Angstrom Advanced Inc.. – 1056 Washington St., Canton, MA 02021 Tel. : 617-202-3880 Fax : 617-202-3878 Who we are: Angstrom.

Slides:



Advertisements
Similar presentations
Augustin Cauchy August 21, 1789 – May 23, Graduated in civil engineering and went to work as a junior engineer where Napoleon planned to build.
Advertisements

Introduction to TFCompanion © 2004 Semiconsoft, Inc. TFCompanion ver. 3.0.
Measuring film thickness using Opti-Probe
Bragg’s Law nl=2dsinΘ Just needs some satisfaction!! d Θ l
Spectroscopic Ellipsometry University of Texas at El Paso Lynn Santiago Dr. Elizabeth Gardner Chem 5369.
11 Components of Optical Instruments Lecture Spectroscopic methods are based on either: 1. Absorption 2. Emission 3. Scattering.
The AxoScan™ Ellipsometer
1 Components of Optical Instruments, Cont… Lecture 6.
SLAC National Accelerator Center
1 Extreme Ultraviolet Polarimetry Utilizing Laser-Generated High- Order Harmonics N. Brimhall, M. Turner, N. Herrick, D. Allred, R. S. Turley, M. Ware,
Deal-Grove Model Predictions Once B and B/A are determined, we can predict the thickness of the oxide versus time Once B and B/A are determined, we can.
Ellipsometry and X-ray Reflectivity (XRR)
Film Thickness Measurement Julian Peters Joe Fitzmyer Brad Demers P06402.
OL Series 754 Portable UV-VIS-NIR Spectroradiometer The OL 754 Portable UV-Visible-NIR Spectroradiometers are a series of compact, portable, double monochromator.
NIH 3T3 fibroblasts stained for Filamentous-actin Phalloidin Alexa Fluor 488 nm A. G. Sostarecz, P.A. Janmey, data not published.
Are you getting the concept? Calculate D a, D l, R d and s g for 1 st order diffraction under optimal conditions for the indicated 0.5 m grating with 100.
ARC 11/02/10 Recent Advances in Surface Plasmon Resonance: From Biosensor to Space/astronomical Interest Hololab and CSL S. Habraken, C. Lenaerts, and.
SiO2 thickness measurements Using the NanoSpec Model 200 Automatic Film Thickness tool.
Abstract The index of refraction of a material can be used to determine how light bends as the rays travel through a substance. Therefore, this property.
Silver / Polystyrene Coated Hollow Glass Waveguides for the Transmission of Visible and Infrared Radiation Carlos M. Bledt a and James A. Harrington a.
Pioneers in Non-contact Measurement. MTI Instruments, Inc.  Founded in now a public company listed on NASDAQ  Designs, manufactures and markets.
D EDICATED S PECTROPHOTOMETER F OR L OCALIZED T RANSMITTANCE A ND R EFLECTANCE M EASUREMENTS Laetitia ABEL-TIBERINI, Frédéric LEMARQUIS, Michel LEQUIME.
Overview of course Capabilities of photonic crystals Applications MW 3:10 - 4:25 PMFeatheringill 300 Professor Sharon Weiss.
Models The first major model is that of Deal and Grove (1965) The first major model is that of Deal and Grove (1965) This lead to the linear/parabolic.
The aerogel radiator: optical characterization and performances L.L. Pappalardo INFN - University of Ferrara 1 CLAS12 RICH Review – JLab - September 5-6.
Udo_ME2006.ppt, © Udo v. Toussaint, 11. July Bayesian Analysis of Ellipsometry Measurements Udo v. Toussaint and Thomas Schwarz-Selinger Ellipsometry.
Electrical and optical properties of organic materials are closely related to its molecular orientation. SE is employed in the understanding of molecular.
OL Series 750 Automated Spectroradiometric Measurement System The OL Series 750 is an extremely versatile spectroradiometric measurement system capable.
Tao Yuan, Jingzhou Xu, and Xicheng Zhang Rensselaer Polytechnic Institute, Troy, New York Scanning THz Emission Microscope Abstract A THz image system.
Divergent Illumination Optical Testing Device M. Fried 1, Z. Horváth 2, G. Juhász 1, T. Mosoni 1, P. Petrik 1 1 Research Institute for Technical Physics.
Peter J. LaPuma1 © 1998 BRUKER AXS, Inc. All Rights Reserved This is powder diffraction!
Divergent Illumination Optical Testing Device M. Fried 1, Z. Horváth 2, G. Juhász 1, O. Polgár 1, T. Mosoni 1, P. Petrik 1 1 Research Institute for Technical.
work for PID in Novosibirsk E.A.Kravchenko Budker INP, Novosibirsk.
NANO 225 Intro to Nano/Microfabrication
Compact High-Speed Spectroscopic Ellipsometer
Haga clic para modificar el estilo de texto del patrón Infrared transparent detectors Manuel Lozano G. Pellegrini, E. Cabruja, D. Bassignana, CNM (CSIC)
1.Stable radiation source 2.Wavelength selector 3.Transparent sample holder: cells/curvettes made of suitable material (Table 7- 2) 4.Radiation detector.
OL 750 Measurement Systems OL 750 Measurement Systems Optronic Laboratories, Inc.
EPFL – October 7 th Introduction to software J.Ph.PIEL (PhD) Application Lab Manager SOPRALAB.
Slide 1 5th LHC RADIATION WORKSHOP, CERN, , Jochen Kuhnhenn, Fraunhofer INT Radiation tolerant fibres for LHC controls and communications.
STUDY OF TRANSPARENT FERROELECTRIC THIN FILMS BY OPTICAL REFLECTOMETRY AND ELLIPSOMETRY I. Aulika Institute of Solid State Physics, University of Latvia,
SPECTRAL PRODUCTS INTRODUCTION 111 Highland Drive, Putnam, CT 06260, USA (East Office) 2659A Pan American Freeway NE, Albuquerque, NM 87107, USA (West.
Real-time Ellipsometry on Cesium-Telluride Photocathode Formation
The Authors - David Hall ● David Hall is an Electrical Engineer designing electronic circuits for almost 30 years. Most of that time was in the aerospace.
Speaker: Hao-Wen Chuang ( 莊浩彣 ) Advisor: Assistant Prof. Chung-Hao Tien Assistant Prof. Yi-Pai Huang Display Institute, National Chiao Tung University,
EPFL October 7 th Introduction to ellipsometry J.Ph.PIEL (PhD) Application Lab Manager SOPRALAB.
LIGHT BACKSCATTERING ANALYSIS of Textured Silicon SAMPLES
Evaluation of Polydimethlysiloxane (PDMS) as an adhesive for Mechanically Stacked Multi-Junction Solar Cells Ian Mathews Dept. of Electrical and Electronic.
UV/VIS SPECTROSCOPY.
Ekaterina N. Lazareva1,2 and Valery V. Tuchin1,2,3
Window Coating Absorbance Spectra
Design and Fabrication of Alumina/Silica Optical Bandpass Filter
Multiple Beam Interference
Laser Physics & Nonlinear Optics
BAHIRDAR UNIVERSTY COLLEGE OF SCIENCE DEPARTMENT :MATERIAL SCIENCE AND ENGINNERING PRESENTETON ON: ELLIPSOMETRY INSTRUMENT PREPEARED BY :ZELALEM GETU AMSALE.
Reproducibility Analysis of E-beam Deposited Multilayer Dielectric Reflective Filter Nancy Sharmaa , P Sunitaa, b, VSRS Praveen Kumara,b , Gaurav Dwivedia,
Determining the Index of Refraction of AlF3
List of materials which have been evaporated:
Standard Operation Procedure
Characterizing Multilayer Thin films
Possible mirror coatings for POLLUX
FIB, Ellipsometry, Interferometry...
DIFFUSION OF PEG-200 IN SKIN TISSUE
Behavior of Light.
FIB, Ellipsometry, Interferometry...
Radiation tolerant fibres for LHC controls and communications
Profile Extraction with Specular Spectroscopic Scatterometry
OL 750 Measurement Systems
Solar spectrum in space (thin line) and on Earth's surface (thick line). Solar spectrum in space (thin line) and on Earth's surface (thick line). Below.
OL 750 Spectroradiometer & Linear Spectral Transmission Measurements
Presentation transcript:

Angstrom Advanced Inc.. – 1056 Washington St., Canton, MA Tel. : Fax : Who we are: Angstrom Advanced is the leading supplier for ellipsometers. We offer full range of ellipsometers for thin film thickness measurement and optical characterization for refractive index and extinction coefficient (n & k). The Angstrom Advanced ellipsometer family includes discrete wavelength ellipsometers (single wavelength ellipsometers and multi-wavelength ellipsometers), deep UV, UV, VIS, NIR and IR spectroscopic ellipsometers. Our ellipsometers have been delivered to many renowned universities, research institutes and companies worldwide. Angstrom Advanced's goal is to supply the most accurate and repeatable ellipsometers with the highest standard of customer satisfaction. Many upgrade accessories are available for different applications. What we do: Angstrom Advanced Inc is one of the largest suppliers for ellipsometers in the world and we have the widest range of ellipsometers in the globe. We offers the ellipsometers, after-sales service, training and contract laboratory testing services.  PHE101 Discrete Wavelength Laser Ellipsometer  PHE101 Multi-Wavelength Ellipsometer  PHE102 UV/VIS NIR Spectroscopic Ellipsometer  PHE103 UV/VIS NIR Spectroscopic Ellipsometer  PHE104 Infrared Spectroscopic Ellipsometer Angstrom Advanced Inc.

Angstrom Advanced Inc.. – 1056 Washington St., Canton, MA Tel. : Fax : . PHE-101 Discrete Wavelength Ellipsometer Parameters :  Light Source: He-Ne  Wavelength: 632.8nm  Accuracy of film thickness: 0.005nm  Accuracy of Refractive index:  Measurement speed: Less 1 second  Incident angle : 20  to 90  , 5  /Step  Thickness range : 0-6,000nm Functions/Features :  Thin film’s thickness, refractive index and extinction coefficient, single or Multi-layer;  Second laser is used to make alignment most convenient and accuracy;  Economical cost.  Full material library;  Data and graph output function;  Based on windows XP operation system; Integrated data acquisition, analysis software;  Sample size up to 300mm;  wide applications, such as dielectrics, semiconductors, metal, organics and more;

Angstrom Advanced Inc.. – 1056 Washington St., Canton, MA Tel. : Fax : . PHE-101Multi-Wavelength Ellipsometer Parameters :  Light Source : He-Ne and semiconductor Lasers  Wavelength: 532, 632.8, 1064nm, …  Accuracy of film thickness: 0.005nm  Accuracy of refractive index:  Incident angle : 20  to 90  , 5  /Step  Repeatability : Psi=  0.01  , Delta=  0.02   Thickness range: 0-10,000nm Functions/Features:  Integrated data acquisition, analysis software ;  Thin film’s thickness, refractive index and extinction coefficient, single layer or multi-layer;  Second Laser is used to make alignment most convenient and accuracy;  Full material library, generate Psi and Delta with any sample structures;  Simulate experimental data and give fitting parameter values, confidence and correlation matrix;  Full Cauchy, EMA, Lorenz et. al. dispersion formula and a lot of database;  User can build own dispersion formula and database;  Data and graph output function.

Angstrom Advanced Inc.. – 1056 Washington St., Canton, MA Tel. : Fax : . PHE-102 UV/VIS NIR Spectroscopic Ellipsometer Functions/Features :  Film’s thickness, refractive index and extinction coefficient, single or multi-layer;  Powerful software with full materials library, Full Cauchy, EMA, Lorenz et. al. dispersion formula and a lot of database;  Transmittance and reflectance  Automated angle of incidence  (optional), Wafer Mapping & Motorized X-Y Sample stage, 3D graph display (optional); Parameters :  Wavelength: nm( nm), nm( nm);  Incident angle : 20  to 90  , 5  /Step;  Repeatability : Psi=  0.01  , Delta=  0.02  ;  Thickness range 0-30,000nm

Angstrom Advanced Inc.. – 1056 Washington St., Canton, MA Tel. : Fax : . PHE-103 UV/VIS, NIR Spectroscopic Ellipsometer Parameters :  Wavelength: nm( nm), nm ( nm);  Incident angle : 20  to 90  , automated 0.01  /Step;  Repeatability : Psi=  0.01  , Delta=  0.02  ;  Vertical Sample stage Functions/Features :  Film’s thickness, refractive index and extinction coefficient, single or multi-layer;  Powerful software with full materials library, Full Cauchy, EMA, Lorenz et. al. dispersion formula and a lot of database;  Transmittance and reflectance;  Automated angle of incidence  (optional), Wafer Mapping & Motorized X-Y Sample stage, 3D graph display (optional);

Angstrom Advanced Inc.. – 1056 Washington St., Canton, MA Tel. : Fax : . PHE-104 Infrared Spectroscopic Ellipsometer Functions/Features :  Film’s thickness, N & K measurement;  Resistivity measurements and doping profiles;  Identification of chemical bonds and buried layers investigation ;  Transmittance and reflectance; Parameters :  Wavelength: cm-1(2.5-25um)  Beam size: 1X34mm  Automated incident angle : 35  to 90  , 0.01  /Step