From Interstellar Polycyclic Aromatic Hydrocarbons and Ice to Astrobiology
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Theoretical Electron Affinities of Pahs and Electronic Absorption Spectra Of
A&A 432, 585–594 (2005) Astronomy DOI: 10.1051/0004-6361:20042246 & c ESO 2005 Astrophysics Theoretical electron affinities of PAHs and electronic absorption spectra of their mono-anions G. Malloci1,2,G.Mulas1, G. Cappellini2,3, V. Fiorentini2,3, and I. Porceddu1 1 INAF - Osservatorio Astronomico di Cagliari – Astrochemistry Group, Strada n. 54, Loc. Poggio dei Pini, 09012 Capoterra (CA), Italy e-mail: [gmalloci;gmulas;iporcedd]@ca.astro.it 2 Dipartimento di Fisica, Università degli Studi di Cagliari, Complesso Universitario di Monserrato, S. P. Monserrato-Sestu Km 0,700, 09042 Monserrato (CA), Italy e-mail: [giancarlo.cappellini;vincenzo.fiorentini]@dsf.unica.it 3 INFM - Sardinian Laboratory for Computational Materials Science (SLACS) Received 25 October 2004 / Accepted 8 November 2004 Abstract. We present theoretical electron affinities, calculated as total energy differences, for a large sample of polycyclic aromatic hydrocarbons (PAHs), ranging in size from azulene (C10H8) to dicoronylene (C48H20). For 20 out of 22 molecules under study we obtained electron affinity values in the range 0.4–2.0 eV, showing them to be able to accept an additional electron in their LUMO π orbital. For the mono-anions we computed the absolute photo-absorption cross-sections up to the vacuum ultraviolet (VUV) using an implementation in real time and real space of the Time-Dependent Density Functional Theory (TD–DFT), an approach which has already been proven to yield accurate results for neutral and cationic PAHs. Comparison with available experimental data hints that this is the case for mono-anions as well. We find that PAH anions, like their parent molecules and the corresponding cations, display strong π∗ ← π electronic transitions in the UV. -
Photo-Processing of Astro-Pahs
Photo-processing of astro-PAHs C Joblin1, G Wenzel1, S Rodriguez Castillo1,2, A Simon2,H Sabbah1,3, A Bonnamy1, D Toublanc1, G Mulas1,4, M Ji1, A Giuliani5,6, L Nahon5 1Institut de Recherche en Astrophysique et Plan´etologie(IRAP), Universit´ede Toulouse (UPS), CNRS, CNES, 9 Avenue du Colonel Roche, F-31028 Toulouse Cedex 4, France 2Laboratoire de Chimie et Physique Quantiques (LCPQ/IRSAMC), Universit´ede Toulouse and CNRS,UT3-Paul Sabatier, 118 Route de Narbonne, 31062 Toulouse, France 3Laboratoire Collisions Agr´egatsR´eactivit´e(LCAR/IRSAMC), Universit´ede Toulouse (UPS), CNRS, 118 Route de Narbonne, F-31062 Toulouse, France 4Istituto Nazionale di Astrofisica (INAF), Osservatorio Astronomico di Cagliari, Via della Scienza 5, I-09047 Selargius (Cagliari), Italy 5Synchrotron SOLEIL, L'Orme des Merisiers, F-91192 Gif-sur-Yvette Cedex, France 6INRA, UAR1008, Caract´erisationet Elaboration des Produits Issus de l'Agriculture, F-44316 Nantes, France E-mail: [email protected] Abstract. Polycyclic aromatic hydrocarbons (PAHs) are key species in astrophysical environments in which vacuum ultraviolet (VUV) photons are present, such as star-forming regions. The interaction with these VUV photons governs the physical and chemical evolution of PAHs. Models show that only large species can survive. However, the actual molecular properties of large PAHs are poorly characterized and the ones included in models are only an extrapolation of the properties of small and medium-sized species. We discuss here experiments performed on trapped ions including some at the SOLEIL VUV beam line DESIRS. We focus + on the case of the large dicoronylene cation, C48H20, and compare its behavior under VUV processing with that of smaller species. -
Laboratory Studies for Planetary Sciences
Laboratory Studies for Planetary Sciences A Planetary Decadal Survey White Paper Prepared by the American Astronomical Society (AAS) Working Group on Laboratory Astrophysics (WGLA) http://www.aas.org/labastro Targeted Panels: Terrestrial Planets; Outer Solar System Satellites; Small Bodies Lead Author: Murthy S. Gudipati Ice Spectroscopy Lab, Science Division, Mail Stop 183-301, Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109. [email protected], 818-354-2637 Co-Authors: Michael A'Hearn - University of Maryland [email protected], 301-405-6076 Nancy Brickhouse - Harvard-Smithsonian Center for Astrophysics [email protected], 617-495-7438 John Cowan - University of Oklahoma [email protected], 405-325-3961 Paul Drake - University of Michigan [email protected], 734-763-4072 Steven Federman - University of Toledo [email protected], 419-530-2652 Gary Ferland - University of Kentucky [email protected], 859-257-879 Adam Frank - University of Rochester [email protected], 585-275-1717 Wick Haxton - University of Washington [email protected], 206-685-2397 Eric Herbst - Ohio State University [email protected], 614-292-6951 Michael Mumma - NASA/GSFC [email protected], 301-286-6994 Farid Salama - NASA/Ames Research Center [email protected], 650-604-3384 Daniel Wolf Savin - Columbia University [email protected], 212-854-4124, Lucy Ziurys – University of Arizona [email protected], 520-621-6525 1 Brief Description: The WGLA of the AAS promotes collaboration and exchange of knowledge between astronomy and planetary sciences and the laboratory sciences (physics, chemistry, and biology). -
Computational Surface Modelling of Ices and Minerals of Interstellar Interest—Insights and Perspectives
minerals Review Computational Surface Modelling of Ices and Minerals of Interstellar Interest—Insights and Perspectives Albert Rimola 1,* , Stefano Ferrero 1, Aurèle Germain 2 , Marta Corno 2 and Piero Ugliengo 2,3 1 Departament de Química, Universitat Autònoma de Barcelona, 08193 Bellaterra, Catalonia, Spain; [email protected] 2 Dipartimento di Chimica, Università degli Studi di Torino, 10125 Torino, Italy; [email protected] (A.G.); [email protected] (M.C.); [email protected] (P.U.) 3 Nanostructured Interfaces and Surfaces (NIS) Centre, Università degli Studi di Torino, 10125 Torino, Italy * Correspondence: [email protected]; Tel.: +34-93-581-3723 Abstract: The universe is molecularly rich, comprising from the simplest molecule (H2) to complex organic molecules (e.g., CH3CHO and NH2CHO), some of which of biological relevance (e.g., amino acids). This chemical richness is intimately linked to the different physical phases forming Solar-like planetary systems, in which at each phase, molecules of increasing complexity form. Interestingly, synthesis of some of these compounds only takes place in the presence of interstellar (IS) grains, i.e., solid-state sub-micron sized particles consisting of naked dust of silicates or carbonaceous materials that can be covered by water-dominated ice mantles. Surfaces of IS grains exhibit particular characteristics that allow the occurrence of pivotal chemical reactions, such as the presence of binding/catalytic sites and the capability to dissipate energy excesses through the grain phonons. The present know-how on the physicochemical features of IS grains has been obtained by the fruitful synergy of astronomical observational with astrochemical modelling and laboratory experiments. -
Interstellar Dust Within the Life Cycle of the Interstellar Medium K
EPJ Web of Conferences 18, 03001 (2011) DOI: 10.1051/epjconf/20111803001 C Owned by the authors, published by EDP Sciences, 2011 Interstellar dust within the life cycle of the interstellar medium K. Demyk1,2,a 1Université de Toulouse, UPS-OMP, IRAP, Toulouse, France 2CNRS, IRAP, 9 Av. colonel Roche, BP. 44346, 31028 Toulouse Cedex 4, France Abstract. Cosmic dust is omnipresent in the Universe. Its presence influences the evolution of the astronomical objects which in turn modify its physical and chemical properties. The nature of cosmic dust, its intimate coupling with its environment, constitute a rich field of research based on observations, modelling and experimental work. This review presents the observations of the different components of interstellar dust and discusses their evolution during the life cycle of the interstellar medium. 1. INTRODUCTION Interstellar dust grains are found everywhere in the Universe: in the Solar System, around stars at all evolutionary stages, in interstellar clouds of all kind, in galaxies and in the intergalactic medium. Cosmic dust is intimately mixed with the gas-phase and represents about 1% of the gas (in mass) in our Galaxy. The interstellar extinction and the emission of diffuse interstellar clouds is reproduced by three dust components: a population of large grains, the BGs (Big Grains, ∼10–500 nm) made of silicate and a refractory mantle, a population of carbonaceous nanograins, the VSGs (Very Small Grains, 1–10 nm) and a population of macro-molecules the PAHs (Polycyclic Aromatic Hydrocarbons) [1]. These three components are more or less abundant in the diverse astrophysical environments reflecting the coupling of dust with the environment and its evolution according to the physical and dynamical conditions. -
L115 Modeling the Unidentified Infrared Emission With
The Astrophysical Journal, 511:L115±L119, 1999 February 1 q 1999. The American Astronomical Society. All rights reserved. Printed in U.S.A. MODELING THE UNIDENTIFIED INFRARED EMISSION WITH COMBINATIONS OF POLYCYCLIC AROMATIC HYDROCARBONS L. J. Allamandola, D. M. Hudgins, and S. A. Sandford NASA Ames Research Center, MS 245-6, Moffett Field, CA 94035 Received 1998 July 13; accepted 1998 November 24; published 1999 January 18 ABSTRACT The infrared emission band spectrum associated with many different interstellar objects can be modeled successfully by using combined laboratory spectra of neutral and positively charged polycyclic aromatic hydro- carbons (PAHs). These model spectra, shown here for the ®rst time, alleviate the principal spectroscopic criticisms previously leveled at the PAH hypothesis and demonstrate that mixtures of free molecular PAHs can indeed account for the overall appearance of the widespread interstellar infrared emission spectrum. Furthermore, these models give us insight into the structures, stabilities, abundances, and ionization balance of the interstellar PAH population. These, in turn, re¯ect conditions in the emission zones and shed light on the microscopic processes involved in the carbon nucleation, growth, and evolution in circumstellar shells and the interstellar medium. Subject headings: infrared: ISM: lines and bands Ð ISM: individual (Orion Bar, IRAS 2227215435) Ð line: formation Ð line: identi®cation Ð line: pro®les Ð molecular data Ð radiation mechanisms: nonthermal 1. INTRODUCTION resemblance of the -
Coronene Encapsulation in Singlewalled Carbon Nanotubes
CHEMPHYSCHEM ARTICLES DOI: 10.1002/cphc.201301200 Coronene Encapsulation in Single-Walled Carbon Nanotubes: Stacked Columns, Peapods, and Nanoribbons Ilya V. Anoshkin,*[a] Alexandr V. Talyzin,*[b] Albert G. Nasibulin,[a, e] Arkady V. Krasheninnikov,[c] Hua Jiang,[a] Risto M. Nieminen,[d] and Esko I. Kauppinen[a] Encapsulation of coronene inside single-walled carbon nano- tions between the coronene molecules and the formation of tubes (SWNTs) was studied under various conditions. Under hydrogen-terminated graphene nanoribbons. It was also ob- high vacuum, two main types of molecular encapsulation were served that the morphology of the encapsulated products observed by using transmission electron microscopy: coronene depend on the diameter of the SWNTs. The experimental re- dimers and molecular stacking columns perpendicular or tilted sults are explained by using density functional theory calcula- (45–608) with regard to the axis of the SWNTs. A relatively tions through the energies of the coronene molecules inside small number of short nanoribbons or polymerized coronene the SWNTs, which depend on the orientation of the molecules molecular chains were observed. However, experiments per- and the diameter of the tubes. formed under an argon atmosphere (0.17 MPa) revealed reac- 1. Introduction Graphene nanoribbons (GNRs) are of great interest for various in SWNTs by using thermally induced fusion of the molecular applications due to their unique electronic properties.[1–7] GNRs precursors: coronene and perylene.[17] The nanoribbons exhib- -
Interstellar Ice Photochemistry and the Deuterium Enrichment and Chemical Properties of Meteoritic Polycyclic Aromatic Hydrocarbons S
63rd Annual Meteoritical Society Meeting 5003.pdf INTERSTELLAR ICE PHOTOCHEMISTRY AND THE DEUTERIUM ENRICHMENT AND CHEMICAL PROPERTIES OF METEORITIC POLYCYCLIC AROMATIC HYDROCARBONS S. A. Sandford1, M. P. Bernstein1,2, L. J. Allamandola1, J. S. Gillette3, and R. N. Zare3, 1NASA-Ames Research Center, MS 245-6, Moffett Field CA 94035 ([email protected]), 2SETI Institute, 2035 Landings Drive, Mountain View CA 94043, USA, 3Department of Chemistry, Stanford University, Stanford CA 94305, USA. Introduction: Polycyclic aromatic hydrocarbons surroundings over time. However, exchanged D atoms (PAHs) are known to be abundant and ubiquitous in at the other sites are labile only under UV irradiation; the interstellar medium (ISM) [1]. At the temperatures once irradiation ceases these atoms will not exchange typical of dense interstellar molecular clouds (T = 10–- with the environment. 50 K), the birth sites of stars and planetary systems, Because the aromatic fractions of meteoritic PAHs will be frozen out of the gas phase into icy grain organics are known to be enriched in deuterium [6], mantles. These mantles contain a number of molecular this raises the possibility that interstellar species, the most abundant being H2O, CH3OH, CO, photoprocessing of PAHs in D-enriched interstellar CO2, NH3, CH 4, and possibly N2 and O2 [2]. Many of ices has occurred [7]. The measured D/H ratios of these molecules are expected to be enriched in interstellar ices [8] and the observed exchange rates for deuterium via a number of interstellar chemical coronene (C 24H12)-D2O and d12-coronene (C24D12)-H2O processes [2]. While frozen in these D-enriched ices, isotopic substitution experiments show that PAHs in the PAHs will be exposed to ultraviolet photons from interstellar ices could easily attain the D/H levels nearby stars, the attenuated diffuse ISM radiation field, observed in meteorites [7]. -
Infrared Observations of Interstellar Ices
Infrared Observations of Interstellar Ices Adwin Boogert NASA Herschel Science Center IPAC, Caltech Pasadena, CA, USA 05 June 2012 Interstellar Dust School (Cuijk): Interstellar Ices (Boogert) 1 Scope ●Lecture 1 (Monday): What you need to know when planning, reducing, or analyzing infrared spectroscopic observations of dust and ices. ●Lecture 2 (Tuesday): Basic physical and chemical information derived from interstellar ice observations. Not discussed: laboratory techniques (see Palumbo lectures) and surface chemistry (see Cuppen lectures). ●Lecture 3 (Tuesday): Infrared spectroscopic databases. What's in them and how (not) to use them. ●Drylabs (Tuesday): Using databases of interstellar infrared spectra and of laboratory ices. Deriving ice abundances and analyzing ice band profiles. NOTE: Please download all presentations and drylab tar file: spider.ipac.caltech.edu/~aboogert/Cuijk/ 05 June 2012 Interstellar Dust School (Cuijk): Interstellar Ices (Boogert) 2 Topics ●Basics ● Ice mantle formation ● Deriving ice column densities and abundances ●YSO and background source selection ●Continuum determination ●Vibrational modes ●The interstellar ice inventory ●Ice band profile analysis: ● Polar versus apolar ices ● Amorphous versus crystalline ices ● Segregation in the ices ● Grain size and shape effects ●Location of ices ●Processing of ices by YSOs ●Complex molecules in ices? 05 June 2012 Interstellar Dust School (Cuijk): Interstellar Ices (Boogert) 3 Background Reading ● For the basics: Dust in the galactic environment, 2nd ed. by D.C.B. Whittet. Bristol: Institute of Physics (IOP) Publishing, 2003 Series in Astronomy and Astrophysics, ISBN 0750306246. ● More advanced: Chapter 10 in “The Physics and Chemistry of the Interstellar Medium”, A. G. G. M. Tielens, ISBN 0521826349. Cambridge, UK: Cambridge University Press, 2005. -
UV Photolysis of Quinoline in Interstellar Ice Analogs
Meteoritics & Planetary Science 41, Nr 5, 785–796 (2006) Abstract available online at http://meteoritics.org UV photolysis of quinoline in interstellar ice analogs Jamie E. ELSILA1*, Matthew R. HAMMOND2, Max P. BERNSTEIN1, Scott A. SANDFORD1, and Richard N. ZARE2 1NASA Ames Research Center, MS 245-6, Moffett Field, California 94035–1000, USA 2Department of Chemistry, Stanford University, Stanford, California 94305–5080, USA *Corresponding author. E-mail: [email protected] (Received 16 November 2005; revision accepted 03 February 2006) Abstract–The polycyclic aromatic nitrogen heterocycle (PANH) quinoline (C9H7N) was frozen at 20 K in interstellar ice analogs containing either pure water or water mixed with methanol or methane and exposed to ultraviolet (UV) radiation. Upon warming, the photolysis products were analyzed by high-performance liquid chromatography and nanoscale liquid chromatography-electrospray ionization mass spectrometry. A suite of hydroxyquinolines, which were formed by the addition of oxygen atoms to quinoline, was observed as the primary product in all the ices. Quinoline N oxide was not formed, but five hydroxyquinoline isomers were produced with no clear dominance of one isomer. Reduction products, formed by hydrogen atom addition, were also created. Ices created at 20 K with H2O: quinoline ratios of 10:1 to 100:1 showed similar product distributions to those at 122 K, with no apparent temperature or concentration dependence. Increasing the UV dose led to a decrease in overall yield, indicating that quinoline and its products may be photo-destroyed. Methylquinolines were formed upon photolysis of the methanol- and methane-containing ices. In addition, possible methoxyquinolines or quinoline methylene alcohols were formed in the methanol- containing ice, while methylhydroxyquinolines were created in the methane-containing ice. -
Gudipati Keck Comet Physical and Chemical Composition of Comet
Present Understanding of Comet Nucleus Physical and Chemical Composition Murthy S. Gudipati Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA 91109 Keck Study – Comet – June 5, 2017 Outline Comet – Physical Composition Comet - Chemical Composition Comet – History 2 Comet – Physical Composition Physical Composition of Comets 3 Comet Physical Composition Gas (Volatiles, now Super Volatiles) Dust (Silicate Grains) Water (in the form of Ice – major component) The Elephant in the Room: How these three components are put together in a comet’s nucleus? 4 Porosity Science, 349, aab0639, 2015 Dust/Ice = 0.4 – 2.6 Porosity = 75 -85% Enrichment of Dust Regions and vice versa? Dust = Carbonaceous Chondrites (high percentages of water & organics; silicates, oxides, sulfides, olivine, serpentine, etc.) 5 Density Icarus 277 (2016) 257–278 Density = 532 ± 7 kg m−3 Crystalline water-ice = 920 kg m−3 Amorphous water-ice = ~500 - 800 kg m−3 Carbonaceous chondrites = ~3 to 3.7 kg m−3 6 Thermal Inertia Science, 349, aab0464, 2015 Thermal Inertia:85±35 J m-2K-1s-1/2 Thermal gradient? How Deep to reach <30 K? 7 Surface Science, 349, aaa9816, 2015 ~20 cm granular (soft) Below hard crust How thick is the crust – cm range or m range? 8 Simultaneous UV & IR Absorption + Fluorescence Pyrene in H2O Ice UV - PAH IR - Ice Flu - PAH Lignell & Gudipati J. Phys. Chem A. 119 (2015) 2607 9 Are Comets Like Deep Fried Ice Cream? ~0.1 m Comet CG/67P Lignell & Gudipati J. Phys. Chem A. 119 (2015) 2607 10 Comet – Chemical Composition Chemical Composition of Comets 11 Composition of Interstellar Medium At 1 atm. -
H2O Ice Mixtures with CH3OH and NH3 in the Far-IR Region B
A&A 592, A81 (2016) Astronomy DOI: 10.1051/0004-6361/201628324 & c ESO 2016 Astrophysics Interstellar ice analogs: H2O ice mixtures with CH3OH and NH3 in the far-IR region B. M. Giuliano1; 4, R. Martín-Doménech1, R. M. Escribano2, J. Manzano-Santamaría1; 3, and G. M. Muñoz Caro1 1 Centro de Astrobiología, INTA-CSIC, Carretera de Ajalvir, km 4, Torrejón de Ardoz, 28850 Madrid, Spain e-mail: [email protected] 2 Instituto de Estructura de la Materia-Consejo Superior de Investigaciones Científicas (IEM-CSIC), 28006 Madrid, Spain 3 Dept. de Matemática Aplicada, Ciencia e Ingeniería de Materiales, ESCET, Universidad Rey Juan Carlos. C/ Tulipán s/n, Móstoles 28933 Madrid, Spain 4 Max-Planck-Institut für extraterrestrische Physik, Giessenbachstrasse 1, 85748 Garching, Germany Received 17 February 2016 / Accepted 29 May 2016 ABSTRACT Context. New spectroscopic observations in the far-infrared (IR) range are expected from future planned missions. Although water ice is the only species detected so far in interstellar ices in this range, the presence of ice mixtures requires laboratory characterization of the corresponding spectra. Aims. We present an investigation on far-IR spectra of binary ice mixtures relevant in various astrophysical environments. The fore- most goal is to compare the spectroscopic features of the ice mixtures to those of pure ices, and to search for changes in peak frequencies, intensities, and band strengths of the main bands. Methods. Mixtures H2O:CH3OH and H2O:NH3 of different ratios have been deposited on a diamond substrate at astrophysically relevant conditions. We measured the spectra in the near- and mid-IR regions to derive ice column densities that were subsequently used to calculate the apparent band strengths in the far-IR region.