Time-Resolved Resonance Raman Spectroscopy: Exploring Reactive Intermediates
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On the Photoionization of Large Molecules
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector ________ ~~__ On the Photoionization of Large Molecules C. H. Becker and K. J. Wu* Molecular Phvxics L‘tbordtorv, SRI Irlternatmnal, Menlo Park. ialifornia, USA There is no apparent limit to the size of a molecule for which photoionization can occur. It is argued that it is difficult to obtain useful photoionization mass spectra of peptides (above - 2000 u), proteins, and oligonucleotides, because of the high internal energy of these polar molecules as a result of the desorption event and because vibrationally excited radical cations readily fragment. Evidence to support this hypothesis is presented from the 1%nm single-photon ionization 61’1) mass spectra of the cyclic decapeptide gramicidin S and of fullerencs, from null SPI results with the linear peptides substance P and gramicidin D and oligonucleotides, and from a variety of data found in the literature. The literature data include mass spectra from jet-cooled peptides, perfluorinated polyethers, collisional ioniza- tion of small neutral peptides, and the ultraviolet photoelectron spectroscopy of polymeric solids. (1 Am Sot Mass Spcctrom 1995, 6, 883-888) uch recent effort in mass spectrometry has (MALD), peptides and proteins show significant de- been directed toward the analysis of peptides grees of metastable decay that increases with the mass M and proteins [l, 21, DNA [3, 41, and other of the molecule [ll]. Even for the MALD technique, large biopolymers. Successful analytical approaches to considered currently to be the “gentlest” of all stimu- date have used the direct ionization associated with lated desorption techniques in that it permits observa- the desorption process, especially with laser desorp- tion of the quasimolecular ions of large proteins and tion. -
Donor-Acceptor Interaction and Photochemistry of Polymethylene-Linked Bichromophores in Solution
9042 J. Am. Chem. Soc. 1996, 118, 9042-9051 Donor-Acceptor Interaction and Photochemistry of Polymethylene-Linked Bichromophores in Solution Song-lei Zhang, Matthew J. Lang, Steven Goodman,† Christopher Durnell, Vlastimil Fidlar,‡ Graham R. Fleming, and Nien-chu C. Yang* Contribution from the Department of Chemistry, UniVersity of Chicago, Chicago, Illinois 60637 ReceiVed July 17, 1996X Abstract: The ground-state and the excited-state spectroscopic properties of four series of polymethylene-linked anthracene-dialkylaniline bichromophores were compared as a probe to the relationship between energetics and distance in photoinduced electron transfer (PET). The results demonstrate that, when the energy level of the charge- transfer (CT) state is lowered below that of the localized excited state by appropriate substituents, there is a strong electron-donor-acceptor (EDA) interaction in the ground state which is absent in other bichromophores. Absorption and fluorescence excitation studies revealed that there is an unusually strong EDA interaction in the ground state of A-2 which is absent in other members in the A series. When A-2 is excited directly into this EDA absorption, it exhibits two CT emissions, one at 490 nm and the other at 605 nm. The quantum yield (τf) and the lifetime (Φf) of the two emissions are dependent on the viscosity of the alkane solvent. The Φf and the τf of the 490 nm emission increased when the solvent viscosity was increased; however, those of the 605 nm emission remained essentially unchanged. The risetime of the 605 nm emission is 420 ps, but that of the 490 nm emission is instrument-function limiting. -
Improved Treatment of the Photoionization Process in the Laser Induced Optical Breakdown in the Laser Tissue
U.P.B. Sci. Bull., Series A, Vol. 81, Iss. 4, 2019 ISSN 1223-7027 IMPROVED TREATMENT OF THE PHOTOIONIZATION PROCESS IN THE LASER INDUCED OPTICAL BREAKDOWN IN THE LASER TISSUE Violeta PETROVIĆ1 and Hristina DELIBAŠIĆ1 The development of laser technology led to the discovery that laser-living tissue (cells) interactions have significant biomedical applications and can be used to perform precise surgical procedures of 'water-like' tissues (such as the eye). When the focus is located within transparent biological cells and tissues, nonlinear absorption processes initiate a laser induced optical breakdown. The threshold for breakdown is defined by a certain critical free electron density. An in depth understanding of these processes orientated our theoretical research to the development of rate equations describing electron density growth in a transparent biological media exposed to a femtosecond laser pulse. In order to provide an accurate theoretical model and to predict damage occurrence, we took into account the losses through diffusion of electrons out of the focal volume, cascade ionization and the model of photoionization based on the standard Keldysh and ADK theory. Keywords: laser-induced breakdown, avalanche process, Keldysh theory. 1. Introduction The advent of high-power lasers opened the door for a wide range of laser application [1, 2, 3]. The effect known as the breakdown is a very important topic due to its role in laser applications. Breakdown is an effect which can be produced by high electric field strengths. This means that after a spark the medium becomes electrically conducting. Laser-induced breakdown (LIB) can occur in any media: solid, liquid, or gas. -
Assessment of Portable HAZMAT Sensors for First Responders
The author(s) shown below used Federal funds provided by the U.S. Department of Justice and prepared the following final report: Document Title: Assessment of Portable HAZMAT Sensors for First Responders Author(s): Chad Huffman, Ph.D., Lars Ericson, Ph.D. Document No.: 246708 Date Received: May 2014 Award Number: 2010-IJ-CX-K024 This report has not been published by the U.S. Department of Justice. To provide better customer service, NCJRS has made this Federally- funded grant report available electronically. Opinions or points of view expressed are those of the author(s) and do not necessarily reflect the official position or policies of the U.S. Department of Justice. Assessment of Portable HAZMAT Sensors for First Responders DOJ Office of Justice Programs National Institute of Justice Sensor, Surveillance, and Biometric Technologies (SSBT) Center of Excellence (CoE) March 1, 2012 Submitted by ManTech Advanced Systems International 1000 Technology Drive, Suite 3310 Fairmont, West Virginia 26554 Telephone: (304) 368-4120 Fax: (304) 366-8096 Dr. Chad Huffman, Senior Scientist Dr. Lars Ericson, Director UNCLASSIFIED This project was supported by Award No. 2010-IJ-CX-K024, awarded by the National Institute of Justice, Office of Justice Programs, U.S. Department of Justice. The opinions, findings, and conclusions or recommendations expressed in this publication are those of the author(s) and do not necessarily reflect those of the Department of Justice. This document is a research report submitted to the U.S. Department of Justice. This report has not been published by the Department. Opinions or points of view expressed are those of the author(s) and do not necessarily reflect the official position or policies of the U.S. -
C-2 Ch 2 & 3 Atoms & Molecules
Molecular and Supramolecular Photochemistry Modern Molecular Photochemistry of Organic Molecules Or Principles of Photochemistry N. J. Turro, V. Ramamurthy and J. C. Scaiano Chapters 1 & 2 Photochemistry Interaction of Light with Matter (Molecules) • Organic Photochemistry • Inorganic Photochemistry • Photobiology What is the difference between thermochemistry and photochemistry? • Mode of activation • Activated by collisions (thermo) • Activated by light (photo) • Selectivity in activation • Entire molecule gets activated • Only the chromophore that absorbs the light gets activated • Energy distribution • Energy used for vibrational/rotational transition • Energy used for electronic transition only Visualization of Thermal Reactions • Transition state connects a single reactant to a single product (intermediate) and it is a saddle point along the reaction course. • Collisions are a reservoir of continuous energy (~ 0.6 kcal/mol per impact). • Collisions can add or remove energy from a system. • Concerned with a single surface. Visualization of Photochemical Reactions We need to deal with two surfaces (ground and excited state. Adiabatic Diabatic Photochemistry starts with interaction of a Photon with a Molecule • What is a photon? • What is a molecule? • How do they interact? • What are the consequences of interaction? The Basic Laws of Photochemistry Grotthuss-Draper law The First Law of Photochemistry: light must be absorbed for photochemistry to occur. Grotthus Drapper Stark-Einstein law The Second Law of Photochemistry: for each photon of light absorbed by a chemical system, only one molecule is activated for a photochemical Stark Einstein reaction. The Light Paradigm (500 BC-1850 AD) 500 2018 BC AD 55 BC 1000 1500 1700 Lucretius Newton (1643-1727) Maxwell (1831-1879) Particles! Waves! …but then came the 1900s - new people, tools, and paradigms! Paradigm 1800s: Light consists of waves (energy propagated by waves): Energy is spread over space like a liquid. -
An Overview of Snow Photochemistry: Evidence, Mechanisms and Impacts
Atmos. Chem. Phys., 7, 4329–4373, 2007 www.atmos-chem-phys.net/7/4329/2007/ Atmospheric © Author(s) 2007. This work is licensed Chemistry under a Creative Commons License. and Physics An overview of snow photochemistry: evidence, mechanisms and impacts A. M. Grannas1, A. E. Jones2, J. Dibb3, M. Ammann4, C. Anastasio5, H. J. Beine6, M. Bergin7, J. Bottenheim8, C. S. Boxe9, G. Carver10, G. Chen11, J. H. Crawford11, F. Domine´12, M. M. Frey12,13, M. I. Guzman´ 9,14, D. E. Heard15, D. Helmig16, M. R. Hoffmann9, R. E. Honrath17, L. G. Huey18, M. Hutterli2, H. W. Jacobi19, P. Klan´ 20, B. Lefer29, J. McConnell21, J. Plane15, R. Sander22, J. Savarino12, P. B. Shepson23, W. R. Simpson24, J. R. Sodeau25, R. von Glasow26, 27, R. Weller19, E. W. Wolff2, and T. Zhu28 1Department of Chemistry, Villanova University, Villanova, PA 19085, USA 2British Antarctic Survey, Natural Environment Research Council, Cambridge, CB3 0ET, UK 3Institute for the Study of Earth, Oceans and Space, University of New Hampshire, Durham, NH 03824, USA 4Laboratory for Radio- and Environmental Chemistry, Paul Scherrer Institute, 5232 Villigen, Switzerland 5Department of Land, Air & Water Resources, University of California at Davis, Davis, CA 95616, USA 6Consiglio Nazionale delle Ricerche – Istituto Inquinamento Atmosferico (C.N.R. – I.I.A); Via Salaria Km 29,3; 00016 Monterotondo Scalo, Roma, Italy 7School of Civil and Environmental Engineering and School of Earth and Atmospheric Sciences, Georgia Institute of Technology, Atlanta, GA 30332, USA 8Air Quality Research Branch, -
Glossary of Terms Used in Photochemistry, 3Rd Edition (IUPAC
Pure Appl. Chem., Vol. 79, No. 3, pp. 293–465, 2007. doi:10.1351/pac200779030293 © 2007 IUPAC INTERNATIONAL UNION OF PURE AND APPLIED CHEMISTRY ORGANIC AND BIOMOLECULAR CHEMISTRY DIVISION* SUBCOMMITTEE ON PHOTOCHEMISTRY GLOSSARY OF TERMS USED IN PHOTOCHEMISTRY 3rd EDITION (IUPAC Recommendations 2006) Prepared for publication by S. E. BRASLAVSKY‡ Max-Planck-Institut für Bioanorganische Chemie, Postfach 10 13 65, 45413 Mülheim an der Ruhr, Germany *Membership of the Organic and Biomolecular Chemistry Division Committee during the preparation of this re- port (2003–2006) was as follows: President: T. T. Tidwell (1998–2003), M. Isobe (2002–2005); Vice President: D. StC. Black (1996–2003), V. T. Ivanov (1996–2005); Secretary: G. M. Blackburn (2002–2005); Past President: T. Norin (1996–2003), T. T. Tidwell (1998–2005) (initial date indicates first time elected as Division member). The list of the other Division members can be found in <http://www.iupac.org/divisions/III/members.html>. Membership of the Subcommittee on Photochemistry (2003–2005) was as follows: S. E. Braslavsky (Germany, Chairperson), A. U. Acuña (Spain), T. D. Z. Atvars (Brazil), C. Bohne (Canada), R. Bonneau (France), A. M. Braun (Germany), A. Chibisov (Russia), K. Ghiggino (Australia), A. Kutateladze (USA), H. Lemmetyinen (Finland), M. Litter (Argentina), H. Miyasaka (Japan), M. Olivucci (Italy), D. Phillips (UK), R. O. Rahn (USA), E. San Román (Argentina), N. Serpone (Canada), M. Terazima (Japan). Contributors to the 3rd edition were: A. U. Acuña, W. Adam, F. Amat, D. Armesto, T. D. Z. Atvars, A. Bard, E. Bill, L. O. Björn, C. Bohne, J. Bolton, R. Bonneau, H. -
Direct Measurement of Electron Numbers Created at Near-Infrared Laser-Induced Ionization of Various Gases
Direct Measurement of Electron Numbers Created at Near-Infrared Laser-Induced Ionization of Various Gases A. Sharma1, M. N. Slipchenko1, K. A. Rahman1, M. N. Shneider2, and A. Shashurin1 1 Purdue University, West Lafayette, IN, USA 2 Princeton University, Princeton, NJ, USA Abstract In this work, we present temporally resolved measurements of electron numbers created at photoionization of various gases by femtosecond laser pulse at 800 nm wavelength. The experiments were conducted in O2, Xe, Ar, N2, Kr and CO at room temperature and atmospheric pressure. Elastic microwave scattering was used to directly measure the electron numbers. Numbers of electrons in the range 3108 to 31012 electrons were produced by the laser pulse energies 100-700 J. After the laser pulse, plasma decayed on the time scale varied from 1 to 40 ns depending on the gas type and governed by two competing processes, namely, the creation of new electrons from ionization of the metastable atoms and loss of the electrons due to dissociative recombination and attachment to oxygen. Introduction Broad research history of the laser-induced plasmas is related to studies of various nonlinear effects at laser beam propagation such as laser pulse filamentation, laser beam collapse, self-trapping, dispersion, modulation instability, pulse splitting etc.1,2,3,4,5 These effects are various manifestations of the combined action of focusing Kerr nonlinearity (optical Kerr effect) and defocusing nonlinearity due to plasmas. Nowadays laser-induced plasmas find very wide application for plasma-assisted combustion, combustion diagnostics, laser-induced breakdown spectroscopy etc. 5 Conventional techniques for diagnostics of laser-induced plasmas pose detrimental 16 17 - limitations. -
Photochemistry
Photochemistry 1.1 Introduction:- Photochemistry is concerned with reactions which are initiated by electronically excited molecules. Such molecules are produced by the absorption of suitable radiation in the visible and near ultraviolet region of the spectrum. Photochemistry is basic to the world we live in with sun as the central figure, the origin of life must have been a photochemical act. Simple gaseous molecules like methane, ammonia and carbon dioxide must have reacted photochemically to synthesize complex organic molecules like proteins and nucleic acids. Photobiology, the photochemistry of biological reactions, is a rapidly developing subject and helps in understanding the phenomenon of photosynthesis, phototaxin, photoperiodism, vision and mutagenic effects of light. The relevance of photochemistry also lies in its varied applications in science and technology. Synthetic organic photochemistry has provided methods for the manufacture of many chemicals which could not be produced by dark reactions. Some industrially viable photochemical syntheses include synthesis of vitamin D2 from ergosterol isolated from yeast, synthesis of caprolactum which is the monomer for Nylon 6, manufacture of cleaning solvents and synthesis of some antioxidants. Photoinitiated polymerization and photopolymerisation are used in photography, lithoprinting and manufacture of printed circuits for the electronic industry. The photophysical phenomena of flourescence and phosphorescence have found varied applications in fluorescent tube lights, TV screens, as luminescent dials for watches, as “optical brighteners” in white dress materials, as paints in advertisement hoardings and so on. Another revolutionary application of electronically excited molecular systems is laser technology. The two main processes, therefore, studied under photochemistry are: 1. Photophysical process 2. Photochemical process 1. -
Photoionization
DLJSRF/R 1 fh ~ · DARESBURY SYNCHROTRON RADIATION LECTURE NOTE SERIES No.1 PHOTOIONIZATION by C. Bottcher Science Research Council DARESBURY LABORATORY Daresbury, Warrington, WA4 4AD DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency Thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof. DISCLAIMER Portions of this document may be illegible in electronic image products. Images are produced from the best available original document. © SCIENCE RESEARCH COUNCIL 1974 Enquiries about copyright and reproduction should be addressed to : The Librarian, Daresbury Laboratory, Daresbury, Warrington, WA44AD. IMPORTANT The SRC does not accept any responsibility for loss or damage arising from the use of information contained in any of its reports or in any communication about its tests or investigations. Printed by McCorquodale Printers Ltd., NAwton-IA-Willow,;. M ersey side. DARESBURY SYNCHROTRON RADIATION LECTURE NOTE SERIES No.1 PHOTOIONIZATION C. Bottcher Department of Theoretical Physics University of Manchester Notes on a series of lectures given at Daresbury Laboratory, November 1973 Science Research Council DARESBURY LABORATORY 1974 iWASlER FOREWORD These lectures were given in November 1973 to experimental physicists using the Synchrotron Radiation Facility at Daresbury. -
Spectroscopy and Photochemistry of Astrophysically-Relevant Molecules of the Cyanoactylene Family Urszula Szczepaniak
Spectroscopy and photochemistry of astrophysically-relevant molecules of the cyanoactylene family Urszula Szczepaniak To cite this version: Urszula Szczepaniak. Spectroscopy and photochemistry of astrophysically-relevant molecules of the cyanoactylene family. Chemical Physics [physics.chem-ph]. Université Paris Saclay (COmUE); Insty- tut chemii fizycznej (Pologne), 2017. English. NNT : 2017SACLS128. tel-01562041 HAL Id: tel-01562041 https://tel.archives-ouvertes.fr/tel-01562041 Submitted on 13 Jul 2017 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. NNT: 2017SACLXXXX Urszula Szczepaniak PhD Thesis Spectroscopy and photochemistry of astrophysically-relevant molecules of the cyanoacetylene family Supervisor: Prof. dr hab. Robert Kołos Co-Supervisor: Dr hab. Claudine Crépin-Gilbert, Directrice de Recherches au CNRS This work was prepared in the frame of joint Polish-French programme cotutelle: at International Doctoral Studies at the Institute of Physical Chemistry, Polish Academy of Sciences, ul. Kasprzaka 44/52, 01-224 Warsaw, POLAND and at Université Paris Saclay, Université Paris Sud - Paris XI, ÉCOLE DOCTORALE No 572: Ondes et Matière, DISCIPLINE: Physique; Institut des Sciences Moléculaires d'Orsay, Bat. 210, Domaine de l'Université de Paris Sud, 91400 Orsay FRANCE. Doctoral committee: Prof. dr hab. -
Photoionization of Kcs Molecule: Origin of the Structured Continuum?
atoms Article Photoionization of KCs Molecule: Origin of the Structured Continuum? Goran Pichler 1,*, Robert Beuc 1, Jahja Kokaj 2, David Sarkisyan 3, Nimmy Jose 2 and Joseph Mathew 2 1 Institute of Physics, 10000 Zagreb, Croatia; [email protected] 2 Department of Physics, Kuwait University, P.O. Box 5969, Safat 13060, Kuwait; [email protected] (J.K.); [email protected] (N.J.); [email protected] (J.M.) 3 Institute for Physical Research, Armenian Academy of Science, Ashtarak 0203, Armenia; [email protected] * Correspondence: [email protected]; Tel.: +385-91-469-8826 Received: 30 April 2020; Accepted: 26 May 2020; Published: 28 May 2020 Abstract: We report the experimental observation of photoionization bands of the KCs molecule in the deep ultraviolet spectral region between 200 and 420 nm. We discuss the origin of observed photoionization bands as stemming from the absorption from the ground state of the KCs molecule to the excited states of KCs+ molecule for which we used existing potential curves of the KCs+ molecule. An alternative explanation relies on the absorption from the ground state of the KCs molecule to the doubly excited states of the KCs** molecule, situated above the lowest molecular state of KCs+. The relevant potential curves of KCs** are not known yet, but all those KCs** potential curves are certainly autoionizing. However, these two photoionization pathways may interfere resulting in a special interference structured continuum, which is observed as complex bands. Keywords: photoionization; alkali molecule; autoionization of molecule; heteronuclear molecule 1. Introduction High-temperature alkali mixtures possessing high densities of constituents enable observation of the characteristic bands of mixed alkali molecules [1].