Nanoscale Resolution Options for Optical Localization Techniques. C. Boit TU Berlin Chair of Semiconductor Devices
|
|
- Paula Chrystal Wilkins
- 4 years ago
- Views:
Transcription
1 berlin Nanoscale Resolution Options for Optical Localization Techniques C. Boit TU Berlin Chair of Semiconductor Devices EUFANET Workshop on Optical Localization Techniques Toulouse, Jan 26, 2009
2 Jan 26, 2009 EUFANET 09 Toulouse 2 Nanoprobing of Identified Node Resolution < 50nm Parallel lapping down to contact layer Isolated devices Low ohmic contact Destructive to circuit AFM Feedback Tip Detector Probe Tip Piezo AFP needles tungsten contacts Laser Additonal Signals IMD W PW bulk-si NW bulk Silicon
3 Jan 26, 2009 EUFANET 09 Toulouse 3 Optical Backside Circuit Analysis GHz regime managed by most dynamic techniques Feature Size Resolution: 2 levels of analysis Level 1: IR + SIL to identify critical area Level 2: Nanoprobing to verify critical node prep circuit destructive increasing need for a high resolution optical localization technique Laser Stimulated Electrical Signal LVP Laser CCD Photon Emission
4 Trench Floor Planarity Jan 26, 2009 EUFANET 09 Toulouse 4 Global navigation through silicon with co-axial IR and ion column IR-Microscope Ion Beam DCG Systems - OptiFIB ΔZ 130nm Co-planarity check of trench bottom to chip levels with interference rings (fringes)
5 Jan 26, 2009 EUFANET 09 Toulouse 5 FIB Ultra Thin Back Surface Procedure mechanical thinning localized FIB trench -1 st endpoint on n-wells voltage image contrast -2 nd endpoint on STI material image contrast < 400nm remaining Si local high precision alignment actives 150µm STI n wells poly p-diff n-diff ARC µm 2 STI
6 frontside AFP backside TUB ISTFA 07 parallel lapping down to contact layer isolated devices low ohmic contact Destructive to circuit FIB backside process devices not isolated creation of new circuit nodes Circuit fully functional AFP needles tungsten contacts IMD W FIB Pt D S G PW bulk-si NW bulk Silicon Jan 26, 2009 EUFANET 09 Toulouse 6
7 UltraThin Si - Ideal Platform for NanoAnalysis Jan 26, 2009 EUFANET 09 Toulouse 7 Ultra Thin Backside Technique Visible or UV Laser Stimulation Nanoprobing, C-AFM IR Technique LADA, Dyn. LS TUB Research E-Beam Techniques: - Voltage probing LVP, TRE - E Beam induced photocurrent LADA, Dyn. LS STI e - Light Nano Probes M1 M2 350nm n-well
8 Dual Gates: Ultra Thin Body not to scale etc M2 M2 Cu M1 W CoSi ILD p-poly n-poly p + NW STI STI n + PW p-poly 0,3µm BOX = Buried Oxide n-poly 100µm 1,5µm SX SX Jan 26, 2009 EUFANET 09 Toulouse 8
9 Jan 26, 2009 EUFANET 09 Toulouse 9 Interaction Dimensions Gate length Technology UTS (SOI PD) UTB (SOI FD / Dual Gate etc) 100nm 100nm 40nm 50nm 40nm 50nm
10 Backside Access: Transmission of Light in Silicon Jan 26, 2009 EUFANET 09 Toulouse 10 Spectral Absorption in Silicon Soref et al., IEEE J. of Quant. Elec., Vol. QE-23, No.1, January Concentration of free electrons N [x cm -3 ] UTS: 350nm α (cm -1 ) Blue Light 430nm (2.8 ev): α 350nm undoped T = 300 K Photon Energy (ev) UTB: UV? EBeam?
11 Jan 26, 2009 EUFANET 09 Toulouse 11 SNOM on UTB Resolution = f (tip geometry, working distance) but independent of wavelength! Photon Emission III-V Ge STI
12 Jan 26, 2009 EUFANET 09 Toulouse 12 SNOM on UTB Photon Emission Laser Stimulation - transferred power? LVP - SNR? III-V Ge STI
13 Jan 26, 2009 EUFANET 09 Toulouse 13 Resolution = f (tip geometry, working distance) but independent of wavelength! SNOM on UTB III-V Ge STI
14 Jan 26, 2009 EUFANET 09 Toulouse 14 Photon Emission LVP - SNR? Laser Stimulation - transferred power? Thermal LS when tip is scanning over STI SNOM on UTB III-V Ge STI
15 Jan 26, 2009 EUFANET 09 Toulouse 15 FET Delay Variation on Defined Node shorter wave length absorption depth 100nm optical confinement by FIB trench - waveguide - impact only on exposed transistor hν Resolution of stimulation by confinement
16 FIB Guided SNOM on UTB Jan 26, 2009 EUFANET 09 Toulouse 16 Adaption of Sidewalls to Fiber? Better thermal management: Narrow FIB Trench to UTS Trench as waveguide? or for Fiber probing? Ge STI III-V
17 FIBbed SIL Jan 26, 2009 EUFANET 09 Toulouse 17 Solid Immersion Lens (SIL) created out of the bulk silicon material perpendicular transition Si / air, no refraction sample surface (chip backside) removed material object plane
18 Results Jan 26, 2009 EUFANET 09 Toulouse 18 Images of the SIL (r 91 µm, t 34 µm) using a laser scanning microscope at wavelength λ = 1064 nm 30µm 30µm focused on SIL focused on background
19 Jan 26, 2009 EUFANET 09 Toulouse 19 Nanoscale Potential TUB Research Technique Resolution Potential Comment Optical through 500nm 100nm Limited bulk Si (IR) (SIL) resolution Nanoprobing 50nm 10nm Limited dynamics E Beam 100nm Material degradation? Optical through 300nm < 100nm Realization ultra thin Silicon (SIL) complex UV through ultra 150nm < 50nm Material thin silicon degradation?
20 Jan 26, 2009 EUFANET 09 Toulouse 20
21 Ultra Thin Body UTB Jan 26, 2009 EUFANET 09 Toulouse 21 SOI: Partially depleted = PD Fully Depleted FD V GS = 0 Poly Gate Depleted Si BOX Si V GS > V T Conductive Channel Subthreshold Slope 60mV / dec FD active layer => UTB
Lecture 030 DSM CMOS Technology (3/24/10) Page 030-1
Lecture 030 DSM CMOS Technology (3/24/10) Page 030-1 LECTURE 030 - DEEP SUBMICRON (DSM) CMOS TECHNOLOGY LECTURE ORGANIZATION Outline Characteristics of a deep submicron CMOS technology Typical deep submicron
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
DualBeam Solutions for Electrical Nanoprobing
DualBeam Solutions for Electrical Nanoprobing Richard J. Young, Technologist Peter D. Carleson, Product Marketing Engineer Electrical testing by physically probing device structures has grown more challenging
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
Mass production, R&D Failure analysis. Fault site pin-pointing (EM, OBIRCH, FIB, etc. ) Bottleneck Physical science analysis (SEM, TEM, Auger, etc.
Failure Analysis System for Submicron Semiconductor Devices 68 Failure Analysis System for Submicron Semiconductor Devices Munetoshi Fukui Yasuhiro Mitsui, Ph. D. Yasuhiko Nara Fumiko Yano, Ph. D. Takashi
Winbond W971GG6JB-25 1 Gbit DDR2 SDRAM 65 nm CMOS DRAM Process
Winbond W971GG6JB-25 1 Gbit DDR2 SDRAM 65 nm CMOS DRAM Process Process Review For comments, questions, or more information about this report, or for any additional technical needs concerning semiconductor
ING LA PALMA TECHNICAL NOTE No. 130. Investigation of Low Fringing Detectors on the ISIS Spectrograph.
ING LA PALMA TECHNICAL NOTE No. 130 Investigation of Low Fringing Detectors on the ISIS Spectrograph. Simon Tulloch (ING) June 2005 Investigation of Low Fringing Detectors on the ISIS Spectrograph. 1.
Advanced VLSI Design CMOS Processing Technology
Isolation of transistors, i.e., their source and drains, from other transistors is needed to reduce electrical interactions between them. For technologies
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
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
Limiting factors in fiber optic transmissions
Limiting factors in fiber optic transmissions Sergiusz Patela, Dr Sc Room I/48, Th. 13:00-16:20, Fri. 9:20-10:50 sergiusz.patela@pwr.wroc.pl eportal.pwr.wroc.pl Copying and processing permitted for noncommercial
Near-field scanning optical microscopy (SNOM)
Adviser: dr. Maja Remškar Institut Jožef Stefan January 2010 1 2 3 4 5 6 Fluorescence Raman and surface enhanced Raman 7 Conventional optical microscopy-limited resolution Two broad classes of techniques
Optical Microscopy Beyond the Diffraction Limit: Imaging Guided and Propagating Fields
Optical Microscopy Beyond the Diffraction Limit: Imaging Guided and Propagating Fields M. Selim Ünlü, Bennett B. Goldberg, and Stephen B. Ippolito Boston University Department of Electrical and Computer
Physics 441/2: Transmission Electron Microscope
Physics 441/2: Transmission Electron Microscope Introduction In this experiment we will explore the use of transmission electron microscopy (TEM) to take us into the world of ultrasmall structures. This
Photonic components for signal routing in optical networks on chip
15 th International Conference on Transparent Optical Networks Cartagena, Spain, June 23-27, 213 Photonic components for signal routing in optical networks on chip Vincenzo Petruzzelli, Giovanna Calò Dipartimento
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
Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting
Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting 3G Solar Technologies Multidisciplinary Workshop MRS Spring Meeting San Francisco, CA, 5 April 2010 Michael P.
Substrate maturity and readiness in large volume to support mass adoption of ULP FDSOI platforms. SOI Consortium Conference Tokyo 2016
Substrate maturity and readiness in large volume to support mass adoption of ULP FDSOI platforms Christophe Maleville Substrate readiness 3 lenses view SOI Consortium C1 - Restricted Conference Tokyo 2016
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,
Acoustic GHz-Microscopy: Potential, Challenges and Applications
Acoustic GHz-Microscopy: Potential, Challenges and Applications A Joint Development of PVA TePLa Analytical Systems GmbH and Fraunhofer IWM-Halle Dr. Sebastian Brand (Ph.D.) Fraunhofer CAM Fraunhofer Institute
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
IN LEITERPLATTEN INTEGRIERTE OPTISCHE VERBINDUNGSTECHNIK AUF DÜNNGLASBASIS
IN LEITERPLATTEN INTEGRIERTE OPTISCHE VERBINDUNGSTECHNIK AUF DÜNNGLASBASIS Dr. Henning Schröder henning.schroeder@izm.fraunhofer.de, phone: +49 30 46403 277 Outlook n Motivation n Manufacturing n Waveguide
Optical Communications
Optical Communications Telecommunication Engineering School of Engineering University of Rome La Sapienza Rome, Italy 2005-2006 Lecture #2, May 2 2006 The Optical Communication System BLOCK DIAGRAM OF
DESIGN, FABRICATION AND ELETRICAL CHARACTERIZATION OF SOI FINFET TRANSISTORS
DESIGN, FABRICATION AND ELETRICAL CHARACTERIZATION OF SOI FINFET TRANSISTORS Prof. Dr. João Antonio Martino Professor Titular Departamento de Engenharia de Sistemas Eletrônicos Escola Politécnica da Universidade
Silicon photonics: low cost and high performance. L. Pavesi 18-11-10
Silicon photonics: a new technology platform to enable low cost and high performance photonics Outline Silicon Photonics State of the art Silicon Photonics for lab-on-a-chip NanoSilicon photonics Conclusion
Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014
Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014 Introduction Following our previous lab exercises, you now have the skills and understanding to control
CSCI 4974 / 6974 Hardware Reverse Engineering. Lecture 8: Microscopy and Imaging
CSCI 4974 / 6974 Hardware Reverse Engineering Lecture 8: Microscopy and Imaging Data Acquisition for RE Microscopy Imaging Registration and stitching Microscopy Optical Electron Scanning Transmission Scanning
h e l p s y o u C O N T R O L
contamination analysis for compound semiconductors ANALYTICAL SERVICES B u r i e d d e f e c t s, E v a n s A n a l y t i c a l g r o u p h e l p s y o u C O N T R O L C O N T A M I N A T I O N Contamination
Intel s Revolutionary 22 nm Transistor Technology
Intel s Revolutionary 22 nm Transistor Technology Mark Bohr Intel Senior Fellow Kaizad Mistry 22 nm Program Manager May, 2011 1 Key Messages Intel is introducing revolutionary Tri-Gate transistors on its
Fiber Optics: Engineering from Global to Nanometer Dimensions
Fiber Optics: Engineering from Global to Nanometer Dimensions Prof. Craig Armiento Fall 2003 1 Optical Fiber Communications What is it? Transmission of information using light over an optical fiber Why
Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope
andras@nist.gov Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope Bin Ming, András E. Vladár and Michael T. Postek National Institute of Standards and Technology
PHYS 222 Spring 2012 Final Exam. Closed books, notes, etc. No electronic device except a calculator.
PHYS 222 Spring 2012 Final Exam Closed books, notes, etc. No electronic device except a calculator. NAME: (all questions with equal weight) 1. If the distance between two point charges is tripled, the
L innovazione tecnologica dell industria italiana verso la visione europea del prossimo futuro
L innovazione tecnologica dell industria italiana verso la visione europea del prossimo futuro Mercoledì 2 Aprile 2014 Antonio D Errico, Francesco Testa, Roberto Sabella, Ericsson Silicon Photonics Opportunities
Keywords: Planar waveguides, sol-gel technology, transmission electron microscopy
Structural and optical characterisation of planar waveguides obtained via Sol-Gel F. Rey-García, C. Gómez-Reino, M.T. Flores-Arias, G.F. De La Fuente, W. Assenmacher, W. Mader ABSTRACT Planar waveguides
Measuring of optical output and attenuation
Measuring of optical output and attenuation THEORY Measuring of optical output is the fundamental part of measuring in optoelectronics. The importance of an optical power meter can be compared to an ammeter
BROADBAND PHOTOCURRENT ENHANCEMENT IN LONGWAVE INFRARED QUANTUM DOT PHOTODETECTORS BY SUB-WAVELENGTH SURFACE GRATINGS
Optics and Photonics Letters Vol. 6, No. 1 (2013) 1350002 (6 pages) c World Scientific Publishing Company DOI: 10.1142/S1793528813500020 BROADBAND PHOTOCURRENT ENHANCEMENT IN LONGWAVE INFRARED QUANTUM
Fundamentals of modern UV-visible spectroscopy. Presentation Materials
Fundamentals of modern UV-visible spectroscopy Presentation Materials The Electromagnetic Spectrum E = hν ν = c / λ 1 Electronic Transitions in Formaldehyde 2 Electronic Transitions and Spectra of Atoms
Nano Optics: Overview of Research Activities. Sergey I. Bozhevolnyi SENSE, University of Southern Denmark, Odense, DENMARK
Nano Optics: Overview of Research Activities SENSE, University of Southern Denmark, Odense, DENMARK Optical characterization techniques: Leakage Radiation Microscopy Scanning Near-Field Optical Microscopy
Apertureless Near-Field Optical Microscopy
VI Apertureless Near-Field Optical Microscopy In recent years, several types of apertureless near-field optical microscopes have been developed 1,2,3,4,5,6,7. In such instruments, light scattered from
Avalanche Photodiodes: A User's Guide
!"#$%& Abstract Avalanche Photodiodes: A User's Guide Avalanche photodiode detectors have and will continue to be used in many diverse applications such as laser range finders and photon correlation studies.
SMA5111 - Compound Semiconductors Lecture 2 - Metal-Semiconductor Junctions - Outline Introduction
SMA5111 - Compound Semiconductors Lecture 2 - Metal-Semiconductor Junctions - Outline Introduction Structure - What are we talking about? Behaviors: Ohmic, rectifying, neither Band picture in thermal equilibrium
Volumes. Goal: Drive optical to high volumes and low costs
First Electrically Pumped Hybrid Silicon Laser Sept 18 th 2006 The information in this presentation is under embargo until 9/18/06 10:00 AM PST 1 Agenda Dr. Mario Paniccia Director, Photonics Technology
AMD AXDA3000DKV4D Athlon TM XP Microprocessor Structural Analysis
September 22, 2004 AMD AXDA3000DKV4D Athlon TM XP Microprocessor Structural Analysis Table of Contents Introduction... Page 1 List of Figures... Page 2 Device Identification Major Microstructural Analysis
ME 472 Engineering Metrology
ME 472 Engineering Metrology and Quality Control Chp 6 - Advanced Measurement Systems Mechanical Engineering University of Gaziantep Dr. A. Tolga Bozdana Assistant Professor Coordinate Measuring Machines
View of ΣIGMA TM (Ref. 1)
Overview of the FESEM system 1. Electron optical column 2. Specimen chamber 3. EDS detector [Electron Dispersive Spectroscopy] 4. Monitors 5. BSD (Back scatter detector) 6. Personal Computer 7. ON/STANDBY/OFF
Single Photon Counting Module COUNT -Series
Description Laser Components COUNT series of s has been developed to offer a unique combination of high photon detection efficiency, wide dynamic range and ease of use for photon counting applications.
Numeric modeling of synchronous laser pulsing and voltage pulsing field evaporation
Numeric modeling of synchronous laser pulsing and voltage pulsing field evaporation L. ZHAO 1, A. NORMAND, J. HOUARD, I. BLUM, F. DELAROCHE, F. VURPILLOT Normandie Univ, UNIROUEN, INSA Rouen, CNRS, GPM,
Electrical tests on PCB insulation materials and investigation of influence of solder fillets geometry on partial discharge
, Firenze, Italy Electrical tests on PCB insulation materials and investigation of influence of solder fillets geometry on partial discharge A. Bulletti, L. Capineri B. Dunn ESTEC Material and Process
The MOSFET Transistor
The MOSFET Transistor The basic active component on all silicon chips is the MOSFET Metal Oxide Semiconductor Field Effect Transistor Schematic symbol G Gate S Source D Drain The voltage on the gate controls
High power picosecond lasers enable higher efficiency solar cells.
White Paper High power picosecond lasers enable higher efficiency solar cells. The combination of high peak power and short wavelength of the latest industrial grade Talisker laser enables higher efficiency
High-Performance Wavelength-Locked Diode Lasers
Copyright 29 Society of Photo-Optical Instrumentation Engineers. This paper was published in the proceedings of the SPIE Photonics West 29, Vol. 7198-38 (29), High-Power Diode Laser Technology and High-Performance
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
WAVELENGTH OF LIGHT - DIFFRACTION GRATING
PURPOSE In this experiment we will use the diffraction grating and the spectrometer to measure wavelengths in the mercury spectrum. THEORY A diffraction grating is essentially a series of parallel equidistant
3D TOPOGRAPHY & IMAGE OVERLAY OF PRINTED CIRCUIT BOARD ASSEMBLY
3D TOPOGRAPHY & IMAGE OVERLAY OF PRINTED CIRCUIT BOARD ASSEMBLY Prepared by Duanjie Li, PhD & Andrea Novitsky 6 Morgan, Ste156, Irvine CA 92618 P: 949.461.9292 F: 949.461.9232 nanovea.com Today's standard
Surface plasmon nanophotonics: optics below the diffraction limit
Surface plasmon nanophotonics: optics below the diffraction limit Albert Polman Center for nanophotonics FOM-Institute AMOLF, Amsterdam Jeroen Kalkman Hans Mertens Joan Penninkhof Rene de Waele Teun van
104 Practice Exam 2-3/21/02
104 Practice Exam 2-3/21/02 1. Two electrons are located in a region of space where the magnetic field is zero. Electron A is at rest; and electron B is moving westward with a constant velocity. A non-zero
From apertureless near-field optical microscopy to infrared near-field night vision
From apertureless near-field optical microscopy to infrared near-field night vision Yannick DE WILDE ESPCI Laboratoire d Optique Physique UPR A0005-CNRS, PARIS dewilde@optique.espci.fr From apertureless
Implementation of Short Reach (SR) and Very Short Reach (VSR) data links using POET DOES (Digital Opto- electronic Switch)
Implementation of Short Reach (SR) and Very Short Reach (VSR) data links using POET DOES (Digital Opto- electronic Switch) Summary POET s implementation of monolithic opto- electronic devices enables the
Scientific Exchange Program
Scientific Exchange Program Electrical characterization of photon detectors based on acoustic charge transport Dr. Paulo Santos, Paul Drude Institute, Berlin,Germany Dr. Pablo Diniz Batista, Brazilian
STMicroelectronics. Deep Sub-Micron Processes 130nm, 65 nm, 40nm, 28nm CMOS, 28nm FDSOI. SOI Processes 130nm, 65nm. SiGe 130nm
STMicroelectronics Deep Sub-Micron Processes 130nm, 65 nm, 40nm, 28nm CMOS, 28nm FDSOI SOI Processes 130nm, 65nm SiGe 130nm CMP Process Portfolio from ST Moore s Law 130nm CMOS : HCMOS9GP More than Moore
Technology Developments Towars Silicon Photonics Integration
Technology Developments Towars Silicon Photonics Integration Marco Romagnoli Advanced Technologies for Integrated Photonics, CNIT Venezia - November 23 th, 2012 Medium short reach interconnection Example:
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
Electron Microscopy 3. SEM. Image formation, detection, resolution, signal to noise ratio, interaction volume, contrasts
Electron Microscopy 3. SEM Image formation, detection, resolution, signal to noise ratio, interaction volume, contrasts 3-1 SEM is easy! Just focus and shoot "Photo"!!! Please comment this picture... Any
Analyzing Electrical Effects of RTA-driven Local Anneal Temperature Variation
1 Analyzing Electrical Effects of RTA-driven Local Anneal Temperature Variation Vivek Joshi, Kanak Agarwal*, Dennis Sylvester, David Blaauw Electrical Engineering & Computer Science University of Michigan,
DOE Solar Energy Technologies Program Peer Review. Denver, Colorado April 17-19, 2007
DOE Solar Energy Technologies Program Peer Review Evaluation of Nanocrystalline Silicon Thin Film by Near-Field Scanning Optical Microscopy AAT-2-31605-05 Magnus Wagener and George Rozgonyi North Carolina
INFRARED PARTS MANUAL
INFRARED PARTS MANUAL PIR325 FL65 GLOLAB CORPORATION Thank you for buying our Pyroelectric Infrared components. The goal of Glolab is to produce top quality electronic kits, products and components. All
Recent developments in high bandwidth optical interconnects. Brian Corbett. www.tyndall.ie
Recent developments in high bandwidth optical interconnects Brian Corbett Outline Introduction to photonics for interconnections Polymeric waveguides and the Firefly project Silicon on insulator (SOI)
A More Efficient Way to De-shelve 137 Ba +
A More Efficient Way to De-shelve 137 Ba + Abstract: Andrea Katz Trinity University UW REU 2010 In order to increase the efficiency and reliability of de-shelving barium ions, an infrared laser beam was
Silicon-On-Glass MEMS. Design. Handbook
Silicon-On-Glass MEMS Design Handbook A Process Module for a Multi-User Service Program A Michigan Nanofabrication Facility process at the University of Michigan March 2007 TABLE OF CONTENTS Chapter 1...
Introduction to VLSI Fabrication Technologies. Emanuele Baravelli
Introduction to VLSI Fabrication Technologies Emanuele Baravelli 27/09/2005 Organization Materials Used in VLSI Fabrication VLSI Fabrication Technologies Overview of Fabrication Methods Device simulation
Hard Condensed Matter WZI
Hard Condensed Matter WZI Tom Gregorkiewicz University of Amsterdam VU-LaserLab Dec 10, 2015 Hard Condensed Matter Cluster Quantum Matter Optoelectronic Materials Quantum Matter Amsterdam Mark Golden Anne
DETECTION OF SUBSURFACE DAMAGE IN OPTICAL TRANSPARENT MATERIALSS USING SHORT COHERENCE TOMOGRAPHY. Rainer Boerret, Dominik Wiedemann, Andreas Kelm
URN (Paper): urn:nbn:de:gbv:ilm1-2014iwk-199:0 58 th ILMENAU SCIENTIFIC COLLOQUIUM Technische Universität Ilmenau, 08 12 September 2014 URN: urn:nbn:de:gbv:ilm1-2014iwk:3 DETECTION OF SUBSURFACE DAMAGE
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
Sun to Fiber: a thin film optical funnel for energy conversion and storage
Sun to Fiber: a thin film optical funnel for energy conversion and storage Matthew Garrett, Juan J. Díaz León, Kailas Vodrahalli, Taesung Kim, Ernest Demaray, Nobuhiko Kobayashi Department of Electrical
Spectroscopic Ellipsometry:
Spectroscopic : What it is, what it will do, and what it won t do by Harland G. Tompkins Introduction Fundamentals Anatomy of an ellipsometric spectrum Analysis of an ellipsometric spectrum What you can
X-Rays and Magnetism From Fundamentals to Nanoscale Dynamics
X-Rays and Magnetism From Fundamentals to Nanoscale Dynamics Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-rays have come a long way 1895 1993 10 cm 10 µm 100 nm Collaborators: SSRL Stanford:
Integrated optics Er-Yb amplifier with potassium ion-exchanged glass waveguides
Integrated optics Er-Yb amplifier with potassium ion-exchanged glass waveguides P. Meshkinfam 1, P. Fournier', M.A. Fardad 2, M. P. Andrews 2, and S. I. Najafl' 1 Photonics Research Group, Ecole Polytechnique,
Raman spectroscopy Lecture
Raman spectroscopy Lecture Licentiate course in measurement science and technology Spring 2008 10.04.2008 Antti Kivioja Contents - Introduction - What is Raman spectroscopy? - The theory of Raman spectroscopy
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
Project 2B Building a Solar Cell (2): Solar Cell Performance
April. 15, 2010 Due April. 29, 2010 Project 2B Building a Solar Cell (2): Solar Cell Performance Objective: In this project we are going to experimentally measure the I-V characteristics, energy conversion
Meridian TM WS-DP Next Generation Wafer Based Electrical Fault Isolation System to Improve Yield Ramp
Meridian TM WS-DP Next Generation Wafer Based Electrical Fault Isolation System to Improve Yield Ramp 曹 君 正 Chun-Cheng Tsao September 30, 2014 Find defects that matter Outline Introduction to Meridian
3D Raman Imaging Nearfield-Raman TERS. Solutions for High-Resolution Confocal Raman Microscopy. www.witec.de
3D Raman Imaging Nearfield-Raman TERS Solutions for High-Resolution Confocal Raman Microscopy www.witec.de 01 3D Confocal Raman Imaging Outstanding performance in speed, sensitivity, and resolution with
Application Note AN1
TAKING INVENTIVE STEPS IN INFRARED. MINIATURE INFRARED GAS SENSORS GOLD SERIES UK Patent App. No. 799A USA Patent App. No. 9/78,7 World Patents Pending SENSOR OVERVIEW Application Note AN The Dynament
Realization of a UV fisheye hyperspectral camera
Realization of a UV fisheye hyperspectral camera Valentina Caricato, Andrea Egidi, Marco Pisani and Massimo Zucco, INRIM Outline Purpose of the instrument Required specs Hyperspectral technique Optical
ENGINEERING METROLOGY
ENGINEERING METROLOGY ACADEMIC YEAR 92-93, SEMESTER ONE COORDINATE MEASURING MACHINES OPTICAL MEASUREMENT SYSTEMS; DEPARTMENT OF MECHANICAL ENGINEERING ISFAHAN UNIVERSITY OF TECHNOLOGY Coordinate Measuring
Spectroscopy. Biogeochemical Methods OCN 633. Rebecca Briggs
Spectroscopy Biogeochemical Methods OCN 633 Rebecca Briggs Definitions of Spectrometry Defined by the method used to prepare the sample 1. Optical spectrometry Elements are converted to gaseous atoms or
Components for Infrared Spectroscopy. Dispersive IR Spectroscopy
Components for Infrared Spectroscopy Mid-IR light: 00-000 cm - (5.5 m wavelength) Sources: Blackbody emitters Globar metal oxides Nernst Glower: Silicon Carbide Detectors: Not enough energy for photoelectric
The Focused Ion Beam Scanning Electron Microscope: A tool for sample preparation, two and three dimensional imaging. Jacob R.
The Focused Ion Beam Scanning Electron Microscope: A tool for sample preparation, two and three dimensional imaging Jacob R. Bowen Contents Components of a FIB-SEM Ion interactions Deposition & patterns
Conductivity of silicon can be changed several orders of magnitude by introducing impurity atoms in silicon crystal lattice.
CMOS Processing Technology Silicon: a semiconductor with resistance between that of conductor and an insulator. Conductivity of silicon can be changed several orders of magnitude by introducing impurity
(Amplifying) Photo Detectors: Avalanche Photodiodes Silicon Photomultiplier
(Amplifying) Photo Detectors: Avalanche Photodiodes Silicon Photomultiplier (no PiN and pinned Diodes) Peter Fischer P. Fischer, ziti, Uni Heidelberg, Seite 1 Overview Reminder: Classical Photomultiplier
Composants actifs ultra rapides pour les composants et interconnexions optiques intégrées
Composants actifs ultra rapides pour les composants et interconnexions optiques intégrées Jean-Marc Fedeli CEA,LETI, MinatecCampus, 17 rue des Martyrs, F-38054 GRENOBLE cedex 9, France Contact: jean-marc.fedeli@cea.fr
semiconductor software solutions Stefan Birner
Stefan Birner Schmalkaldener Str. 34 D-80807 Munich +49-89 35 89 53 34 Stefan Birner www.nextnano.de stefan.birner@nextnano.de Goal: Business plan & Spin-off Our vision: To establish as the de facto standard
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
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
Applications of confocal fluorescence microscopy in biological sciences
Applications of confocal fluorescence microscopy in biological sciences B R Boruah Department of Physics IIT Guwahati Email: brboruah@iitg.ac.in Page 1 Contents Introduction Optical resolution Optical
Module 13 : Measurements on Fiber Optic Systems
Module 13 : Measurements on Fiber Optic Systems Lecture : Measurements on Fiber Optic Systems Objectives In this lecture you will learn the following Measurements on Fiber Optic Systems Attenuation (Loss)
ADVANCED IC REVERSE ENGINEERING TECHNIQUES: IN DEPTH ANALYSIS OF A MODERN SMART CARD. Olivier THOMAS Blackhat USA 2015
ADVANCED IC REVERSE ENGINEERING TECHNIQUES: IN DEPTH ANALYSIS OF A MODERN SMART CARD Olivier THOMAS Blackhat USA 2015 About Texplained Texplained [Technology Explained] refers
Methods of plasma generation and plasma sources
Methods of plasma generation and plasma sources PlasTEP trainings course and Summer school 2011 Warsaw/Szczecin Indrek Jõgi, University of Tartu Partfinanced by the European Union (European Regional Development
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
Ultra-High Density Phase-Change Storage and Memory
Ultra-High Density Phase-Change Storage and Memory by Egill Skúlason Heated AFM Probe used to Change the Phase Presentation for Oral Examination 30 th of May 2006 Modern Physics, DTU Phase-Change Material