Scanning Probe Microscopy

Size: px
Start display at page:

Download "Scanning Probe Microscopy"

Transcription

1 Bert Voigtlander Scanning Probe Microscopy Atomic Force Microscopy and Scanning Tunneling Microscopy ^ Springer

2 Contents 1 Introduction Introduction to Scanning Tunneling Microscopy Introduction to Atomic Force Microscopy A Short History of Scanning Probe Microscopy Summary 11 Part I Scanning Probe Microscopy Instrumentation 2 Harmonic Oscillator Free Harmonic Oscillator Driven Harmonic Oscillator Driven Harmonic Oscillator with Damping Transients of Oscillations Dissipation and Quality Factor of a Damped Driven Harmonic Oscillator Effective Mass of a Harmonic Oscillator Linear Differential Equations Summary 29 3 Technical Aspects of Scanning Probe Microscopy Piezoelectric Effect Extensions of Piezoelectric Actuators Piezoelectric Materials Tube Piezo Element Resonance Frequencies of Piezo Tubes Flexure-Guided Piezo Nanopositioning Stages Non-linearities and Hysteresis Effects of Piezoelectric Actuators Hysteresis Creep 49 ix

3 x Contents Thermal Drift STM Tip Preparation Vibration Isolation Isolation of the Microscope from Outer Vibrations The Microscope Considered as a Vibrating System Combining Vibration Isolation and a Microscope with High Resonance Frequency Building Vibrations Summary 63 4 Scanning Probe Microscopy Designs Nanoscope Inertial Sliders Beetle STM Pan Slider KoalaDrive Tip Exchange Summary 75 5 Electronics for Scanning Probe Microscopy Voltage Divider Impedance, Transfer Function, and Bode Plot Output Resistance/Input Resistance Noise Operational Amplifiers Voltage Follower/Impedance Converter Voltage Amplifier Current Amplifier Feedback Controller Proportional Controller Proportional-Integral Controller Feedback Controller in STM Implementation of an STM Feedback Controller Digital-to-Analog Converter Analog-to-Digital Converter High-Voltage Amplifier Summary 99

4 Contents xi 6 Lock-In Technique Lock-In Amplifier Principle of Operation Summary Data Representation and Image Processing Data Representation Image Processing Data Analysis Summary Artifacts in SPM Tip-Related Artifacts Other Artifacts Summary Work Function, Contact Potential, and Kelvin Probe Scanning Force Microscopy Work Function Effect of a Surface on the Work Function Surface Charges and External Electric Fields Contact Potential Measurement of Work Function by the Kelvin Method Kelvin Probe Scanning Force Microscopy (KFM) Summary Surface States Surface States in a One-Dimensional Crystal Surface States in 3D Crystals Surface States Within the Tight Binding Model Summary 141 Part II Atomic Force Microscopy (AFM) 11 Forces Between Tip and Sample Tip-Sample Forces Snap-to-Contact Summary Technical Aspects of Atomic Force Microscopy (AFM) Requirements for Force Sensors Fabrication of Cantilevers Beam Deflection Atomic Force Microscopy 161

5 Xll Contents Sensitivity of the Beam Deflection Method Detection Limit of the Beam Deflection Method Other Detection Methods Calibration of AFM Measurements Experimental Determination of the Sensitivity Factor in AFM Calculation of the Spring Constant from the Geometrical Data of the Cantilever Sader Method for the Determination of the Spring Constant of a Cantilever Thermal Method for the Determination of the Spring Constant of a Cantilever Experimental Determination of the Sensitivity and Spring Constant in AFM Without Tip-Sample Contact Summary Static Atomic Force Microscopy Principles of Static Atomic Force Microscopy Properties of Static AFM Imaging Constant Height Mode in Static AFM Friction Force Microscopy (FFM) Force-Distance Curves Summary Amplitude Modulation (AM) Mode in Dynamic Atomic Force Microscopy Parameters of Dynamic Atomic Force Microscopy Principles of Dynamic Atomic Force Microscopy I (Amplitude Modulation) Amplitude Modulation (AM) Detection Scheme in Dynamic Atomic Force Microscopy Experimental Realization of the AM Detection Mode Time Constant in AM Detection Dissipative Interactions in Non-contact AFM in the Small Amplitude Limit Dependence of the Phase on the Damping and on the Force Gradient Summary 204

6 . Contents xiii 15 Intermittent Contact Mode/Tapping Mode Atomic Force Microscopy with Large Oscillation Amplitudes Resonance Curve for an Anharmonic Force-Distance Dependence Amplitude Instabilities for an Anharmonic Oscillator Energy Dissipation in Dynamic Atomic Force Microscopy Properties of the Intermittent Contact Mode/Tapping Mode Summary Mapping of Mechanical Properties Using Force-Distance Curves Principles of Force-Distance Curve Mapping Mapping of the Mechanical Properties of the Sample Summary Frequency Modulation (FM) Mode in Dynamic Atomic Force Microscopy Non-contact Atomic Force Microscopy Principles of Dynamic Atomic Force Microscopy II Expression for the Frequency Shift Normalized Frequency Shift in the Large Amplitude Limit Recovery of the Tip-Sample Force Experimental Realization of the FM Detection Scheme Self-excitation Mode Frequency Detection with a Phase-Locked Loop (PLL) PLL Tracking Mode The Non-monotonous Frequency Shift in AFM Comparison of Different AFM Modes Summary Noise in Atomic Force Microscopy Thermal Noise Density of a Harmonic Oscillator Thermal Noise in the Static AFM Mode Thermal Noise in the Dynamic AFM Mode with AM Detection Thermal Noise in Dynamic AFM with FM Detection Sensor Displacement Noise in the FM Detection Mode Total Noise in the FM Detection Mode Comparison to Noise in STM Signal-to-Noise Ratio in Atomic Force Microscopy FM Detection Summary 267

7 xiv Contents 19 Quartz Sensors in Atomic Force Microscopy Tuning Fork Quartz Sensor Quartz Needle Sensor Determination of the Sensitivity of Quartz Sensors Summary 275 Part HI Scanning Tunneling Microscopy and Spectroscopy 20 Scanning Tunneling Microscopy One-Dimensional Potential Barrier Model Flux of Matter and Charge in Quantum Mechanics The WKB Approximation for Tunneling Density of States Bardeen Model for Tunneling Energy-Dependent Approximation of the Bardeen Model Tersoff-Hamann Approximation of the Bardeen Model Constant Current Mode and Constant Height Mode Voltage-Dependent Imaging Summary Scanning Tunneling Spectroscopy (STS) Scanning Tunneling Spectroscopy Overview Experimental Realization of Spectroscopy with STM Normalized Differential Conductance Relation Between Differential Conductance and the Density of States Recovery of the Density of States Asymmetry in the Tunneling Spectra Beyond the ID Barrier Approximation Energy Resolution in Scanning Tunneling Spectroscopy Barrier Height Spectroscopy Barrier Resonances Spectroscopic Imaging Example: Spectroscopy of the Si(7 x 7) Surface Summary 333

8 Contents xv 22 Vibrational Spectroscopy with the STM Principles of Inelastic Tunneling Spectroscopy with the STM Examples of Vibrational Spectra Obtained with the STM Summary Spectroscopy and Imaging of Surface States Energy Dependence of the Density of States in Two, One and Zero Dimensions Scattering of Surface State Electrons at Surface Defects Summary Building Nanostructures Atom by Atom Positioning of Single Atoms and Molecules by STM Electron Confinement in Nanoscale Cages Inducing a Single Molecule Chemical Reaction with the STM Tip Summary 357 Appendix A: Horizontal Piezo Constant for a Tube Piezo Element Appendix B: Fermi's Golden Rule and Bardeen's Matrix Elements Appendix C: Frequency Noise in FM Detection 371 References 375 Index 377

Scanning Probe Microscopy

Scanning Probe Microscopy Ernst Meyer Hans Josef Hug Roland Bennewitz Scanning Probe Microscopy The Lab on a Tip With 117 Figures Mß Springer Contents 1 Introduction to Scanning Probe Microscopy f f.1 Overview 2 f.2 Basic Concepts

More information

INTRODUCTION TO SCANNING TUNNELING MICROSCOPY

INTRODUCTION TO SCANNING TUNNELING MICROSCOPY INTRODUCTION TO SCANNING TUNNELING MICROSCOPY SECOND EDITION C. JULIAN CHEN Department of Applied Physics and Applied Mathematics, Columbia University, New York OXJORD UNIVERSITY PRESS Contents Preface

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

STM and AFM Tutorial. Katie Mitchell January 20, 2010

STM and AFM Tutorial. Katie Mitchell January 20, 2010 STM and AFM Tutorial Katie Mitchell January 20, 2010 Overview Scanning Probe Microscopes Scanning Tunneling Microscopy (STM) Atomic Force Microscopy (AFM) Contact AFM Non-contact AFM RHK UHV350 AFM/STM

More information

1 Introduction. 1.1 Historical Perspective

1 Introduction. 1.1 Historical Perspective j1 1 Introduction 1.1 Historical Perspective The invention of scanning probe microscopy is considered one of the major advances in materials science since 1950 [1, 2]. Scanning probe microscopy includes

More information

Lecture 6 Scanning Tunneling Microscopy (STM) General components of STM; Tunneling current; Feedback system; Tip --- the probe.

Lecture 6 Scanning Tunneling Microscopy (STM) General components of STM; Tunneling current; Feedback system; Tip --- the probe. Lecture 6 Scanning Tunneling Microscopy (STM) General components of STM; Tunneling current; Feedback system; Tip --- the probe. Brief Overview of STM Inventors of STM The Nobel Prize in Physics 1986 Nobel

More information

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy 5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy Resolution of optical microscope is limited by diffraction. Light going through an aperture makes diffraction

More information

SCANNING PROBE MICROSCOPY NANOS-E3 SCHOOL 29/09/2015 An introduction to surface microscopy probes

SCANNING PROBE MICROSCOPY NANOS-E3 SCHOOL 29/09/2015 An introduction to surface microscopy probes SCANNING PROBE MICROSCOPY NANOS-E3 SCHOOL 29/09/2015 An introduction to surface microscopy probes SPM is ubiquitous in modern research Physics Nanotechnology/chemistry Nature Nanotechnology 10, 156 160

More information

Preface Light Microscopy X-ray Diffraction Methods

Preface Light Microscopy X-ray Diffraction Methods Preface xi 1 Light Microscopy 1 1.1 Optical Principles 1 1.1.1 Image Formation 1 1.1.2 Resolution 3 1.1.3 Depth of Field 5 1.1.4 Aberrations 6 1.2 Instrumentation 8 1.2.1 Illumination System 9 1.2.2 Objective

More information

Piezoelectric Scanners

Piezoelectric Scanners Piezoelectric Scanners Piezoelectric materials are ceramics that change dimensions in response to an applied voltage and conversely, they develop an electrical potential in response to mechanical pressure.

More information

Nano-Spectroscopy. Solutions AFM-Raman, TERS, NSOM Chemical imaging at the nanoscale

Nano-Spectroscopy. Solutions AFM-Raman, TERS, NSOM Chemical imaging at the nanoscale Nano-Spectroscopy Solutions AFM-Raman, TERS, NSOM Chemical imaging at the nanoscale Since its introduction in the early 80 s, Scanning Probe Microscopy (SPM) has quickly made nanoscale imaging an affordable

More information

A METHOD OF PRECISE CALIBRATION FOR PIEZOELECTRICAL ACTUATORS

A METHOD OF PRECISE CALIBRATION FOR PIEZOELECTRICAL ACTUATORS Uludağ Üniversitesi Mühendislik-Mimarlık Fakültesi Dergisi, Cilt 9, Sayı, 24 A METHOD OF PRECISE CALIBRATION FOR PIEZOELECTRICAL ACTUATORS Timur CANEL * Yüksel BEKTÖRE ** Abstract: Piezoelectrical actuators

More information

- particle with kinetic energy E strikes a barrier with height U 0 > E and width L. - classically the particle cannot overcome the barrier

- particle with kinetic energy E strikes a barrier with height U 0 > E and width L. - classically the particle cannot overcome the barrier Tunnel Effect: - particle with kinetic energy E strikes a barrier with height U 0 > E and width L - classically the particle cannot overcome the barrier - quantum mechanically the particle can penetrated

More information

Compact mobilized and low-cost scanning tunneling microscope for educational use

Compact mobilized and low-cost scanning tunneling microscope for educational use A. Compact mobilized and low-cost scanning tunneling microscope for educational use Eli Flaxer AFEKA - Tel-Aviv Academic College of Engineering, 69107 Tel-Aviv, Israel. We developed a mobile, compact and

More information

Force Spectroscopy with the Atomic Force Microscope

Force Spectroscopy with the Atomic Force Microscope Force Spectroscopy with the Atomic Force Microscope Application Note Wenhai Han, Agilent Technologies F. Michael Serry Figure 1. In Force spectroscopy raster-scanning is disabled temporarily or indefinitely

More information

22.302 Experiment 5. Strain Gage Measurements

22.302 Experiment 5. Strain Gage Measurements 22.302 Experiment 5 Strain Gage Measurements Introduction The design of components for many engineering systems is based on the application of theoretical models. The accuracy of these models can be verified

More information

Tecniche a scansione di sonda per nanoscopia e nanomanipolazione: STM, AFM e derivati

Tecniche a scansione di sonda per nanoscopia e nanomanipolazione: STM, AFM e derivati LS Scienza dei Materiali - a.a. 2006/07 Fisica delle Nanotecnologie part 5.1 Version 5a, Nov 2006 Francesco Fuso, tel 0502214305, 0502214293 - fuso@df.unipi.it http://www.df.unipi.it/~fuso/dida Tecniche

More information

Fast-scanning near-field scanning optical microscopy. using a high-frequency dithering probe

Fast-scanning near-field scanning optical microscopy. using a high-frequency dithering probe Fast-scanning near-field scanning optical microscopy using a high-frequency dithering probe Yongho Seo and Wonho Jhe * Center for Near-field Atom-photon Technology and School of Physics, Seoul National

More information

Scanning Near-Field Optical Microscopy for Measuring Materials Properties at the Nanoscale

Scanning Near-Field Optical Microscopy for Measuring Materials Properties at the Nanoscale Scanning Near-Field Optical Microscopy for Measuring Materials Properties at the Nanoscale Outline Background Research Design Detection of Near-Field Signal Submonolayer Chemical Sensitivity Conclusions

More information

Surface Analysis with STM and AFM

Surface Analysis with STM and AFM Sergei N. Magonov, Myung-Hwan Whangbo Surface Analysis with STM and AFM Experimental and Theoretical Aspects of Image Analysis VCH Weinheim New York Basel Cambridge Tokyo Preface V 1 Introduction 1 1.1

More information

Surface Profilometry as a tool to Measure Thin Film Stress, A Practical Approach. Gianni Franceschinis, RIT MicroE Graduate Student

Surface Profilometry as a tool to Measure Thin Film Stress, A Practical Approach. Gianni Franceschinis, RIT MicroE Graduate Student 1 Surface Profilometry as a tool to Measure Thin Film Stress, A Practical Approach. Gianni Franceschinis, RIT MicroE Graduate Student Abstract-- As the film decreases in thickness the requirements of more

More information

Tecniche a scansione di sonda per nanoscopia e nanomanipolazione 2: AFM e derivati

Tecniche a scansione di sonda per nanoscopia e nanomanipolazione 2: AFM e derivati LS Scienza dei Materiali - a.a. 2008/09 Fisica delle Nanotecnologie part 5.2 Version 7, Nov 2008 Francesco Fuso, tel 0502214305, 0502214293 - fuso@df.unipi.it http://www.df.unipi.it/~fuso/dida Tecniche

More information

7/3/2014. Introduction to Atomic Force Microscope. Introduction to Scanning Force Microscope. Invention of Atomic Force Microscope (AFM)

7/3/2014. Introduction to Atomic Force Microscope. Introduction to Scanning Force Microscope. Invention of Atomic Force Microscope (AFM) Introduction to Atomic Force Microscope Introduction to Scanning Force Microscope Not that kind of atomic Tien Ming Chuang ( 莊 天 明 ) Institute of Physics, Academia Sinica Tien Ming Chuang ( 莊 天 明 ) Institute

More information

Multi-mode Atomic Force Microscope (with High Voltage Piezo Force Microscope and +/- 8000 Oe Variable Field module.)

Multi-mode Atomic Force Microscope (with High Voltage Piezo Force Microscope and +/- 8000 Oe Variable Field module.) Multi-mode Atomic Force Microscope (with High Voltage Piezo Force Microscope and +/- 8000 Oe Variable Field module.) Main specifications of the proposed instrument: 1 Instrument Resolution: 1.1 The instrument

More information

SPM 150 Aarhus with KolibriSensor

SPM 150 Aarhus with KolibriSensor Customied Systems and Solutions Nanostructures and Thin Film Deposition Surface Analysis and Preparation Components Surface Science Applications SPM 150 Aarhus with KolibriSensor Atomic resolution NC-AFM

More information

UNIVERSITY OF SOUTHAMPTON. Scanning Near-Field Optical Microscope Characterisation of Microstructured Optical Fibre Devices.

UNIVERSITY OF SOUTHAMPTON. Scanning Near-Field Optical Microscope Characterisation of Microstructured Optical Fibre Devices. UNIVERSITY OF SOUTHAMPTON Scanning Near-Field Optical Microscope Characterisation of Microstructured Optical Fibre Devices. Christopher Wyndham John Hillman Submitted for the degree of Doctor of Philosophy

More information

Basic principles and mechanisms of NSOM; Different scanning modes and systems of NSOM; General applications and advantages of NSOM.

Basic principles and mechanisms of NSOM; Different scanning modes and systems of NSOM; General applications and advantages of NSOM. Lecture 16: Near-field Scanning Optical Microscopy (NSOM) Background of NSOM; Basic principles and mechanisms of NSOM; Basic components of a NSOM; Different scanning modes and systems of NSOM; General

More information

Contents. Preface. xiii. Part I 1

Contents. Preface. xiii. Part I 1 Contents Preface xiii Part I 1 Chapter 1 Introduction to Frequency-Modulated Continuous-Wave 3 Radar 1.1 Brief History 3 1.2 Examples of Use of FMCW Radar 5 1.2.1 Radio Altimeters 5 1.2.2 Level-Measuring

More information

Calibration of AFM with virtual standards; robust, versatile and accurate. Richard Koops VSL Dutch Metrology Institute Delft

Calibration of AFM with virtual standards; robust, versatile and accurate. Richard Koops VSL Dutch Metrology Institute Delft Calibration of AFM with virtual standards; robust, versatile and accurate Richard Koops VSL Dutch Metrology Institute Delft 19-11-2015 VSL Dutch Metrology Institute VSL is the national metrology institute

More information

It has long been a goal to achieve higher spatial resolution in optical imaging and

It has long been a goal to achieve higher spatial resolution in optical imaging and Nano-optical Imaging using Scattering Scanning Near-field Optical Microscopy Fehmi Yasin, Advisor: Dr. Markus Raschke, Post-doc: Dr. Gregory Andreev, Graduate Student: Benjamin Pollard Department of Physics,

More information

Atomic Force Microscopy. Long Phan Nanotechnology Summer Series May 15, 2013

Atomic Force Microscopy. Long Phan Nanotechnology Summer Series May 15, 2013 Atomic Force Microscopy Long Phan Nanotechnology Summer Series May 15, 2013 1 World s Smallest Movie 2 Outline What is AFM? How does AFM Work? 3 Modes: Contact mode Non contact mode Tapping mode Imaging

More information

CREOL, College of Optics & Photonics, University of Central Florida

CREOL, College of Optics & Photonics, University of Central Florida OSE6650 - Optical Properties of Nanostructured Materials Optical Properties of Nanostructured Materials Fall 2013 Class 3 slide 1 Challenge: excite and detect the near field Thus far: Nanostructured materials

More information

ATOMIC FORCE MICROSCOPY

ATOMIC FORCE MICROSCOPY ATOMIC FORCE MICROSCOPY Introduction The atomic force microscope, or AFM, is a member of the family of instruments known as scanning probe microscopes. The AFM operates under a completely different principle

More information

Usage of Carbon Nanotubes in Scanning Probe Microscopes as Probe. Keywords: Carbon Nanotube, Scanning Probe Microscope

Usage of Carbon Nanotubes in Scanning Probe Microscopes as Probe. Keywords: Carbon Nanotube, Scanning Probe Microscope International Journal of Arts and Sciences 3(1): 18-26 (2009) CD-ROM. ISSN: 1944-6934 InternationalJournal.org Usage of Carbon Nanotubes in Scanning Probe Microscopes as Probe Bedri Onur Kucukyildirim,

More information

Department of Aerospace Engineering Indian Institute of Science Bangalore

Department of Aerospace Engineering Indian Institute of Science Bangalore Department of Aerospace Engineering Indian Institute of Science Bangalore Brief Outline of Department The department of Aerospace Engineering is one of the oldest departments in the country encompassing

More information

The Design and Characteristic Study of a 3-dimensional Piezoelectric Nano-positioner

The Design and Characteristic Study of a 3-dimensional Piezoelectric Nano-positioner SICE Annual Conference August 8-,, The Grand Hotel, Taipei, Taiwan The Design and Characteristic Study of a -dimensional Piezoelectric Nano-positioner Yu-Chi Wang Department of Mechanical Engineering National

More information

Scanning probe microscopy AFM, STM. Near field Scanning Optical Microscopy(NSOM) Scanning probe fabrication

Scanning probe microscopy AFM, STM. Near field Scanning Optical Microscopy(NSOM) Scanning probe fabrication Scanning probe microscopy AFM, STM Near field Scanning Optical Microscopy(NSOM) Scanning probe fabrication Scanning Probe Microscopy 1986 Binning and Rohrer shared Nobel Prize in Physics for invention.stm

More information

Optics and Spectroscopy at Surfaces and Interfaces

Optics and Spectroscopy at Surfaces and Interfaces Vladimir G. Bordo and Horst-Gunter Rubahn Optics and Spectroscopy at Surfaces and Interfaces WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Contents Preface IX 1 Introduction 1 2 Surfaces and Interfaces 5

More information

Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives

Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives Physics 9e/Cutnell correlated to the College Board AP Physics 1 Course Objectives Big Idea 1: Objects and systems have properties such as mass and charge. Systems may have internal structure. Enduring

More information

Agilent 5500 AFM. Data Sheet. Features and Benefits

Agilent 5500 AFM. Data Sheet. Features and Benefits Agilent 5500 AFM Data Sheet Figure 1. STM image of HOPG showing atomic structure. Scan size: 4 nm. Features and Benefits Exceptional environmental and temperature control Superior scanning in fluids, gases,

More information

E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE

E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE References for Nuclear Magnetic Resonance 1. Slichter, Principles of Magnetic Resonance, Harper and Row, 1963. chapter

More information

AFM-kit. Development of a kit for building from scratch an educational (but decently performing - i.e. usable) AFM.

AFM-kit. Development of a kit for building from scratch an educational (but decently performing - i.e. usable) AFM. AFM-kit Development of a kit for building from scratch an educational (but decently performing - i.e. usable) AFM. Building AFM is the best way to understand how it "really" works. initial tasks Define

More information

Nano-Microscopy: Lecture 1. Pavel Zinin HIGP, University of Hawaii, Honolulu, USA

Nano-Microscopy: Lecture 1. Pavel Zinin HIGP, University of Hawaii, Honolulu, USA GG 711: Advanced Techniques in Geophysics and Materials Science Nano-Microscopy: Lecture 1 Scanning Tunneling and Atomic Force Microscopies Principles Pavel Zinin HIGP, University of Hawaii, Honolulu,

More information

Current control of piezoelectric actuators with power loss compensation

Current control of piezoelectric actuators with power loss compensation Tampere University of Technology Author(s) Title Citation onkanen, Pekka; Kallio, Pasi; Koivo, Heikki Current control of piezoelectric actuators with power loss compensation onkanen, Pekka; Kallio, Pasi;

More information

Microscopie à force atomique: Le mode noncontact

Microscopie à force atomique: Le mode noncontact Microscopie à force atomique: Le mode noncontact Clemens Barth barth@crmcn.univ-mrs.fr CRMCN-CNRS, Campus de Lumny, Case 913, 13288 Marseille Cedex09, France La Londe les Maures (France) -- 20-21/03/2007

More information

DYNAMIC ANALYSIS ON STEEL FIBRE

DYNAMIC ANALYSIS ON STEEL FIBRE International Journal of Civil Engineering and Technology (IJCIET) Volume 7, Issue 2, March-April 2016, pp. 179 184, Article ID: IJCIET_07_02_015 Available online at http://www.iaeme.com/ijciet/issues.asp?jtype=ijciet&vtype=7&itype=2

More information

Sensor Performance Metrics

Sensor Performance Metrics Sensor Performance Metrics Michael Todd Professor and Vice Chair Dept. of Structural Engineering University of California, San Diego mdtodd@ucsd.edu Email me if you want a copy. Outline Sensors as dynamic

More information

5. Measurement of a magnetic field

5. Measurement of a magnetic field H 5. Measurement of a magnetic field 5.1 Introduction Magnetic fields play an important role in physics and engineering. In this experiment, three different methods are examined for the measurement of

More information

Non-Contact Vibration Measurement of Micro-Structures

Non-Contact Vibration Measurement of Micro-Structures Non-Contact Vibration Measurement of Micro-Structures Using Laser Doppler Vibrometry (LDV) and Planar Motion Analysis (PMA) to examine and assess the vibration characteristics of micro- and macro-structures.

More information

(Nano)materials characterization

(Nano)materials characterization (Nano)materials characterization MTX9100 Nanomaterials Lecture 8 OUTLINE 1 -What SEM and AFM are good for? - What is the Atomic Force Microscopes Contribution to Nanotechnology? - What is Spectroscopy?

More information

Characterization of surfaces by AFM topographical, mechanical and chemical properties

Characterization of surfaces by AFM topographical, mechanical and chemical properties Characterization of surfaces by AFM topographical, mechanical and chemical properties Jouko Peltonen Department of physical chemistry Åbo Akademi University Atomic Force Microscopy (AFM) Contact mode AFM

More information

Safakcan Tuncdemir 1, William M. Bradley *2. 1. Introduction

Safakcan Tuncdemir 1, William M. Bradley *2. 1. Introduction Modeling and Experimental Verification of the Power Transfer and Thermal Characteristics of Piezoelectric Transformers Subjected to Combined Mechanical and Electrical Loading Safakcan Tuncdemir 1, William

More information

Dynamic Process Modeling. Process Dynamics and Control

Dynamic Process Modeling. Process Dynamics and Control Dynamic Process Modeling Process Dynamics and Control 1 Description of process dynamics Classes of models What do we need for control? Modeling for control Mechanical Systems Modeling Electrical circuits

More information

Unsteady Pressure Measurements

Unsteady Pressure Measurements Quite often the measurements of pressures has to be conducted in unsteady conditions. Typical cases are those of -the measurement of time-varying pressure (with periodic oscillations or step changes) -the

More information

Microscopie à champs proche: et application

Microscopie à champs proche: et application Microscopie à champs proche: Théorie et application STM, effet tunnel et applications AFM, interactions et applications im2np, Giens 2010 Optical microscopy: resolution limit resolution limit: d min =

More information

FXA 2008. UNIT G484 Module 2 4.2.3 Simple Harmonic Oscillations 11. frequency of the applied = natural frequency of the

FXA 2008. UNIT G484 Module 2 4.2.3 Simple Harmonic Oscillations 11. frequency of the applied = natural frequency of the 11 FORCED OSCILLATIONS AND RESONANCE POINTER INSTRUMENTS Analogue ammeter and voltmeters, have CRITICAL DAMPING so as to allow the needle pointer to reach its correct position on the scale after a single

More information

4 SENSORS. Example. A force of 1 N is exerted on a PZT5A disc of diameter 10 mm and thickness 1 mm. The resulting mechanical stress is:

4 SENSORS. Example. A force of 1 N is exerted on a PZT5A disc of diameter 10 mm and thickness 1 mm. The resulting mechanical stress is: 4 SENSORS The modern technical world demands the availability of sensors to measure and convert a variety of physical quantities into electrical signals. These signals can then be fed into data processing

More information

Signal to Noise Instrumental Excel Assignment

Signal to Noise Instrumental Excel Assignment Signal to Noise Instrumental Excel Assignment Instrumental methods, as all techniques involved in physical measurements, are limited by both the precision and accuracy. The precision and accuracy of a

More information

Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications

Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications Saulius Marcinkevičius Optics, ICT, KTH 1 Outline Optical near field. Principle of scanning near field optical microscope

More information

AMS Verification at SoC Level: A practical approach for using VAMS vs SPICE views

AMS Verification at SoC Level: A practical approach for using VAMS vs SPICE views AMS Verification at SoC Level: A practical approach for using VAMS vs SPICE views Nitin Pant, Gautham Harinarayan, Manmohan Rana Accellera Systems Initiative 1 Agenda Need for SoC AMS Verification Mixed

More information

1. Photon Beam Damage and Charging at Solid Surfaces John H. Thomas III

1. Photon Beam Damage and Charging at Solid Surfaces John H. Thomas III 1. Photon Beam Damage and Charging at Solid Surfaces John H. Thomas III 1. Introduction............................. 2. Electrostatic Charging of Samples in Photoemission Experiments............................

More information

How To Image A Magnetic Microscope

How To Image A Magnetic Microscope Agustina Asenjo Dpto. Propiedades Opticas, Magnéticas y de Transporte Instituto de Ciencia de Materiales de Madrid- CSIC Introducción: Esquema MFM frente a otras técnicas de observación de dominios. Fundamentos

More information

Microscopy: Principles and Advances

Microscopy: Principles and Advances Microscopy: Principles and Advances Chandrashekhar V. Kulkarni University of Central Lancashire, Preston, United kingdom May, 2014 University of Ljubljana Academic Background 2005-2008: PhD-Chemical Biology

More information

Atomic Force Microscope and Magnetic Force Microscope Background Information

Atomic Force Microscope and Magnetic Force Microscope Background Information Atomic Force Microscope and Magnetic Force Microscope Background Information Lego Building Instructions There are several places to find the building instructions for building the Lego models of atomic

More information

Calibration and Use of a Strain-Gage-Instrumented Beam: Density Determination and Weight-Flow-Rate Measurement

Calibration and Use of a Strain-Gage-Instrumented Beam: Density Determination and Weight-Flow-Rate Measurement Chapter 2 Calibration and Use of a Strain-Gage-Instrumented Beam: Density Determination and Weight-Flow-Rate Measurement 2.1 Introduction and Objectives This laboratory exercise involves the static calibration

More information

Infrared Spectroscopy: Theory

Infrared Spectroscopy: Theory u Chapter 15 Infrared Spectroscopy: Theory An important tool of the organic chemist is Infrared Spectroscopy, or IR. IR spectra are acquired on a special instrument, called an IR spectrometer. IR is used

More information

Robert G. Hunsperger. Integrated Optics. Theory and Technology. Fourth Edition. With 195 Figures and 17 Tables. Springer

Robert G. Hunsperger. Integrated Optics. Theory and Technology. Fourth Edition. With 195 Figures and 17 Tables. Springer Robert G. Hunsperger Integrated Optics Theory and Technology Fourth Edition With 195 Figures and 17 Tables Springer Contents 1. Introduction 1 1.1 Advantages of Integrated Optics 2 1.1.1 Comparison of

More information

Atomic Force Microscope

Atomic Force Microscope Atomic Force Microscope (Veeco Nanoman) User Manual Basic Operation 4 th Edition Aug 2012 NR System Startup If the system is currently ON To start the NanoScope software, double-click the NanoScope startup

More information

Laminar and Turbulent flow. Flow Sensors. Reynolds Number. Thermal flow Sensor. Flow and Flow rate. R = Mass Flow controllers

Laminar and Turbulent flow. Flow Sensors. Reynolds Number. Thermal flow Sensor. Flow and Flow rate. R = Mass Flow controllers Flow and Flow rate. Laminar and Turbulent flow Laminar flow: smooth, orderly and regular Mechanical sensors have inertia, which can integrate out small variations due to turbulence Turbulent flow: chaotic

More information

PIEZOELECTRIC TRANSDUCERS MODELING AND CHARACTERIZATION

PIEZOELECTRIC TRANSDUCERS MODELING AND CHARACTERIZATION Piezoelectric Transducers Modeling and Characterization (complete technology and know-how inside). 266 pages, August 2004 www.mpi-ultrasonics.com mpi@bluewin.ch Here you can only see the content and several

More information

vii TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENT ABSTRACT ABSTRAK

vii TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENT ABSTRACT ABSTRAK vii TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENT ABSTRACT ABSTRAK TABLE OF CONTENTS LIST OF TABLES LIST OF FIGURES LIST OF SYMBOLS / ABBREVIATIONS LIST OF APPENDICES ii iii

More information

An Electromagnetic Micro Power Generator Based on Mechanical Frequency Up-Conversion

An Electromagnetic Micro Power Generator Based on Mechanical Frequency Up-Conversion International Journal of Materials Science and Engineering Vol. 1, No. December 013 An Electromagnetic Micro Power Generator Based on Mechanical Frequency Up-Conversion Vida Pashaei and Manouchehr Bahrami

More information

Overview of Topics. Stress-Strain Behavior in Concrete. Elastic Behavior. Non-Linear Inelastic Behavior. Stress Distribution.

Overview of Topics. Stress-Strain Behavior in Concrete. Elastic Behavior. Non-Linear Inelastic Behavior. Stress Distribution. Stress-Strain Behavior in Concrete Overview of Topics EARLY AGE CONCRETE Plastic shrinkage shrinkage strain associated with early moisture loss Thermal shrinkage shrinkage strain associated with cooling

More information

Vehicle-Bridge Interaction Dynamics

Vehicle-Bridge Interaction Dynamics Vehicle-Bridge Interaction Dynamics With Applications to High-Speed Railways Y. B. Yang National Taiwan University, Taiwan J. D. Yau Tamkang University, Taiwan Y. S. Wu Sinotech Engineering Consultants,

More information

Sensors & Instruments for station. returned samples. Chun Chia Tan

Sensors & Instruments for station. returned samples. Chun Chia Tan Sensors & Instruments for station based materials characterization of returned samples Chun Chia Tan 04/01/2009 Outline Introduction to materials characterization General overview of the equipment used

More information

ENS 07 Paris, France, 3-4 December 2007

ENS 07 Paris, France, 3-4 December 2007 ENS 7 Paris, France, 3-4 December 7 FRICTION DRIVE SIMULATION OF A SURFACE ACOUSTIC WAVE MOTOR BY NANO VIBRATION Minoru Kuribayashi Kurosawa, Takashi Shigematsu Tokyou Institute of Technology, Yokohama

More information

Traceable cantilever stiffness calibration method using a MEMS nano-force transducer

Traceable cantilever stiffness calibration method using a MEMS nano-force transducer Traceable cantilever stiffness calibration method using a MEMS nano-force transducer Sai Gao 1, Uwe Brand 1, Wolfgang Engl 2, Thomas Sulzbach 2 1 PTB, 5.11 Hardness and tactile probing methods 2 Nanoworld

More information

Dually Fed Permanent Magnet Synchronous Generator Condition Monitoring Using Stator Current

Dually Fed Permanent Magnet Synchronous Generator Condition Monitoring Using Stator Current Summary Dually Fed Permanent Magnet Synchronous Generator Condition Monitoring Using Stator Current Joachim Härsjö, Massimo Bongiorno and Ola Carlson Chalmers University of Technology Energi och Miljö,

More information

State Newton's second law of motion for a particle, defining carefully each term used.

State Newton's second law of motion for a particle, defining carefully each term used. 5 Question 1. [Marks 28] An unmarked police car P is, travelling at the legal speed limit, v P, on a straight section of highway. At time t = 0, the police car is overtaken by a car C, which is speeding

More information

ENERGY TRANSFER SYSTEMS AND THEIR DYNAMIC ANALYSIS

ENERGY TRANSFER SYSTEMS AND THEIR DYNAMIC ANALYSIS ENERGY TRANSFER SYSTEMS AND THEIR DYNAMIC ANALYSIS Many mechanical energy systems are devoted to transfer of energy between two points: the source or prime mover (input) and the load (output). For chemical

More information

NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY WITH STM AND AFM PROBES

NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY WITH STM AND AFM PROBES Vol. 93 (1997) A CTA PHYSICA POLONICA A No. 2 Proceedings of the 1st International Symposium on Scanning Probe Spectroscopy and Related Methods, Poznań 1997 NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY

More information

Keysight Technologies How to Choose your MAC Lever. Technical Overview

Keysight Technologies How to Choose your MAC Lever. Technical Overview Keysight Technologies How to Choose your MAC Lever Technical Overview Introduction Atomic force microscopy (AFM) is a sub-nanometer scale imaging and measurement tool that can be used to determine a sample

More information

Loop Bandwidth and Clock Data Recovery (CDR) in Oscilloscope Measurements. Application Note 1304-6

Loop Bandwidth and Clock Data Recovery (CDR) in Oscilloscope Measurements. Application Note 1304-6 Loop Bandwidth and Clock Data Recovery (CDR) in Oscilloscope Measurements Application Note 1304-6 Abstract Time domain measurements are only as accurate as the trigger signal used to acquire them. Often

More information

Lezione 6 Communications Blockset

Lezione 6 Communications Blockset Corso di Tecniche CAD per le Telecomunicazioni A.A. 2007-2008 Lezione 6 Communications Blockset Ing. Marco GALEAZZI 1 What Is Communications Blockset? Communications Blockset extends Simulink with a comprehensive

More information

ATOMIC FORCE MICROSCOPE CANTILEVER WITH REDUCED SECOND HARMONIC FREQUENCY DURING TIP-SURFACE CONTACT JONATHAN R. FELTS THESIS

ATOMIC FORCE MICROSCOPE CANTILEVER WITH REDUCED SECOND HARMONIC FREQUENCY DURING TIP-SURFACE CONTACT JONATHAN R. FELTS THESIS ATOMIC FORCE MICROSCOPE CANTILEVER WITH REDUCED SECOND HARMONIC FREQUENCY DURING TIP-SURFACE CONTACT BY JONATHAN R. FELTS THESIS Submitted in partial fulfillment of the requirements for the degree of Master

More information

Candidate Number. General Certificate of Education Advanced Level Examination June 2012

Candidate Number. General Certificate of Education Advanced Level Examination June 2012 entre Number andidate Number Surname Other Names andidate Signature General ertificate of Education dvanced Level Examination June 212 Physics PHY4/1 Unit 4 Fields and Further Mechanics Section Monday

More information

Indiana's Academic Standards 2010 ICP Indiana's Academic Standards 2016 ICP. map) that describe the relationship acceleration, velocity and distance.

Indiana's Academic Standards 2010 ICP Indiana's Academic Standards 2016 ICP. map) that describe the relationship acceleration, velocity and distance. .1.1 Measure the motion of objects to understand.1.1 Develop graphical, the relationships among distance, velocity and mathematical, and pictorial acceleration. Develop deeper understanding through representations

More information

Procon Engineering. Technical Document PELR 1002. TERMS and DEFINITIONS

Procon Engineering. Technical Document PELR 1002. TERMS and DEFINITIONS Procon Engineering Technical Document PELR 1002 TERMS and DEFINITIONS The following terms are widely used in the weighing industry. Informal comment on terms is in italics and is not part of the formal

More information

Nanoscience Course Descriptions

Nanoscience Course Descriptions Nanoscience Course Descriptions NANO*1000 Introduction to Nanoscience This course introduces students to the emerging field of nanoscience. Its representation in popular culture and journalism will be

More information

Case Studies on Paper Machine Vibration Problems

Case Studies on Paper Machine Vibration Problems Case Studies on Paper Machine Vibration Problems Andrew K. Costain, B.Sc.Eng. Bretech Engineering Ltd., 70 Crown Street, Saint John, NB Canada E2L 3V6 email: andrew.costain@bretech.com website: www.bretech.com

More information

AFM (Atomic Force Microscope) Instructions

AFM (Atomic Force Microscope) Instructions AFM (Atomic Force Microscope) Instructions Contact Mode AFM Advantages: High scan speeds (throughput) Contact mode AFM is the only AFM technique, which can obtain "atomic resolution" images. Rough samples

More information

DEGREE: Bachelor's Degree in Industrial Electronics and Automation COURSE: 1º TERM: 2º WEEKLY PLANNING

DEGREE: Bachelor's Degree in Industrial Electronics and Automation COURSE: 1º TERM: 2º WEEKLY PLANNING SESSION WEEK COURSE: Physics II DEGREE: Bachelor's Degree in Industrial Electronics and Automation COURSE: 1º TERM: 2º WEEKLY PLANNING DESCRIPTION GROUPS (mark ) Indicate YES/NO If the session needs 2

More information

Scanning Tunneling Microscopy: Fundamentals and Applications

Scanning Tunneling Microscopy: Fundamentals and Applications McGill University, Montreal, March 30 th 2007 Scanning Tunneling Microscopy: Fundamentals and Applications Federico Rosei Canada Research Chair in Nanostructured Organic and Inorganic Materials Énergie,

More information

Manufacturing Equipment Modeling

Manufacturing Equipment Modeling QUESTION 1 For a linear axis actuated by an electric motor complete the following: a. Derive a differential equation for the linear axis velocity assuming viscous friction acts on the DC motor shaft, leadscrew,

More information

Relationship between large subject matter areas

Relationship between large subject matter areas H02M APPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER;

More information

Deconvolution of Atomic Force Measurements in Special Modes Methodology and Application

Deconvolution of Atomic Force Measurements in Special Modes Methodology and Application 1 Deconvolution of Atomic Force Measurements in Special Modes Methodolog and Application Dipl.-Ing. T. Machleidt PD Dr.-Ing. habil. K.-H. Franke Dipl.-Ing. E. Sparrer Computer Graphics Group / TU-Ilmenau

More information

nanovea.com MECHANICAL TESTERS Indentation Scratch Wear

nanovea.com MECHANICAL TESTERS Indentation Scratch Wear MECHANICAL TESTERS Indentation Scratch Wear nanovea.com MECHANICAL TESTER INTRO Nanovea Mechanical Testers provide unmatched multi-function Nano and Micro/Macro modules on a single platform. Both the Nano

More information

- thus, the total number of atoms per second that absorb a photon is

- thus, the total number of atoms per second that absorb a photon is Stimulated Emission of Radiation - stimulated emission is referring to the emission of radiation (a photon) from one quantum system at its transition frequency induced by the presence of other photons

More information

Energia da vibrazioni

Energia da vibrazioni Energy harves,ng Energia da vibrazioni Luca Gammaitoni Dipar,mento di Fisica, Università di Perugia www.nipslab.org Energy required to operate the portable devices Energy available from portable sources

More information

Raman Spectroscopy Basics

Raman Spectroscopy Basics Raman Spectroscopy Basics Introduction Raman spectroscopy is a spectroscopic technique based on inelastic scattering of monochromatic light, usually from a laser source. Inelastic scattering means that

More information