Laser-Induced Breakdown Spectroscopy Assisted by Machine Learning for Plastics/Polymers Identification
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Atomic and Molecular Laser-Induced Breakdown Spectroscopy of Selected Pharmaceuticals
Article Atomic and Molecular Laser-Induced Breakdown Spectroscopy of Selected Pharmaceuticals Pravin Kumar Tiwari 1,2, Nilesh Kumar Rai 3, Rohit Kumar 3, Christian G. Parigger 4 and Awadhesh Kumar Rai 2,* 1 Institute for Plasma Research, Gandhinagar, Gujarat-382428, India 2 Laser Spectroscopy Research Laboratory, Department of Physics, University of Allahabad, Prayagraj-211002, India 3 CMP Degree College, Department of Physics, University of Allahabad, Pragyagraj-211002, India 4 Physics and Astronomy Department, University of Tennessee, University of Tennessee Space Institute, Center for Laser Applications, 411 B.H. Goethert Parkway, Tullahoma, TN 37388-9700, USA * Correspondence: [email protected]; Tel.: +91-532-2460993 Received: 10 June 2019; Accepted: 10 July 2019; Published: 19 July 2019 Abstract: Laser-induced breakdown spectroscopy (LIBS) of pharmaceutical drugs that contain paracetamol was investigated in air and argon atmospheres. The characteristic neutral and ionic spectral lines of various elements and molecular signatures of CN violet and C2 Swan band systems were observed. The relative hardness of all drug samples was measured as well. Principal component analysis, a multivariate method, was applied in the data analysis for demarcation purposes of the drug samples. The CN violet and C2 Swan spectral radiances were investigated for evaluation of a possible correlation of the chemical and molecular structures of the pharmaceuticals. Complementary Raman and Fourier-transform-infrared spectroscopies were used to record the molecular spectra of the drug samples. The application of the above techniques for drug screening are important for the identification and mitigation of drugs that contain additives that may cause adverse side-effects. Keywords: paracetamol; laser-induced breakdown spectroscopy; cyanide; carbon swan bands; principal component analysis; Raman spectroscopy; Fourier-transform-infrared spectroscopy 1. -
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. -
Vacuum Ultra Violet Monochromator I Grating & OEM
Feature Article JY Division nformation Vacuum Ultra Violet Monochromator I Grating & OEM Erick Jourdain Abstract Taking the advantage of Jobin Yvon(JY) leading position in the design and realisation of diffraction grating JY has developed over the last past 30 years some of the most innovative Vacuum Ultra Violet (VUV) monochromators for synchrotron centre. These monochromators, which combine the ultimate advanced diffraction grating technologies and some ultra precise under vacuum mechanics, have been installed in several synchrotron centres and have demonstrated superior performances. Today the development of new compact VUV sources and applications require compact VUV monochromators. Based on diffraction grating capabilities and our large experience acquired in the difficult and demanding market of under vacuum synchrotron monochromators JY is currently developing new compact monochromators for application such as Extreme UV lithography or X-ray Photoemission Spectroscopy. Introduction In the middle of the seventies thank to the development of the aberration corrected holographic toroidal gratings at Jobin Yvon (JY) we introduced on the market a new VUV monochromator concept that drastically enhanced the spectroscopic performances in this field [1]. During the eighties the Toroidal Grating Monochromator (TGM) and its associated toroidal gratings had a large and world wide success. At that time most of the synchrotron VUV beamline got equipped with this monochromator type and even today some recent beamline are still been developed Fig. -
FT-IR Spectroscopy
ORIEL ORIEL PRODUCT TRAINING FT-IR Spectroscopy SECTION FOUR FEATURES • Glossary of Terms • Introduction to FT-IR Spectroscopy Stratford, CT • Toll Free 800.714.5393 Fax 203.378.2457 • www.newport.com/oriel • [email protected] GLOSSARY OF TERMS Before we start the technical discussion on FT-IR Spectrometers, we devote a couple of pages to a Glossary, to facilitate the discussion that follows. 100% Line: Calculated by ratioing two background spectra Collimation: The ideal input beam is a cylinder of light. No taken under identical conditions. Ideally, the result is a flat beam of finite dimensions can be perfectly collimated; at best line at 100% transmittance. there is a diffraction limit. In practice the input beam is a Absorbance: Units used to measure the amount of IR cone that is determined by the source size or aperture used. radiation absorbed by a sample. Absorbance is commonly The degree of collimation can affect the S/N and the used as the Y axis units in IR spectra. Absorbance is defined resolution. by Beer’s Law, and is linearly proportional to concentration. Constructive Interference: A phenomenon that occurs when Aliasing: If frequencies above the Nyquist Frequency are not two waves occupy the same space and are in phase with filtered out, energy in these will appear as spectral artefacts each other. Since the amplitudes of waves are additive, the below the Nyquist Frequency. Optical and electronic anti two waves will add together to give a resultant wave which is aliasing can be used to prevent this. Sometimes the higher more intense than either of the individual waves. -
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............................................................................................... -
Absorption Spectroscopy and Imaging from the Visible Through Mid-Infrared with 20 Nm Resolution
Absorption spectroscopy and imaging from the visible through mid-infrared with 20 nm resolution. Aaron M. Katzenmeyer,1 Glenn Holland,1 Kevin Kjoller2 and Andrea Centrone1* 1Center for Nanoscale Science and Technology, National Institute of Standards and Technology, 100 Bureau Drive, Gaithersburg, Maryland 20899, United States. *E-mail: [email protected] 2Anasys Instruments, Inc., 325 Chapala Street, Santa Barbara, California 93101, United States. Abstract Absorption spectroscopy and mapping from visible through mid-IR wavelengths has been achieved with spatial resolution exceeding the limit imposed by diffraction, via the photothermal induced resonance technique. Correlated vibrational (chemical), and electronic properties are obtained simultaneously with topography with a wavelength-independent resolution of ≈ 20 nm using a single laboratory-scale instrument. This marks the highest resolution reported for PTIR, as determined by comparing height and PTIR images, and its first extension to near-IR and visible wavelengths. Light-matter interaction enables scientists to characterize materials and biological samples across a large range of energies. Visible (VIS) and near-infrared (NIR) light (from 400 nm to 2.5 µm) probes electronic transitions in materials [1], providing information regarding band gap, defects, and energy transfer which is crucial for the semiconductor and optoelectronic industries and for understanding processes such as photosynthesis. Mid-infrared (mid-IR) light (from 2.5 µm to 15 µm) probes vibrational transitions and provides rich chemical and structural information enabling materials identification [2]. Spectral maps can be obtained by coupling a light source and a spectrometer with an optical microscope [3]. However, light diffraction limits the lateral resolution achievable with conventional microscopic techniques to approximately half the wavelength of light [4]. -
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. -
Nitrogen-15 Magnetic Resonance Spectroscopy, I
VOL. 51, 1964 CHEMISTRY: LAMBERT, BINSCH, AND ROBERTS 735 11 Felsenfeld, G., G. Sandeen, and P. von Hippel, these PROCEEDINGS, 50, 644 (1963). 12Bollum, F. J., J. Cell. Comp. Physiol., 62 (Suppi. 1), 61 (1963); Von Borstel, R. C., D. M. Prescott, and F. J. Bollum, J. Cell Biol., 19, 72A (1963). 13 Huang, R. C., and J. Bonner, these PROCEEDINGS, 48, 216 (1962); Allfrey, V. G., V. C. Littau, and A. E. Mirsky, these PROCEEDINGS, 49, 414 (1963). 14 Baxill, G. W., and J. St. L. Philpot, Biochim. Biophys. Acta, 76, 223 (1963). NITROGEN-15 MAGNETIC RESONANCE SPECTROSCOPY, I. CHEMICAL SHIFTS* BY JOSEPH B. LAMBERT, GERHARD BINSCH, AND JOHN D. ROBERTS GATES AND CRELLIN LABORATORIES OF CHEMISTRY, t CALIFORNIA INSTITUTE OF TECHNOLOGY Communicated March 23, 1964 Except for the original determination' of nuclear moments, nitrogen magnetic resonance spectroscopy has been limited to the isotope of mass number 14. Al- though N14 is an abundant isotope, it possesses an electric quadrupole moment, which seriously broadens the resonances of nitrogen in all but the most sym- metrical of environments.2 Consequently, nitrogen n.m.r. spectroscopy has seen only limited use in the determination of organic structure. It might be expected that N15, which has a spin of 1/2 and no quadrupole moment, would be very useful, but the low natural abundance (0.36%) and the inherently low signal intensity (1.04 X 10-3 that of H' at constant field) have thus far precluded utilization of N15 in n.m.r. spectroscopy'3 Resonance signals from N'5 have now been obtained from a series of N"5-enriched (30-99%) compounds with a Varian model 4300B spectrometer operated at 6.08 Mc/sec and 14,100 gauss. -
2. Molecular Stucture/Basic Spectroscopy the Electromagnetic Spectrum
2. Molecular stucture/Basic spectroscopy The electromagnetic spectrum Spectral region fooatocadr atomic and molecular spectroscopy E. Hecht (2nd Ed.) Optics, Addison-Wesley Publishing Company,1987 Per-Erik Bengtsson Spectral regions Mo lecu lar spec troscopy o ften dea ls w ith ra dia tion in the ultraviolet (UV), visible, and infrared (IR) spectltral reg ions. • The visible region is from 400 nm – 700 nm • The ultraviolet region is below 400 nm • The infrared region is above 700 nm. 400 nm 500 nm 600 nm 700 nm Spectroscopy: That part of science which uses emission and/or absorption of radiation to deduce atomic/molecular properties Per-Erik Bengtsson Some basics about spectroscopy E = Energy difference = c /c h = Planck's constant, 6.63 10-34 Js ergy nn = Frequency E hn = h/hc /l E = h = hc / c = Velocity of light, 3.0 108 m/s = Wavelength 0 Often the wave number, , is used to express energy. The unit is cm-1. = E / hc = 1/ Example The energy difference between two states in the OH-molecule is 35714 cm-1. Which wavelength is needed to excite the molecule? Answer = 1/ =35714 cm -1 = 1/ = 280 nm. Other ways of expressing this energy: E = hc/ = 656.5 10-19 J E / h = c/ = 9.7 1014 Hz Per-Erik Bengtsson Species in combustion Combustion involves a large number of species Atoms oxygen (O), hydrogen (H), etc. formed by dissociation at high temperatures Diatomic molecules nitrogen (N2), oxygen (O2) carbon monoxide (CO), hydrogen (H2) nitr icoxide (NO), hy droxy l (OH), CH, e tc. -
Absorption Spectroscopy
World Bank & Government of The Netherlands funded Training module # WQ - 34 Absorption Spectroscopy New Delhi, February 2000 CSMRS Building, 4th Floor, Olof Palme Marg, Hauz Khas, DHV Consultants BV & DELFT HYDRAULICS New Delhi – 11 00 16 India Tel: 68 61 681 / 84 Fax: (+ 91 11) 68 61 685 with E-Mail: [email protected] HALCROW, TAHAL, CES, ORG & JPS Table of contents Page 1 Module context 2 2 Module profile 3 3 Session plan 4 4 Overhead/flipchart master 5 5 Evaluation sheets 22 6 Handout 24 7 Additional handout 29 8 Main text 31 Hydrology Project Training Module File: “ 34 Absorption Spectroscopy.doc” Version 06/11/02 Page 1 1. Module context This module introduces the principles of absorption spectroscopy and its applications in chemical analyses. Other related modules are listed below. While designing a training course, the relationship between this module and the others, would be maintained by keeping them close together in the syllabus and place them in a logical sequence. The actual selection of the topics and the depth of training would, of course, depend on the training needs of the participants, i.e. their knowledge level and skills performance upon the start of the course. No. Module title Code Objectives 1. Basic chemistry concepts WQ - 02 • Convert units from one to another • Discuss the basic concepts of quantitative chemistry • Report analytical results with the correct number of significant digits. 2. Basic aquatic chemistry WQ - 24 • Understand equilibrium chemistry and concepts ionisation constants. • Understand basis of pH and buffers • Calculate different types of alkalinity. -
1. What Is the Difference Between Slit and Monochromator? a Slit Is A
1. What is the difference between slit and monochromator? A slit is a mechanical opening in a black painted metallic sheet, with a circular or triangular hole through which incident rays pass which lead to a monochromator. The slit permits passage of only a small fraction of incident radiation, which is selected for further processing such as wavelength selection and detection etc. Usually the output of the radiation is in the image of the slit. When the slit is wide relative to the wavelength, diffraction is difficult to observe. But when the wavelength and slit opening are of the same order of magnitude, diffraction is observed easily. Here the slit behaves as if it is a source of radiation. The output in this case occurs in a series of 1800 arcs. The plot of the frequency of the radiation as a function of peak transmittance is in the form of a Gaussian curve with maximum intensity being the midpoint of the frequency range. In contrast, monochromator may be defined as a device to select different wavelength of the original source radiation. Usually monochromators used in a UV-Visible/Fluorescence/AAS refer to the combination of slits, lenses, mirrors, windows, prisms and gratings. The output of monochromator is also a narrow band of continuous radiation. The band width is an inverse measure of the quality of the monochromator device. The band widths obtained from filters, prisms, gratings etc., become progressively narrower in each case. 2. Where is the monochromator being placed between source and sample or sample and detector in UV visible spectrophotometer? In a UV- Visible spectrophotometer, the monochromator is placed between the source of light and the sample. -
The Power of Crowding for the Origins of Life
Orig Life Evol Biosph (2014) 44:307–311 DOI 10.1007/s11084-014-9382-5 ORIGIN OF LIFE The Power of Crowding for the Origins of Life Helen Greenwood Hansma Received: 2 October 2014 /Accepted: 2 October 2014 / Published online: 14 January 2015 # Springer Science+Business Media Dordrecht 2015 Abstract Molecular crowding increases the likelihood that life as we know it would emerge. In confined spaces, diffusion distances are shorter, and chemical reactions produce fewer and more regular products. Crowding will occur in the spaces between Muscovite mica sheets, which has many advantages as a site for life’s origins. Keywords Muscovite mica . Molecular crowding . Origin of life . Mechanochemistry. Abiogenesis . Chemical confinement effects . Chirality. Protocells Cells are crowded. Protein molecules in cells are typically so close to each other that there is room for only one protein molecule between them (Phillips, Kondev et al. 2008). This is nothing like a dilute ‘prebiotic soup.’ Therefore, by analogy with living cells, the origins of life were probably also crowded. Molecular Confinement Effects Many chemical reactions are limited by the time needed for reactants to diffuse to each other. Shorter distances speed up these reactions. Molecular complementarity is another principle of life in which pairs or groups of molecules form specific interactions (Root-Bernstein 2012). Current examples are: enzymes & substrates & cofactors; nucleic acid base pairs; antigens & antibodies; nucleic acid - protein interactions. Molecular complementarity is likely to have been involved at life’s origins and also benefits from crowding. Mineral surfaces are a likely place for life’s origins and for formation of polymeric molecules (Orgel 1998).