EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Slides:



Advertisements
Similar presentations
C. Björkas, K. Vörtler and K. Nordlund Department of Physics, University of Helsinki Joint TFE-SEWG - Material Migration and Material Mixing meeting MD.
Advertisements

Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.
Cross Sections for Positrons Colliding with H, H 2, He Department of Physics National Tsing Hua University G.T. Chen 2007/6/12.
Program Degrad.1.0 Auger cascade model for electron thermalisation in gas mixtures produced by photons or particles in electric and magnetic fields S.F.Biagi.
Hee Seo, Chan-Hyeung Kim, Lorenzo Moneta, Maria Grazia Pia Hanyang Univ. (Korea), INFN Genova (Italy), CERN (Switzerland) 18 October 2010 Design, development.
Ionization II: Chemical Ionization CU- Boulder CHEM 5181 Mass Spectrometry & Chromatography J. Kimmel Fall 2007.
- Kinetic Theory of Mater - States of matter - Phase changes - Classes of Matter - Properties of Matter - Conservation of Mass.
Chemistry Review Matter- anything that has mass and takes up space Matter Anti- matter.
Mass Spectrometry The substance being analyzed (solid or liquid) is injected into the mass spectrometer and vaporized at elevated temperature and reduced.
Secondary electron emission in proton-Uracil collision: preliminary results P.Moretto-Capelle D.Bordenave-Montesquieu A.Bordenave-Montesquieu (A.Rentenier)
Ionisation of H 2 O by Proton and Atomic Hydrogen Impact at velocities ~ the Bragg peak Sam Eden Institut de Physique Nucléaire de Lyon
Water cluster- silica collision Water cluster, 104 H 2 O Simulation time, 17ps NVE simulations O 1560 Si atoms Molecular mass g/mole.
Phys 250 Ch12 p1 Chapter 12: Gas Laws and Kinetic Theory Air Pressure at bottom of column of mercury: P =  gh, h≈76 cm pressure= atmospheric pressure,
Salamanca.ppt, © Thomas Schwarz-Selinger, 03. Juni 2008 G. S. Oehrlein*, T. Schwarz-Selinger, K. Schmid, M. Schlüter and W. Jacob Interaction of Deuterium.
Electron interactions with CO 2 Bob Merlino Department of Physics and Astronomy The University of Iowa Iowa City, IA U. S. Department of Energy National.
Partial and differential electron impact ionization cross sections of acetylene S. Feil, K. Głuch, S. Matt, P. Scheier and T. Märk Institut für Ionenphysik.
C-O and O-H Bond Activation of Methanol by Lanthanum Atom Ruchira Silva, Dilrukshi Hewage and Dong-Sheng Yang Department of Chemistry University of Kentucky.
Chapter 2 Chemistry of Life
Fragmentation mechanisms for Methane induced by electron impact
1 Li Xiao and Lichang Wang Department of Chemistry & Biochemistry Southern Illinois University Carbondale The Structure Effect of Pt Clusters on the Vibrational.
PULSED-FIELD IONIZATION ELECTRON SPECTROSCOPY OF Al-URACIL COMPLEX Sergiy Krasnokutski and Dong-Sheng Yang University of Kentucky, Lexington, KY 40506,
Reforming and Fixation of Carbon Oxides in Atmospheric Pressure Non- thermal CO/CO 2 Plasmas Robert Geiger Advisor: Dr. David Staack Texas A&M Mechanical.
Investigation of Deposits in a Carbon Monoxide DBD Robert Geiger Advisor: Dr. David Staack Texas A&M Mechanical Engineering Plasma Engineering & Diagnostics.
Molecular mass spectrometry Chapter 20 The study of “molecular ions” M + e -  M e -
Forschergruppe Laboratory Astrophysics Interstellar Molecules.
Department of Experimental Physics, Comenius University Bratislava, Slovakia Formation of positive ions by electron impact: Temperature effects Š. Matejčík.
Plasma diagnostics using spectroscopic techniques
Pulsed Field Ionization-Zero Electron Kinetic Energy (PFI-ZEKE) Spectroscopy of Sc-C 6 H 5 X(X=F,CH 3,OH) Complexes Changhua Zhang, Serge A. Krasnokutskia.
The Advanced Light Source (ALS) at Lawerence Berkeley National Laboratory Berkeley, California Tunable VUV radiation from 8 – 30 eV Brian W. Ticknor 1,
Infrared Photodissociation Spectroscopy of Aluminum Benzene Cation Complexes Nicki Reishus, Biswajit Bandyopadhyay and Michael A. Duncan Department of.
VUV-diagnostics of inelastic collision processes in low temperature hydrogen plasmas J. Komppula & JYFL ion source group University of Jyväskylä Department.
Sputter deposition.
Modification of Si nanocrystallites in SiO2 matrix
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chemistry of Life Chapter 2 Table of Contents Section 1 Composition.
Basic Chemistry Element: pure substance that cannot be chemically broken down into simpler kinds of matter. Atom: smallest unit of an element that retains.
Max-Planck-Institut für Plasmaphysik CRP on ‘Atomic and Molecular Data for Plasma Modelling’, IAEA, Vienna26-28 September 2005 Compilation and Extension.
Infrared Spectra of Chloride- Fluorobenzene Complexes in the Gas Phase: Electrostatics versus Hydrogen Bonding Holger Schneider OSU International Symposium.
IR spectra of Methanol Clusters (CH3OH)n Studied by IR Depletion and VUV Ionization Technique with TOF Mass Spectrometer Department of Applied Chemistry.
Abel Blazevic GSI Plasma Physics/TU Darmstadt June 8, 2004 Energy loss of heavy ions in dense plasma Goal: To understand the interaction of heavy ions.
Chemistry of Life Chapter 2 Table of Contents Section 1 Composition of Matter Section 2 Energy Section 3 Water and Solutions.
To join as much as possible of the brazilian scientific and technological production in atomic, molecular and plasma physics that may be of interest to.
Atomic and Molecular Structure. 1. e. Students know the nucleus of the atom is much smaller than the atom yet contains most of its mass.
Main Title Manori Perera 1 and Ricardo Metz University of Massachusetts Amherst 64 th International Symposium on Molecular Spectroscopy June 25th, 2009.
PULSED-FIELD IONIZATION ELECTRON SPECTROSCOPY OF LANTHANIDE (Gd, Lu) BENZENE COMPLEXES M. ROUDJANE, S. KUMARI and D.-S. YANG University of Kentucky Lexington,
Ce-Promoted Bond Activation of Ethylene Probed by Mass-Analyzed Threshold Ionization Spectroscopy Department of Chemistry University of Kentucky, Lexington,
Penning transfers: survey of available data, life-time of excited states, pressure dependence Ozkan SAHIN Uludag University Physics Department Bursa -TURKEY.
Heavy Atom Vibrational Modes and Low-Energy Vibrational Autodetachment in Nitromethane Anions Michael C. Thompson, Joshua H. Baraban, Devin A. Matthews,
Velocity Map Imaging Study of a Mass-Selected Ion Beam: the Photoinitiated Charge-Transfer Dissociation of and Ag + (C 6 H 6 ) Jonathon A. Maner, Daniel.
INVESTIGATION OF VAN DER WAALS COMPLEXES IN A FREE EXPANSION OF C 2 H 2 /X (X=RARE GAS) (X=Rg) USING CW CAVITY RING-DOWN SPECTROSCOPY IN THE OVERTONE RANGE.
Many mass spectra are observed in addition to those of nitrogen (28amu) and benzene (78amu) molecules between 1 and 80amu, when the discharge is not generated.
The Chemistry of Life Electron Configuration & practice with the Periodic Table.
Forschungszentrum Karlsruhe Erice, 7th July th International School for Cosmic Rays Astrophysics Motivation Energy Reconstruction Air Fluorescence.
3.3 The Atom. Periodic Table of Elements Atomic Number: Number of protons in an atom; usually appears directly above the chemical symbol. Number of protons.
2. What are isotopes? Use two particles from the table above to illustrate your answer. (3 marks) 17 O & 18 O (1) Same Atomic mass / number of protons.
Saturn Magnetosphere Plasma Model J. Yoshii, D. Shemansky, X. Liu SET-PSSD 06/26/11.
Mass-Analyzed Threshold Ionization of Lu 2 Lu Wu, Mourad Roudjane, Dong-Sheng Yang Department of Chemistry University of Kentucky Lexington, KY, 40504,USA.
Dissociation of Molecular Ions Studied by
Electronic Spectrum of Cryogenic Ruthenium-Tris-Bipyridine Dications
FEBIAD ion source development efficiency improvement
ELEMENTS AND COMPOUNDS
Department of Chemistry University of Kentucky
Sub-Ns Electric Field Measurements
GENERATION OF NOVEL EEDFS IN A TANDEM PLASMA REACTOR
Chemistry-Part 1 Inside the Atom
Mass spectrometry Detection of ionic species to determine the molecular weight of and obtain structural information on a molecule.
DOE Plasma Science Center Control of Plasma Kinetics
Electron Impact Ionization of selected hydrocarbon molecules
Hot Cold Molecules: Collisions at Astrophysical Temperatures
Key Question: What is meant by a change in state?
Department of Chemistry University of Kentucky
Presentation transcript:

EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia

Bratislava

Overview - Appearance energies of C 2 D 6 - Cross section for EII to propane - BeH and BeH 2 – structure and energies - Structure and energetics of Be m H n clusters

Electron impact ionization cross sections (total, partial) ionization energies appearance energies kinetic energy release gas temperature dependencies products of the reactions

Experimental setup

Cross section measurements Absolute measurement of the pressure Relative flow technique Ar as a calibration gas

Atoms: Wannier theory:  w (E,AE,A,d) = 0 E<AE A(E-IE) d E>AE d=1.127 Threshold behaviour of the cross sections f(E,U) - EEDF Fitting function:

d=1.127±0.01 Threshold behaviour of the cross sections

CH 3 D AE (eV) 293 K CD 4 AE (eV) 293 K CH 4 AE (eV) 293 K CH 3 D ± ± ± 0.04CH 4 + CH 2 D + + H – CH 2 D + + H ± ± ± ± ± 0.1 CH H – CH H Isotopic effect on AE Denifl et al. IJMS 248 (2005) 29

Present meV a) meV b) meV (CH 3 D) + /CH 3 D10050 (CH 2 D) + /CH 3 D80 (CH 3 ) + /CH 3 D200 (CHD) + /CH 3 D110 (CD 4 ) + /CD (CD 3 ) + /CD (CD 2 ) + /CD a) F. P. Lossing, A. W. Tickner, W. A. Bryce, J. Chem. Phys. 19, 1254 (1951). b) V. H. Dibeler, M. Krauss, R. M. Reese, F. N. Harlee J. Chem. Phys. 42, 3791 (1965). Isotopic shift Denifl et al. IJMS 248 (2005) 29

EII of C 2 D 6 e + C 2 D 6 → C 2 D e → C 2 D D – + 2e → C 2 D D 2 + e

EII to C 2 D 6

Izotopic effects in C 2 D 6 a E. Vaseková, M. Stano, S. Matejcik,, J.D. Skalný, P. Mach, T.D. Märk, J. Urban Int. J. of Mass Spect., 235 (2004) e + C 2 D 6 →AE (in eV) PresentEthan a ( C 2 D 6 ) ± ± 0.06 ( C 2 D 5 ) ± 0.07 ?12.06± 0.03 ( C 2 D 4 ) ± ± 0.04 ( C 2 D 2 ) ± ± 0.2

Grill et al. ZPhysD 25 (1993) 217

EII to C 3 H 8

Appearance energies C 3 H 8 Denifl CPL 402 (2005) 80

EII to C 3 H 8 cross sections Exp: N. Duric, I. Čadež, M. Kurepa, Int. J. Mass Spectrom. & Ion Processes, 108 (1991) R1-R10.

Total cross sections σ BEB (12 eV)σ Present (12 eV)σ Exp (12 eV) [ cm 2 ] Exp: N. Duric, I. Čadež, M. Kurepa, Int. J. Mass Spectrom. & Ion Processes, 108 (1991) R1-R10. BEB: W. Hwang, Y.-K. Kim and M.E. Rudd, J. Chem. Phys., 104 (1996) 2956

Cross sections at 700 K Not finnished yet Problems with contamination

EII to Be x H y Experimental problems Vaporisation only at T>1000°C Toxicity of Be

BeH dissoc. energy CCSDT-R12 1exc. energy 2 Σ – 2 Π, experiment cm -1, theory – cm -1

BeH bond lenght

BeH 2 basisBeH 2 Be-H [A] TAE a) [eV] DE Be+H2 [eV] CCSD(T)- R12 Be:19s14p8d6f4g H: 9s,6p,4d,3f CCSD(T) Full aug-cc-pCvDZ aug-cc-pCvTZ aug-cc-pCvQZ aug-cc-pCv5Z B3LYP G(3d,3p) aug-cc-pCv5Z

BeH 2 bond lenght

Be n H clusters – MP2

Be n H 1

Be 3 H n Be 4 H n

Futher plans Propane cross section at high T C 2 D 6 – high T, cross sections Ionization energies of the Be compounds Appearance energies of the fragments Simulation of the Be surface Chemistry on the Be surface

Thank you for your attention