ADVANCED SPECTROMETER Introduction
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Design and Testing of Collimators for Use in Measuring X-Ray Attenuation
DESIGN AND TESTING OF COLLIMATORS FOR USE IN MEASURING X-RAY ATTENUATION By RAJESH PANTHI Master of Science (M.Sc.) in Physics Tribhuvan University Kathmandu, Nepal 2009 Submitted to the Faculty of the Graduate College of the Oklahoma State University in partial fulfillment of the requirements for the Degree of MASTER OF SCIENCE December, 2017 DESIGN AND TESTING OF COLLIMATORS FOR USE IN MEASURING X-RAY ATTENUATION Thesis Approved: Dr. Eric R. Benton Thesis Adviser and Chair Dr. Eduardo G. Yukihara Dr. Mario F. Borunda ii ACKNOWLEDGEMENTS I would like to express the deepest appreciation to my thesis adviser As- sociate Professor Dr. Eric Benton of the Department of Physics at Oklahoma State University for his vigorous guidance and help in the completion of this work. He provided me all the academic resources, an excellent lab environment, financial as- sistantship, and all the lab equipment and materials that I needed for this project. I am grateful for many skills and knowledge that I gained from his classes and personal discussion with him. I would like to thank Adjunct Profesor Dr. Art Lucas of the Department of Physics at Oklahoma State University for guiding me with his wonderful experience on the Radiation Physics. My sincere thank goes to the members of my thesis committee: Professor Dr. Eduardo G. Yukihara and Assistant Professor Dr. Mario Borunda of the Department of Physics at Oklahoma State University for generously offering their valuable time and support throughout the preparation and review of this document. I would like to thank my colleague Mr. Jonathan Monson for helping me to access the Linear Accelerators (Linacs) in St. -
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. -
Lhc Collimator Alignment Operational Tool∗
TUPPC120 Proceedings of ICALEPCS2013, San Francisco, CA, USA LHC COLLIMATOR ALIGNMENT OPERATIONAL TOOL∗ G. Valentinoy , CERN, Geneva, Switzerland and University of Malta, Msida, Malta R. W. Aßmannz , S. Redaelli, CERN, Geneva, Switzerland N. Sammut, University of Malta, Msida, Malta Abstract tor tanks housing the jaws and other equipment such as Beam-based LHC collimator alignment is necessary to quadrupole magnets and Beam Position Monitors (BPMs). determine the beam centers and beam sizes at the colli- The actual beam orbit may deviate from the design orbit mator locations for various machine configurations. Fast over several months of operation due to ground motion and and automatic alignment is provided through an opera- thermal effects [4]. Hence, all collimators are periodically tional tool has been developed for use in the CERN Con- aligned to the beam to determine these parameters. A jaw trol Center, which is described in this paper. The tool is is aligned when a sharp increase followed by a slow expo- implemented as a Java application, and acquires beam loss nential decrease appears in the signal read out from a Beam and collimator position data from the hardware through a Loss Monitoring (BLM) detector [5] placed downstream of middleware layer. The user interface is designed to allow the collimator. for a quick transition from application start up, to select- ing the required collimators for alignment and configuring OPERATIONAL TOOL the alignment parameters. The measured beam centers and Main Display sizes are then logged and displayed in different forms to A screenshot of the main display of the collimator appli- help the user set up the system. -
Evaluation of Infrared Collimators for Testing Thermal Imaging Systems
OPTO-ELECTRONICS REVIEW 15(2), 82–87 DOI: 10.2478/s11772-007-0005-9 Evaluation of infrared collimators for testing thermal imaging systems K. CHRZANOWSKI*1,2 1Institute of Optoelectronics, Military University of Technology, 2 Kaliskiego Str., 00-908 Warsaw, Poland 2INFRAMET, 24 Graniczna Str., Kwirynów, 05-082 Stare Babice, Poland Infrared reflective collimators are important components of expensive sophisticated test systems used for testing thermal imagers. Too low quality collimators can become a source of significant measurement errors and collimators of too high quality can unnecessarily increase cost of a test system. In such a situation it is important for test system users to know proper requirements on the collimator and to be able to verify its performance. A method for evaluation of infrared reflective collimators used in test systems for testing thermal imagers is presented in this paper. The method requires only easily avail- able optical equipment and can be used not only by collimator manufactures but also by users of test equipment to verify per- formance of the collimators used for testing thermal imagers. Keywords: IR systems, testing thermal imaging systems, IR optical design. 1. Introduction requirement that the collimator spatial resolution should match the spatial resolution capabilities of the tested thermal IR collimators are typical elements of laboratory sets-up used imager. for testing thermal imaging systems. Reflective two-mirror Although IR collimators are frequently used for testing collimators built using an off-axis parabolic collimating mir- thermal imagers since the 1970s, there has been little interest ror and smaller directional flat mirror represent a typical de- in a problem of evaluation of these optical systems. -
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. -
Super-Collimation in a Rod-Based Photonic Crystal by Ta-Ming Shih B.S
Super-collimation in a Rod-based Photonic Crystal by Ta-Ming Shih B.S. Electrical Engineering and Computer Science University of California, Berkeley 2006 Submitted to the Department of Electrical Engineering and Computer Science in partial ful¯llment of the requirements for the degree of Master of Science in Electrical Engineering at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY September 2007 °c Massachusetts Institute of Technology 2007. All rights reserved. Author.............................................................. Ta-Ming Shih Department of Electrical Engineering and Computer Science August 20, 2007 Certi¯ed by. Leslie A. Kolodziejski Professor of Electrical Engineering and Computer Science Thesis Supervisor Accepted by . Arthur C. Smith Chair, Department Committee on Graduate Students 2 Super-collimation in a Rod-based Photonic Crystal by Ta-Ming Shih Submitted to the Department of Electrical Engineering and Computer Science on August 20, 2007, in partial ful¯llment of the requirements for the degree of Master of Science in Electrical Engineering Abstract Super-collimation is the propagation of a light beam without spreading that occurs when the light beam is guided by the dispersion properties of a photonic crystal, rather than by defects in the photonic crystal. Super-collimation has many potential applications, the most straight-forward of which is in the area of integrated optical circuits, where super-collimation can be utilized for optical routing and optical logic. Another interesting direction is the burgeoning ¯eld of optofluidics, in which inte- grated biological or chemical sensors can be based on super-collimating structures. The work presented in the thesis includes the design, fabrication, and characteriza- tion of a rod-based two-dimensional photonic crystal super-collimator. -
Novel Fiber Fused Lens for Advanced Optical Communication Systems Andrew A
Novel Fiber Fused Lens for Advanced Optical Communication Systems Andrew A. Chesworth*a, Randy K. Rannow b, Omar Ruiz a, Matt DeRemer a, Joseph Leite a, Armando Martinez b, Dustin Guenther b aLightPath Technology, 2603 Challenger Tech Ct., Orlando, FL, 32826, USA bAPIC Corporation, 5800 Uplander Way, Los Angeles, CA, 90230, USA ABSTRACT We report on a novel fused collimator design as part of a transmitter optical sub-assembly (TOSA) used for agile microwave photonic links. The fused collimator consists of a PM fiber that is laser fused to a C type lens. The fusion joint provides a low loss interface between the two components and eliminates the need for separate components in the optical path. The design simplifies the number of components with the optical assembly leading to several advantages over traditional designs. In this paper we use the fiber coupling efficiency as a design metric and discuss the opt- mechanical tolerances and its effect on the overall design parameters. Keywords: Fiber Collimators, Fiber Coupling, RF Photonic Links, TOSA 1. INTRODUCTION Recent advances in the development of high power 1550nm semiconductor lasers for agile microwave photonic links have created a demand for high performance, reliable and robust beam delivery optics. In this paper we describe a transmitter optical sub-assembly (TOSA) based on a novel collimator design. The basic elements of the TOSA are the laser source, precision molded asphere, isolator, focusing lens and PM fiber. Traditionally, the focusing lens and fiber are discrete elements. In this application, the focusing lens and optical fiber are fused together to produce a single element referred to as a collimator (although in this application it’s used as a coupler). -
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.