7 research outputs found

    Photodissociation spectroscopy and dynamics of the CH(2)CFO radical

    Get PDF
    Alexandra A. Hoops, Jason R. Gascooke, Kathryn E. Kautzman, Ann Elise Faulhaber, and Daniel M. Neumar

    PHOTODISSOCIATION OF SMALL Iāˆ’^{-}(H2{_2}O)n{_n} CLUSTERS EXCITED TO THE CHARGE TRANSFER TO SOLVENT STATE

    No full text
    Author Institution: The Department of Chemistry, the University of California, Berkeley, and the Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, 94720Anions in polar solvents typically display a broad absorption band in the UV due to the transfer of charge from the anion to the solvent. These charge transfer to solvent states (CTTS) have been the subject of many studies in the bulk and more recently in clusters. Although Iāˆ’^{-}(H2{_2}O)n{_n} clusters have been studied both theoretically as well as experimentally, there is still some uncertainty as to the nature of the cluster analog of the CTTS state. Results presented here describe experiments performed using the fast beam photofragment coincident imaging technique to determine the main photodissociation products and translational energy distributions (P(ET{_T})) of Iāˆ’^{-}(H2{_2}O)n{_n} clusters excited to the CTTS state. A cool beam of Iāˆ’^{-}(H2{_2}O)n{_n} (n = 2-5) clusters is accelerated, mass selected and excited to the CTTS state. The resulting photofragments strike a time-and-position-sensitive detector, enabling the calculation of product masses as well as the corresponding P(ET{_T}). In all cases, two channels are observed. The main channel is a 2-body process producing neutral I and (H2{_2}O)n{_n} products, and the minor channel is a 3-body process forming neutral I, (H2{_2}O)nāˆ’1{_{n-1}} and H2{_2}O products. Both channels impart little translational energy to the photofragments for all cluster sizes. Photodissociation is believed to occur following autodetachment of the cluster, producing neutral products

    Dissociative Photodetachment Studies of I 2

    No full text

    Light-Absorbing Oligomer Formation in Secondary Organic Aerosol from Reactive Uptake of Isoprene Epoxydiols

    No full text
    Secondary organic aerosol (SOA) produced from reactive uptake and multiphase chemistry of isoprene epoxydiols (IEPOX) has been found to contribute substantially (upward of 33%) to the fine organic aerosol mass over the Southeastern U.S. Brown carbon (BrC) in rural areas of this region has been linked to secondary sources in the summer when the influence of biomass burning is low. We demonstrate the formation of light-absorbing (290 < Ī» < 700 nm) SOA constituents from reactive uptake of <i>trans</i>-Ī²-IEPOX onto preexisting sulfate aerosols as a potential source of secondary BrC. IEPOX-derived BrC generated in controlled chamber experiments under dry, acidic conditions has an average mass absorption coefficient of āˆ¼300 cm<sup>2</sup> g<sup>ā€“1</sup>. Chemical analyses of SOA constituents using UVā€“visible spectroscopy and high-resolution mass spectrometry indicate the presence of highly unsaturated oligomeric species with molecular weights separated by mass units of 100 (C<sub>5</sub>H<sub>8</sub>O<sub>2</sub>) and 82 (C<sub>5</sub>H<sub>6</sub>O) coincident with the observations of enhanced light absorption, suggesting such oligomers as chromophores, and potentially explaining one source of humic-like substances (HULIS) ubiquitously present in atmospheric aerosol. Similar light-absorbing oligomers were identified in fine aerosol collected in the rural Southeastern U.S., supporting their atmospheric relevance and revealing a previously unrecognized source of oligomers derived from isoprene that contributes to ambient fine aerosol mass

    Fast beam studies of I(2)(-) and I(2)(-) (.) Ar photodissociation

    No full text
    Copyright Ā© 2003 Elsevier Science B.VThe photodissociation dynamics of bare Iā‚‚ā» and Iā‚‚ā» ā€¢ Ar at 413 and 390 nm have been investigated using a fast beam instrument coupled with a new photofragment coincidence imaging detector. Results from the application of this technique to the dissociation of Iā‚‚ā» and Iā‚‚ā» ā€¢ Ar yielded the dissociation energy of Iā‚‚ā» (Dā‚€(Iā‚‚ā»)=1.012Ā±0.008 eV) and Iā‚‚ā»ā€“Ar binding energy (D0(Iā‚‚ā»ā€“Ar)=45Ā±8 meV). The experiments show that at these wavelengths, Iā‚‚ā» ā€¢ Ar undergoes three-body dissociation to Iā» + I* + Ar, with very low momentum in the Ar atom and unequal momentum partitioning between the two I atoms.Alexandra A. Hoops, Jason R. Gascooke, Ann Elise Faulhaber, Kathryn E. Kautzman and Daniel M. Neumar
    corecore