Laser-Induced Breakdown Spectroscopy (LIBS) in Cultural Heritage Cite This: Anal
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Laser Raman Microprobing Techniques P
LASER RAMAN MICROPROBING TECHNIQUES P. Dhamelincourt, J. Barbillat, M. Delhaye To cite this version: P. Dhamelincourt, J. Barbillat, M. Delhaye. LASER RAMAN MICROPROBING TECHNIQUES. Journal de Physique Colloques, 1984, 45 (C2), pp.C2-249-C2-253. 10.1051/jphyscol:1984255. jpa- 00223968 HAL Id: jpa-00223968 https://hal.archives-ouvertes.fr/jpa-00223968 Submitted on 1 Jan 1984 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. JOURNAL DE PHYSIQUE Colloque C2, suppldment au n02, Tome 45, fdvrier 1984 page C2-249 LASER RAMAN MICROPROBING TECHNIQUES P. Dhamelincourt, J. Barbillat and M. Delhaye Laboratoire de Spectrochimie Infrarouge et Raman, C. N. R. S., lhziversitB des Sciences et Techniques de LiZZe, B&. C. 5, 59655 ViZZeneuve d 'Ascq Cedex, France @sun6 - L1int6r&t de la microspectrcm6trie Raman pour l'analyse mol6culaire non destructive ainsi que 1'6volution des techniques sont pr6sentBs. Quelques exem- ples d'application illustrent l'exps6. Abstract - The analytical potential of micr0Fm-w spectroscopy for non des- tructive mlecular analysis is presented. -
ADVANCED SPECTROMETER Introduction
ADVANCED SPECTROMETER Introduction In principle, a spectrometer is the simplest of scientific very sensitive detection and precise measurement, a real instruments. Bend a beam of light with a prism or diffraction spectrometer is a bit more complicated. As shown in Figure grating. If the beam is composed of more than one color of 1, a spectrometer consists of three basic components; a light, a spectrum is formed, since the various colors are collimator, a diffracting element, and a telescope. refracted or diffracted to different angles. Carefully measure The light to be analyzed enters the collimator through a the angle to which each color of light is bent. The result is a narrow slit positioned at the focal point of the collimator spectral "fingerprint," which carries a wealth of information lens. The light leaving the collimator is therefore a thin, about the substance from which the light emanates. parallel beam, which ensures that all the light from the slit In most cases, substances must be hot if they are to emit strikes the diffracting element at the same angle of inci- light. But a spectrometer can also be used to investigate cold dence. This is necessary if a sharp image is to be formed. substances. Pass white light, which contains all the colors of The diffracting element bends the beam of light. If the beam the visible spectrum, through a cool gas. The result is an is composed of many different colors, each color is dif- absorption spectrum. All the colors of the visible spectrum fracted to a different angle. are seen, except for certain colors that are absorbed by the gas. -
Electron Microprobe Analysis Course 12.141 Notes MIT Electron
Electron Microprobe Analysis Course 12.141 Notes Dr. Nilanjan Chatterjee The electron microprobe provides a complete micron-scale quantitative chemical analysis of inorganic solids. The method is nondestructive and utilizes characteristic x-rays excited by an electron beam incident on a flat surface of the sample. This course provides an introduction to the theory of x-ray microanalysis by wavelength and energy dispersive spectrometry (WDS and EDS), ZAF matrix correction procedures, and scanning electron imaging techniques using backscattered electron (BE), secondary electron (SE), x-ray (elemental mapping), and cathodoluminescence (CL) signals. Lab sessions involve hands- on use of the JEOL JXA-8200 Superprobe. MIT Electron Microprobe Facility Massachusetts Institute of Technology Department of Earth, Atmospheric & Planetary Sciences Room: 54-1221, Cambridge, MA 02139 Phone: (617) 253-1995; Fax: (617) 253-7102 e-mail: [email protected] web: http://web.mit.edu/e-probe/www/ Nilanjan ChatterjeeMIT, Cambridge, MA, USA October 2017 2 TABLE OF CONTENTS Page number 1. INTRODUCTION 3 2. ELECTRON SPECIMEN INTERACTIONS 5 2.1. ELASTIC SCATTERING 5 2.1.1. Electron backscattering 5 2.1.2. Electron interaction volume 6 2.2. INELASTIC SCATTERING 7 2.2.1. Secondary electron generation 7 2.2.2. Characteristic x-ray generation: inner-shell ionization 7 2.2.3. X-ray production volume 10 2.2.4. Bremsstrahlung or continuum x-ray generation 11 2.2.5. Cathodoluminescence 12 3. QUANTITATIVE X-RAY SPECTROMETRY 13 3.1. MATRIX CORRECTIONS 14 3.1.1. Atomic number correction (Z) 14 3.1.2. Absorption correction (A) 16 3.1.3. -
Spectrum 100 Series User's Guide
MOLECULAR SPECTROSCOPY SPECTRUM 100 SERIES User’s Guide 2 . Spectrum 100 Series User’s Guide Release History Part Number Release Publication Date L1050021 A October 2005 Any comments about the documentation for this product should be addressed to: User Assistance PerkinElmer Ltd Chalfont Road Seer Green Beaconsfield Bucks HP9 2FX United Kingdom Or emailed to: [email protected] Notices The information contained in this document is subject to change without notice. Except as specifically set forth in its terms and conditions of sale, PerkinElmer makes no warranty of any kind with regard to this document, including, but not limited to, the implied warranties of merchantability and fitness for a particular purpose. PerkinElmer shall not be liable for errors contained herein for incidental consequential damages in connection with furnishing, performance or use of this material. Copyright Information This document contains proprietary information that is protected by copyright. All rights are reserved. No part of this publication may be reproduced in any form whatsoever or translated into any language without the prior, written permission of PerkinElmer, Inc. Copyright © 2005 PerkinElmer, Inc. Trademarks Registered names, trademarks, etc. used in this document, even when not specifically marked as such, are protected by law. PerkinElmer is a registered trademark of PerkinElmer, Inc. Spectrum, Spectrum 100, and Spectrum 100N are trademarks of PerkinElmer, Inc. Spectrum 100 Series User’s Guide . 3 Contents Contents............................................................................................... -
Experiment 2 Radiation in the Visible Spectrum Emission Spectra Can Be
Experiment 2 Radiation in the Visible Spectrum Emission spectra can be a unique fingerprint of an atom or molecule. The photon energies and wavelengths are directly related to the allowed quantum energy states of the system. In the following experiments we will examine the radiation given off by sources radiating in the visible region. We will be using a spectrometer produced by Ocean Optics. Light enters the spectrometer via a fiber optic cable. Inside the spectrometer a diffraction grating diffracts the different frequencies onto a CCD. The CCD basically ”counts” the photons according to wavelength. The data is transferred via a usb port to a PC. The Ocean Optics software displays the spectrum as counts versus wavelength. We will examine the spectra given off by the following sources: incandescent light filament, hydrogen, helium, various light emitting diodes and a laser pointer. You will also be given an unknown gas discharge tube and will need to identify the gas via its spectral emissions Pre Lab 1) Obtain a spectrum for hydrogen, mercury, sodium and neon gas emissions. The spectrum must contain an accurate listing of major emission lines (in nm), not simply a color photo of the emission. 2) Make yourself familiar with the manual for the spectrometer and the software. These are available via the following links: http://www.oceanoptics.com/technical/hr4000.pdf http://www.oceanoptics.com/technical/SpectraSuite.pdf These documents are also available on Black Board. 3) How does the Ocean Optics spectrometer work? In your answer list its three main components and describe what each component does. -
Orbitrap Fusion Tribrid Mass Spectrometer
MASS SPECTROMETRY Product Specifications Thermo Scientific Orbitrap Fusion Tribrid Mass Spectrometer Unmatched analytical performance, revolutionary MS architecture The Thermo Scientific™ Orbitrap Fusion™ mass spectrometer combines the best of quadrupole, Orbitrap, and linear ion trap mass analysis in a revolutionary Thermo Scientific™ Tribrid™ architecture that delivers unprecedented depth of analysis. It enables life scientists working with even the most challenging samples—samples of low abundance, high complexity, or difficult-to-analyze chemical structure—to identify more compounds faster, quantify them more accurately, and elucidate molecular composition more thoroughly. • Tribrid architecture combines quadrupole, followed by ETD or EThCD for glycopeptide linear ion trap, and Orbitrap mass analyzers characterization or HCD followed by CID • Multiple fragmentation techniques—CID, for small-molecule structural analysis. HCD, and optional ETD and EThCD—are available at any stage of MSn, with The ultrahigh resolution of the Orbitrap mass subsequent mass analysis in either the ion analyzer increases certainty of analytical trap or Orbitrap mass analyzer results, enabling molecular-weight • Parallelization of MS and MSn acquisition determination for intact proteins and confident to maximize the amount of high-quality resolution of isobaric species. The unsurpassed data acquired scan rate and resolution of the system are • Next-generation ion sources and ion especially useful when dealing with complex optics increase system ease of operation and robustness and low-abundance samples in proteomics, • Innovative instrument control software metabolomics, glycomics, lipidomics, and makes setup easier, methods more similar applications. powerful, and operation more intuitive The intuitive user interface of the tune editor The Orbitrap Fusion Tribrid MS can perform and method editor makes instrument calibration a wide variety of analyses, from in-depth and method development easier. -
Mass Spectrometer
CLASSICAL CONCEPT REVIEW 6 Mass Spectrometer One of several devices currently used to measure the charge-to-mass ratio q m of charged atoms and molecules is the mass spectrometer. The mass spectrometer is used to find the charge-to-mass ratio of ions of known charge by measuring> the radius of their circular orbits in a uniform magnetic field. Equation 3-2 gives the radius of R for the circular orbit of a particle of mass m and charge q moving with speed u in a magnetic field B that is perpendicular to the velocity of the particle. Figure MS-1 shows a simple schematic drawing of a mass spectrometer. Ions from an ion source are accelerated by an electric field and enter a uniform magnetic field produced by an electromagnet. If the ions start from rest and move through a poten- tial DV, their kinetic energy when they enter the magnetic field equals their loss in potential energy, qDV: B out 1 mu2 = qDV MS-1 2 R The ions move in a semicircle of radius R given by Equation 3-2 and exit through a P P narrow aperture into an ion detector (or, in earlier times, a photographic plate) at point 1 u 2 P2, a distance 2R from the point where they enter the magnet. The speed u can be eliminated from Equations 3-2 and MS-1 to find q m in terms of DV, B, and R. The + + q result is Source > – + q 2DV ∆V = 2 2 MS-2 m B R MS-1 Schematic drawing of a mass spectrometer. -
Microprobe Operating Procedure
TWS-ESS-DP-07, R3 MICROPROBE OPERATING PROCEDURE Effective Date $1fj3 O/il ga" A*4,- Roland Hagan Date Preparer / /A Dad-, David Vaniman Technical Reviewer =AQ vc) Henry Paul Nunas Date Quality Assurane Project Leader TechnicaMrojeci Officer .B912190174 891211 -N !PDR WASTE WM-11 PDC TWS-ESS-DP-07, R3 Page 1 of 11 MICROPROBE OPERATING PROCEDURE 1.0 PURPOSE The purpose of this procedure is to allow an investigator to bring the Electron Microprobe from a standby condition to an analysis condition, perform one or more analyses, and when finished, return the system to a standby condition. 2.0 SCOPE This procedure describes the start-up, calibration, quantitative analysis and shut-down routines for the Electron Microprobe. Requirements for Los Alamos Yucca Mountain Project (LA YMP) analytical work are listed throughout this procedure. 3.0 APPLICABLE DOCUMENTS Documents referenced in this procedure are: Cameca Technical Manual, Option A-21 Tracor Northern Operators Manual, 1988 SANDIA TASKS: A Subroutined Electron Microprobe Automation system, Sandia Report 2037, 1985 CONFIG8 A Configuration File Generator for SANDIA TASKS, Sandia Report TWS-ESS-DP-06, 2035,1985 Operating Instructions For the Ladd Vacuum Evaporator For Carbon Coating TWS-ESS-DP. 122, Preparation of Electron Microprobe Standard Mounts TWS-ESS-DP-101, Procedure for Identification and Control for Mineralogy-Petrology TWS-QAS-QP-02.1, Los Alamos YMP Personnel Certification Procedure TWS-ESS-DP-125, Certification of Standards for Microanalysis TWS-QAS-QP.3.1, LANL, Yucca Mo ain Project Computer Software Control 4.0 RESPONSIBILrITES 4.1 It is the responsibility of the Operator to ascertain that all Electron Microprobe systems are operational before an Investigator begins a microanalysis session. -
Development and Applications of a Real-Time Magnetic Electron
Louisiana State University LSU Digital Commons LSU Doctoral Dissertations Graduate School 12-13-2017 Development and Applications of a Real-time Magnetic Electron Energy Spectrometer for Use with Medical Linear Accelerators Paul Ethan Maggi Louisiana State University and Agricultural and Mechanical College, [email protected] Follow this and additional works at: https://digitalcommons.lsu.edu/gradschool_dissertations Part of the Health and Medical Physics Commons Recommended Citation Maggi, Paul Ethan, "Development and Applications of a Real-time Magnetic Electron Energy Spectrometer for Use with Medical Linear Accelerators" (2017). LSU Doctoral Dissertations. 4180. https://digitalcommons.lsu.edu/gradschool_dissertations/4180 This Dissertation is brought to you for free and open access by the Graduate School at LSU Digital Commons. It has been accepted for inclusion in LSU Doctoral Dissertations by an authorized graduate school editor of LSU Digital Commons. For more information, please [email protected]. DEVELOPMENT AND APPLICATIONS OF A REAL-TIME MAGNETIC ELECTRON ENERGY SPECTROMETER FOR USE WITH MEDICAL LINEAR ACCELERATORS A Dissertation Submitted to the Graduate Faculty of the Louisiana State University and Agricultural and Mechanical College in partial fulfillment of the requirements for the degree of Doctor in Philosophy in The Department of Physics and Astronomy by Paul Ethan Maggi B.S., California Polytechnic State University, San Luis Obispo, 2012 May 2018 ACKNOWLEDGEMENTS I thank Kenneth Hogstrom for providing the initial idea for this project, as well as partial funding support. I thank Edison Liang of Rice University for providing the magnet block and measurements of the magnetic field. I thank my adviser, Kip Matthews for his advice, guidance, and patience during my tenure at LSU. -
Vernier Spectrometer Solution, Proceed Directly to the Calibrate Section Below
Select the Type of Data (or Units) You Want to Measure The default data type is absorbance. If you want to measure the absorbance of a Vernier Spectrometer solution, proceed directly to the Calibrate section below. (Order Code: V-SPEC) If you want to measure %T or intensity, do the following: 1. Choose Change Units ► Spectrometer from the Experiment menu. 2. Select the unit or data type you wish to measure. The Vernier Spectrometer is a portable visible light spectrometer. Calibrate (Not Required if Measuring Intensity) 1. To calibrate the Spectrometer, choose Calibrate ► Spectrometer from the What is Included with the Vernier Spectrometer? Experiment menu. Note: For best results, allow the Spectrometer to warm up for a Spectrometer (with light source/cuvette holder attached) minimum of five minutes. One package of 15 plastic cuvettes and lids 2. Fill a cuvette about ¾ full with distilled water (or the solvent being used in the USB cable experiment) to serve as the blank. After the Spectrometer has warmed up, place the blank cuvette in the Spectrometer. Align the cuvette so the clear side of the Software Requirements cuvette is facing the light source. Logger Pro® 3 (version 3.8.5 or newer) software is required if you are using a 3. Follow the instructions in the dialog box to complete the calibration, and then computer. LabQuest App version 2.0, or newer, is required if you are using click . LabQuest® 2. LabQuest App 1.1, or newer, is required if you are using the original LabQuest. Visit the downloads section of www.vernier.com to update your software. -
Real-Time Magnetic Electron Energy Spectrometer for Use with Medical Linear Accelerators P
ISBN 978-3-95450-180-9 Proceedings of NAPAC2016, Chicago, IL, USA TUPOA38 REAL-TIME MAGNETIC ELECTRON ENERGY SPECTROMETER FOR USE WITH MEDICAL LINEAR ACCELERATORS P. E. Maggi†, K. R. Hogstrom, K. L. Matthews II, Louisiana State University, Baton Rouge, LA 70803, USA R. L. Carver, Mary Bird Perkins Cancer Center, Baton Rouge, LA 70809, USA Abstract that there is a low-energy tail present in the spectrum [1] Accelerator characterization and quality assurance is an as a result of beam conditioning for therapeutic use. Addi- integral part of electron linear accelerator (linac) use in a tionally, measurements by Kok et al [4] have shown that medical setting. The current clinical method for radiation spectra for certain traveling-wave linacs (Elekta, Phillips) metrology of electron beams (dose on central axis versus can have further spectral deviations violating the Gaussi- depth in water) only provides a surrogate for the underly- an assumption; this is due to accelerator tuning parame- ing performance of the accelerator and does not provide ters (e.g. High Powered Phase Shifter) relating to the RF direct information about the electron energy spectrum. recycling system. A magnetic spectrometer has the poten- We have developed an easy to use real-time magnetic tial to simplify beam measurements, reduce the time electron energy spectrometer for characterizing the elec- needed for beam matching, and provides more infor- tron beams of medical linacs. Our spectrometer uses a mation about the electron beam. 0.57 T permanent magnet block as the dispersive element and scintillating fibers coupled to a CCD camera as the SPECTROMETER HARDWARE position sensitive detector. -
Angwcheminted, 2000, 39, 2587-2631.Pdf
REVIEWS Femtochemistry: Atomic-Scale Dynamics of the Chemical Bond Using Ultrafast Lasers (Nobel Lecture)** Ahmed H. Zewail* Over many millennia, humankind has biological changes. For molecular dy- condensed phases, as well as in bio- thought to explore phenomena on an namics, achieving this atomic-scale res- logical systems such as proteins and ever shorter time scale. In this race olution using ultrafast lasers as strobes DNA structures. It also offers new against time, femtosecond resolution is a triumph, just as X-ray and electron possibilities for the control of reactivity (1fs 10À15 s) is the ultimate achieve- diffraction, and, more recently, STM and for structural femtochemistry and ment for studies of the fundamental and NMR spectroscopy, provided that femtobiology. This anthology gives an dynamics of the chemical bond. Ob- resolution for static molecular struc- overview of the development of the servation of the very act that brings tures. On the femtosecond time scale, field from a personal perspective, en- about chemistryÐthe making and matter wave packets (particle-type) compassing our research at Caltech breaking of bonds on their actual time can be created and their coherent and focusing on the evolution of tech- and length scalesÐis the wellspring of evolution as a single-molecule trajec- niques, concepts, and new discoveries. the field of femtochemistry, which is tory can be observed. The field began the study of molecular motions in the with simple systems of a few atoms and Keywords: femtobiology ´ femto- hitherto unobserved ephemeral transi- has reached the realm of the very chemistry ´ Nobel lecture ´ physical tion states of physical, chemical, and complex in isolated, mesoscopic, and chemistry ´ transition states 1.