materials Engineering Department MME 2509 Materials Processing Laboratory SOL-GEL DIP COATING Metallurgical and Materials Engineering Department MME 2509 Materials Processing Laboratory SOL-GEL DIP COATING Assist. Prof. Dr. Tolga TAVŞANOĞLU 1. Sol-gel Process Sol-gel process is used for production

More information

AFM for Measuring Surface Topography and Forces

AFM for Measuring Surface Topography and Forces ENB 2007 07.03.2007 AFM for Measuring Surface Topography and Forces Andreas Fery Scanning Probe : What is it and why do we need it? AFM as a versatile tool for local analysis and manipulation Dates Course

More information

Rationale: Phase diagrams are standard in all high school chemistry textbooks and therefore are considered prior knowledge.

Rationale: Phase diagrams are standard in all high school chemistry textbooks and therefore are considered prior knowledge. Big Idea 2: Chemical and physical properties of materials can be explained by the structure and the arrangement of atoms, ions, or molecules and the forces between them. Material Covered (Y or N) and Location

More information

Chapter 11. Intermolecular Forces and Liquids & Solids

Chapter 11. Intermolecular Forces and Liquids & Solids Chapter 11 Intermolecular Forces and Liquids & Solids The Kinetic Molecular Theory of Liquids & Solids Gases vs. Liquids & Solids difference is distance between molecules Liquids Molecules close together;

More information

Integrating MEMS Electro-Static Driven Micro-Probe and Laser Doppler Vibrometer for Non-Contact Vibration Mode SPM System Design

Integrating MEMS Electro-Static Driven Micro-Probe and Laser Doppler Vibrometer for Non-Contact Vibration Mode SPM System Design Tamkang Journal of Science and Engineering, Vol. 12, No. 4, pp. 399 407 (2009) 399 Integrating MEMS Electro-Static Driven Micro-Probe and Laser Doppler Vibrometer for Non-Contact Vibration Mode SPM System

More information

Thin film techniques: the layer-by-layer self assembly technique

Thin film techniques: the layer-by-layer self assembly technique Thin film techniques: the layer-by-layer self assembly technique Carmelina Ruggiero University of Genoa Overview Thin films Thin film techniques Langmuir-Blodgett technique Chemical self-assembling Layer-by-Layer

More information

ERT320 BIOSEPARATION ENGINEERING CHROMATOGRAPHY

ERT320 BIOSEPARATION ENGINEERING CHROMATOGRAPHY ERT320 BIOSEPARATION ENGINEERING CHROMATOGRAPHY CHROMATOGRAPHY Week 9-10 Reading Assignment: Chapter 7. Bioseparations Science & Engineering, Harrison, R; Todd, P; Rudge, S.C and Petrides, D,P CHROMATOGRAPHY

More information

Surface Transfer Doping of Diamond by Organic Molecules

Surface Transfer Doping of Diamond by Organic Molecules Surface Transfer Doping of Diamond by Organic Molecules Qi Dongchen Department of Physics National University of Singapore Supervisor: Prof. Andrew T. S. Wee Dr. Gao Xingyu Scope of presentation Overview

More information

Module17: Intermolecular Force between Surfaces and Particles. Lecture 23: Intermolecular Force between Surfaces and Particles

Module17: Intermolecular Force between Surfaces and Particles. Lecture 23: Intermolecular Force between Surfaces and Particles Module17: Intermolecular Force between Surfaces and Particles Lecture 23: Intermolecular Force between Surfaces and Particles 1 We now try to understand the nature of spontaneous instability in a confined

More information

Measurements of interaction forces in (biological) model systems

Measurements of interaction forces in (biological) model systems Measurements of interaction forces in (biological) model systems Marina Ruths Department of Chemistry, UMass Lowell What can force measurements tell us about a system? Depending on the technique, we might

More information

LAYER BY LAYER (LbL) SELF-ASSEMBLY STRATEGY AND ITS APPLICATIONS

LAYER BY LAYER (LbL) SELF-ASSEMBLY STRATEGY AND ITS APPLICATIONS LAYER BY LAYER (LbL) SELF-ASSEMBLY STRATEGY AND ITS APPLICATIONS A. Z. Cheng 1, R. Swaminathan 2 1 Nanotechnology Engineering, University of Waterloo, azcheng@uwaterloo.ca; 2 Nanotechnology Engineering,

More information

Graphene The Search For Two Dimensions. Christopher Scott Friedline Arizona State University

Graphene The Search For Two Dimensions. Christopher Scott Friedline Arizona State University Graphene The Search For Two Dimensions Christopher Scott Friedline Arizona State University What Is Graphene? Single atomic layer of graphite arranged in a honeycomb crystal lattice Consists of sp 2 -bonded

More information

Lecture: P1_Wk1_L1 IntraMolecular Interactions. Ron Reifenberger Birck Nanotechnology Center Purdue University 2012

Lecture: P1_Wk1_L1 IntraMolecular Interactions. Ron Reifenberger Birck Nanotechnology Center Purdue University 2012 Lecture: IntraMolecular Interactions Distinguish between IntraMolecular (within a molecule) and InterMolecular (between molecules) Ron Reifenberger Birck Nanotechnology Center Purdue University 2012 1

More information

Chapter 3 Engineering Science for Microsystems Design and Fabrication

Chapter 3 Engineering Science for Microsystems Design and Fabrication Lectures on MEMS and MICROSYSTEMS DESIGN and MANUFACTURE Chapter 3 Engineering Science for Microsystems Design and Fabrication In this Chapter, we will present overviews of the principles of physical and

More information

Institute for Electron Microscopy and Nanoanalysis Graz Centre for Electron Microscopy

Institute for Electron Microscopy and Nanoanalysis Graz Centre for Electron Microscopy Institute for Electron Microscopy and Nanoanalysis Graz Centre for Electron Microscopy Micromechanics Ass.Prof. Priv.-Doz. DI Dr. Harald Plank a,b a Institute of Electron Microscopy and Nanoanalysis, Graz

More information

6. Plasmon coupling between a flat gold interface and gold nanoparticles.

6. Plasmon coupling between a flat gold interface and gold nanoparticles. 6. Plasmon coupling between a flat gold interface and gold nanoparticles. 6.1. Introduction In this outlook oriented chapter the applicability of the multilayered system used in chapter 4.1., for the study

More information

Lecture 4 Scanning Probe Microscopy (SPM)

Lecture 4 Scanning Probe Microscopy (SPM) Lecture 4 Scanning Probe Microscopy (SPM) General components of SPM; Tip --- the probe; Cantilever --- the indicator of the tip; Tip-sample interaction --- the feedback system; Scanner --- piezoelectric

More information

Scanning probe studies of the electrical activity at interfaces formed by silicon wafer direct bonding

Scanning probe studies of the electrical activity at interfaces formed by silicon wafer direct bonding phys. stat. sol. (c) 4, No. 8, 893 897 (007) / DOI 10.100/pssc.00675481 Scanning probe studies of the electrical activity at interfaces formed by silicon wafer direct bonding M. Ratzke *, 1,, O. Vyvenko

More information

Intermolecular Forces and Liquids and Solids

Intermolecular Forces and Liquids and Solids PowerPoint Lecture Presentation by J. David Robertson University of Missouri Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction

More information

Fundamentals of Atomic Force Microscopy Part 2: Dynamic AFM Methods

Fundamentals of Atomic Force Microscopy Part 2: Dynamic AFM Methods Fundamentals of tomic Force Microscopy Part 2: Dynamic FM Methods Week 2, Lecture 5 ttractive and repulsive regimes and phase contrast in amplitude modulation FM rvind Raman Mechanical Engineering Birck

More information

Single-Molecule Recognition and Manipulation Studied by Scanning Probe Microscopy

Single-Molecule Recognition and Manipulation Studied by Scanning Probe Microscopy Single-Molecule Recognition and Manipulation Studied by Scanning Probe Microscopy Byung Kim Department of Physics Boise State University Langmuir (in press, 2006) swollen collapsed Hydrophilic non-sticky

More information

Introduction to Scanning Probe Microscopy Zhe Fei

Introduction to Scanning Probe Microscopy Zhe Fei Introduction to Scanning Probe Microscopy Zhe Fei Phys 590B, Apr. 2019 1 Outline Part 1 SPM Overview Part 2 Scanning tunneling microscopy Part 3 Atomic force microscopy Part 4 Electric & Magnetic force

More information

Kavli Workshop for Journalists. June 13th, CNF Cleanroom Activities

Kavli Workshop for Journalists. June 13th, CNF Cleanroom Activities Kavli Workshop for Journalists June 13th, 2007 CNF Cleanroom Activities Seeing nm-sized Objects with an SEM Lab experience: Scanning Electron Microscopy Equipment: Zeiss Supra 55VP Scanning electron microscopes

More information

The negatively charged insulator-semiconductor structure: Concepts, technological considerations and applications

The negatively charged insulator-semiconductor structure: Concepts, technological considerations and applications The negatively charged insulator-semiconductor structure: Concepts, technological considerations and applications D. König, G. Ebest Department of Electronic Devices, Technical University of Chemnitz,

More information

Using the surface spontaneous depolarization field of ferroelectrics to direct the assembly of virus particles

Using the surface spontaneous depolarization field of ferroelectrics to direct the assembly of virus particles Appl. Phys. Lett. Vol 85, Issue 16, 3537 (2004) Using the surface spontaneous depolarization field of ferroelectrics to direct the assembly of virus particles Working Title: Directed assembly of biological

More information

Intermolecular Forces and Liquids and Solids. Chapter 11. Copyright The McGraw Hill Companies, Inc. Permission required for

Intermolecular Forces and Liquids and Solids. Chapter 11. Copyright The McGraw Hill Companies, Inc. Permission required for Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw Hill Companies, Inc. Permission required for 1 A phase is a homogeneous part of the system in contact with other parts of the

More information

Wafer-scale fabrication of graphene

Wafer-scale fabrication of graphene Wafer-scale fabrication of graphene Sten Vollebregt, MSc Delft University of Technology, Delft Institute of Mircosystems and Nanotechnology Delft University of Technology Challenge the future Delft University

More information

Glassy dynamics in geometrical confinement as studied by Broadband Dielectric Spectroscopy F. Kremer Universität Leipzig

Glassy dynamics in geometrical confinement as studied by Broadband Dielectric Spectroscopy F. Kremer Universität Leipzig Glassy dynamics in geometrical confinement as studied by Broadband Dielectric Spectroscopy F. Kremer Universität Leipzig Co-authors: M. Treß, E.U. Mapesa, W. Kipnusu, C. Iacob (Leipzig), Reiche (Halle),

More information

Intermolecular Forces and Liquids and Solids

Intermolecular Forces and Liquids and Solids Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. A phase is a homogeneous part of the system in contact

More information

Supplementary information for

Supplementary information for Supplementary information for Transverse electric field dragging of DNA in a nanochannel Makusu Tsutsui, Yuhui He, Masayuki Furuhashi, Rahong Sakon, Masateru Taniguchi & Tomoji Kawai The Supplementary

More information

Scanning Force Microscopy

Scanning Force Microscopy Scanning Force Microscopy Roland Bennewitz Rutherford Physics Building 405 Phone 398-3058 roland.bennewitz@mcgill.ca Scanning Probe is moved along scan lines over a sample surface 1 Force Microscopy Data

More information

Magnetic nanoparticles containing soft-hard diblock

Magnetic nanoparticles containing soft-hard diblock Electronic Supplementary Material (ESI) for Nanoscale. This journal is The Royal Society of Chemistry 2018 Electronic Supplementary Information Magnetic nanoparticles containing soft-hard diblock copolymer

More information

Characterization of MEMS Devices

Characterization of MEMS Devices MEMS: Characterization Characterization of MEMS Devices Prasanna S. Gandhi Assistant Professor, Department of Mechanical Engineering, Indian Institute of Technology, Bombay, Recap Characterization of MEMS

More information

Supporting Information for: Electrical probing and tuning of molecular. physisorption on graphene

Supporting Information for: Electrical probing and tuning of molecular. physisorption on graphene Supporting Information for: Electrical probing and tuning of molecular physisorption on graphene Girish S. Kulkarni, Karthik Reddy #, Wenzhe Zang, Kyunghoon Lee, Xudong Fan *, and Zhaohui Zhong * Department

More information

One Q partial negative, the other partial negative Ø H- bonding particularly strong. Abby Carroll 2

One Q partial negative, the other partial negative Ø H- bonding particularly strong. Abby Carroll 2 Chemistry Notes v Polarity Experiment Ø Things involved Polarity Solubility Dispersion Ø Polarity Shaving cream has soap steric acid Water is polar Food coloring is polar/ionic because dissolved Like dissolves

More information

CHAPTER 10. Characteristics of the Surfaces of Biomaterials

CHAPTER 10. Characteristics of the Surfaces of Biomaterials CHAPTER 10 Characteristics of the Surfaces of Biomaterials 10.1 Surface Characteristics Related to Chemical Bonding 10.2 Surface Chemistry Related to Bonding of Biological Molecules 10.3 Porosity 10.4

More information

Temporary Wafer Bonding - Key Technology for 3D-MEMS Integration

Temporary Wafer Bonding - Key Technology for 3D-MEMS Integration Temporary Wafer Bonding - Key Technology for 3D-MEMS Integration 2016-06-15, Chemnitz Chemnitz University of Technology Basic Research Fraunhofer ENAS System-Packaging (SP) Back-End of Line (BEOL) Applied

More information

Single ion implantation for nanoelectronics and the application to biological systems. Iwao Ohdomari Waseda University Tokyo, Japan

Single ion implantation for nanoelectronics and the application to biological systems. Iwao Ohdomari Waseda University Tokyo, Japan Single ion implantation for nanoelectronics and the application to biological systems Iwao Ohdomari Waseda University Tokyo, Japan Contents 1.History of single ion implantation (SII) 2.Novel applications

More information

Electrical Characterization with SPM Application Modules

Electrical Characterization with SPM Application Modules Electrical Characterization with SPM Application Modules Metrology, Characterization, Failure Analysis: Data Storage Magnetoresistive (MR) read-write heads Semiconductor Transistors Interconnect Ferroelectric

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION 1. Supplementary Methods Characterization of AFM resolution We employed amplitude-modulation AFM in non-contact mode to characterize the topography of the graphene samples. The measurements were performed

More information

Techniken der Oberflächenphysik (Techniques of Surface Physics)

Techniken der Oberflächenphysik (Techniques of Surface Physics) Techniken der Oberflächenphysik (Techniques of Surface Physics) Prof. Yong Lei & Dr. Yang Xu (& Liying Liang) Fachgebiet 3D-Nanostrukturierung, Institut für Physik Contact: yong.lei@tu-ilmenau.de; yang.xu@tu-ilmenau.de;

More information

Techniken der Oberflächenphysik (Techniques of Surface Physics)

Techniken der Oberflächenphysik (Techniques of Surface Physics) Techniken der Oberflächenphysik (Techniques of Surface Physics) Prof. Yong Lei & Dr. Yang Xu Fachgebiet 3D-Nanostrukturierung, Institut für Physik Contact: yong.lei@tu-ilmenau.de yang.xu@tu-ilmenau.de

More information

Optimal Design and Evaluation of Cantilever Probe for Multifrequency Atomic Force Microscopy

Optimal Design and Evaluation of Cantilever Probe for Multifrequency Atomic Force Microscopy 11 th World Congress on Structural and Multidisciplinary Optimisation 07 th -12 th, June 2015, Sydney Australia Optimal Design and Evaluation of Cantilever Probe for Multifrequency Atomic Force Microscopy

More information

Transport gap of organic semiconductors in organic modified Schottky contacts

Transport gap of organic semiconductors in organic modified Schottky contacts Applied Surface Science 212 213 (2003) 423 427 Transport gap of organic semiconductors in organic modified Schottky contacts Dietrich R.T. Zahn *, Thorsten U. Kampen, Henry Méndez Institut für Physik,

More information

Proteins polymer molecules, folded in complex structures. Konstantin Popov Department of Biochemistry and Biophysics

Proteins polymer molecules, folded in complex structures. Konstantin Popov Department of Biochemistry and Biophysics Proteins polymer molecules, folded in complex structures Konstantin Popov Department of Biochemistry and Biophysics Outline General aspects of polymer theory Size and persistent length of ideal linear

More information

Concept Summary. Adapted from Batesville High School Physics

Concept Summary. Adapted from Batesville High School Physics Grounding Providing a path from a charged object to the Earth is called grounding it. Charges will be attracted from (or repelled to) the Earth by the charged object. Since the Earth is so large, both

More information

2.76/2.760 Multiscale Systems Design & Manufacturing

2.76/2.760 Multiscale Systems Design & Manufacturing 2.76/2.760 Multiscale Systems Design & Manufacturing Fall 2004 MOEMS Devices for Optical communications system Switches and micromirror for Add/drops Diagrams removed for copyright reasons. MOEMS MEMS

More information

Development of a nanostructural microwave probe based on GaAs

Development of a nanostructural microwave probe based on GaAs Microsyst Technol (2008) 14:1021 1025 DOI 10.1007/s00542-007-0484-0 TECHNICAL PAPER Development of a nanostructural microwave probe based on GaAs Y. Ju Æ T. Kobayashi Æ H. Soyama Received: 18 June 2007

More information

Nanotechnology Nanofabrication of Functional Materials. Marin Alexe Max Planck Institute of Microstructure Physics, Halle - Germany

Nanotechnology Nanofabrication of Functional Materials. Marin Alexe Max Planck Institute of Microstructure Physics, Halle - Germany Nanotechnology Nanofabrication of Functional Materials Marin Alexe Max Planck Institute of Microstructure Physics, Halle - Germany Contents Part I History and background to nanotechnology Nanoworld Nanoelectronics

More information

Program Operacyjny Kapitał Ludzki SCANNING PROBE TECHNIQUES - INTRODUCTION

Program Operacyjny Kapitał Ludzki SCANNING PROBE TECHNIQUES - INTRODUCTION Program Operacyjny Kapitał Ludzki SCANNING PROBE TECHNIQUES - INTRODUCTION Peter Liljeroth Department of Applied Physics, Aalto University School of Science peter.liljeroth@aalto.fi Projekt współfinansowany

More information

CHAPTER 10. Characteristics of the Surfaces of Biomaterials

CHAPTER 10. Characteristics of the Surfaces of Biomaterials CHAPTER 10 Characteristics of the Surfaces of Biomaterials 10.1 Surface Characteristics Related to Chemical Bonding 10.2 Surface Chemistry Related to Bonding of Biological Molecules 10.3 Porosity 10.4

More information

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

The Science and Engineering of Materials, 4 th ed Donald R. Askeland Pradeep P. Phulé. Chapter 2 Atomic Structure The Science and Engineering of Materials, 4 th ed Donald R. Askeland Pradeep P. Phulé Chapter 2 Atomic Structure Objectives of Chapter 2 The goal of this chapter is to describe the underlying physical

More information

ECE280: Nano-Plasmonics and Its Applications. Week8

ECE280: Nano-Plasmonics and Its Applications. Week8 ECE280: Nano-Plasmonics and Its Applications Week8 Surface Enhanced Raman Scattering (SERS) and Surface Plasmon Amplification by Stimulated Emission of Radiation (SPASER) Raman Scattering Chandrasekhara

More information

Noncontact-AFM (nc-afm)

Noncontact-AFM (nc-afm) Noncontact-AFM (nc-afm) Quantitative understanding of nc-afm A attractive interaction Δf Resonance frequency: f 0 Width of resonance curve (FWHM): Γ Γ+ΔΓ Γ Q-factor: Q π f Γ = 0 f 0 f Conservative forces

More information

Introduction to Photolithography

Introduction to Photolithography http://www.ichaus.de/news/72 Introduction to Photolithography Photolithography The following slides present an outline of the process by which integrated circuits are made, of which photolithography is

More information

Section 12: Intro to Devices

Section 12: Intro to Devices Section 12: Intro to Devices Extensive reading materials on reserve, including Robert F. Pierret, Semiconductor Device Fundamentals Bond Model of Electrons and Holes Si Si Si Si Si Si Si Si Si Silicon

More information

PLASMA-POLYMER MODIFICATION OF BASAL PLANE GRAPHITE SURFACES FOR IMPROVED BIOCOMPATIBILITY

PLASMA-POLYMER MODIFICATION OF BASAL PLANE GRAPHITE SURFACES FOR IMPROVED BIOCOMPATIBILITY PLASMA-POLYMER MODIFICATION OF BASAL PLANE GRAPHITE SURFACES FOR IMPROVED BIOCOMPATIBILITY Anca Orăşanu, Marcus R. Davidson, Robert H. Bradley Advanced Materials & Biomaterials Research Centre, School

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 10/02/2007 MS Junctions, Lecture 2 MOS Cap, Lecture 1 Reading: finish chapter14, start chapter16 Announcements Professor Javey will hold his OH at

More information

Electron Beam Curable Varnishes. Rapid Processing of Planarization Layers on Polymer Webs

Electron Beam Curable Varnishes. Rapid Processing of Planarization Layers on Polymer Webs Electron Beam Curable Varnishes Rapid Processing of Planarization Layers on Polymer Webs Juliane Fichtner, Michaela Hagenkamp, Markus Noss, Steffen Günther Fraunhofer Institute for Organic Electronics,

More information

DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD

DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD Chapter 4 DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD 4.1 INTRODUCTION Sputter deposition process is another old technique being used in modern semiconductor industries. Sputtering

More information

Specific ion effects on the interaction of. hydrophobic and hydrophilic self assembled

Specific ion effects on the interaction of. hydrophobic and hydrophilic self assembled Supporting Information Specific ion effects on the interaction of hydrophobic and hydrophilic self assembled monolayers T. Rios-Carvajal*, N. R. Pedersen, N. Bovet, S.L.S. Stipp, T. Hassenkam. Nano-Science

More information

Diamond in Nanoscale Biosensing

Diamond in Nanoscale Biosensing Czech Nano-Team Workshop 2006 Diamond in Nanoscale Biosensing Bohuslav Rezek Institute of Physics AS CR Acknowledgements Dr. Christoph Nebel Dr. Dongchan Shin Dr. Hideyuki Watanabe Diamond Research Center

More information

2. (10%) Correct answers are given below. Every correct answer gives a student 1⅔=1.666 point. There are no negative points for incorrect answers

2. (10%) Correct answers are given below. Every correct answer gives a student 1⅔=1.666 point. There are no negative points for incorrect answers 1. (9%) There are 9 correct answers: (0,0), (1,-1), (1,0), (1,1), (2,-2), (2,-1), (2,0), (2,1), and (2,2). Each correct answer gives a student +1 point. All other answers are incorrect. Every incorrect

More information

Nanometer scale lithography of silicon(100) surfaces using tapping mode atomic force microscopy

Nanometer scale lithography of silicon(100) surfaces using tapping mode atomic force microscopy Nanometer scale lithography of silicon(100) surfaces using tapping mode atomic force microscopy J. Servat, a) P. Gorostiza, and F. Sanz Department Química-Fisica, Universitat de Barcelona, 08028 Barcelona,

More information

9/2/10 TYPES OF INTERMOLECULAR INTERACTIONS

9/2/10 TYPES OF INTERMOLECULAR INTERACTIONS Tro Chpt. 11 Liquids, solids and intermolecular forces Solids, liquids and gases - A Molecular Comparison Intermolecular forces Intermolecular forces in action: surface tension, viscosity and capillary

More information

Supplementary Figure 1: Micromechanical cleavage of graphene on oxygen plasma treated Si/SiO2. Supplementary Figure 2: Comparison of hbn yield.

Supplementary Figure 1: Micromechanical cleavage of graphene on oxygen plasma treated Si/SiO2. Supplementary Figure 2: Comparison of hbn yield. 1 2 3 4 Supplementary Figure 1: Micromechanical cleavage of graphene on oxygen plasma treated Si/SiO 2. Optical microscopy images of three examples of large single layer graphene flakes cleaved on a single

More information