A-444. Adaptive PolCarr carriers for novel applications in life sciences. Heidemarie Schmidt
|
|
- Arlene McKenzie
- 6 years ago
- Views:
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) M108 Stand: 20.10.2015 Aim: Presentation of an application of the AFM for studying surface morphology. Inhalt 1.Introduction...
More informationDeposition 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 informationLecture 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 informationAtomic 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 informationScanning 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 informationGeneral 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 informationScanning 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 informationINTRODUCTION 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 informationContents. 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 informationAFM 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 informationIntermittent-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 informationScanning 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 informationImaging 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 informationModule 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 informationCHAPTER 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 informationIntermolecular 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 informationMEEN 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 informationInstrumentation 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 informationL8: 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 informationReview 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 informationECE 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 informationAbstract. 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 informationGreg Andreev and Aravind Vijayaraghavan 9/27/13
Mapping Graphene s surface potential with
More informationEcole 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 informationAtomic 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 informationNanotechnology 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 informationElectrochemically 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 informationSupplementary 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 informationCNPEM 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 informationMagnetic 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 informationMagnetic 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 informationSupporting 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 informationHigh-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 informationContents. 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 informationMetallurgical 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 informationAFM 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 informationRationale: 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 informationChapter 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 informationIntegrating 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 informationThin 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 informationERT320 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 informationSurface 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 informationModule17: 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 informationMeasurements 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 informationLAYER 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 informationGraphene 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 informationLecture: 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 informationChapter 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 informationInstitute 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 information6. 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 informationLecture 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 informationScanning 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 informationIntermolecular 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 informationFundamentals 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 informationSingle-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 informationIntroduction 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 informationKavli 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 informationThe 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 informationUsing 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 informationIntermolecular 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 informationWafer-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 informationGlassy 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 informationIntermolecular 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 informationSupplementary 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 informationScanning 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 informationMagnetic 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 informationCharacterization 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 informationSupporting 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 informationOne 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 informationCHAPTER 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 informationTemporary 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 informationSingle 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 informationElectrical 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 informationSUPPLEMENTARY 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 informationTechniken 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 informationTechniken 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 informationOptimal 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 informationTransport 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 informationProteins 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 informationConcept 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 information2.76/2.760 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 informationDevelopment 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 informationNanotechnology 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 informationProgram 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 informationCHAPTER 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 informationThe 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 informationECE280: 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 informationNoncontact-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 informationIntroduction 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 informationSection 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 informationPLASMA-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 informationEECS130 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 informationElectron 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 informationDEPOSITION 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 informationSpecific 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 informationDiamond 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 information2. (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 informationNanometer 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 information9/2/10 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 informationSupplementary 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