Formation of positive ions of quadricyclane

POSTER

Abstract

Quadricyclane (QC) is one of the strained hydrocarbons that have potential as high-energy density materials used as aerospace fuel or as additives to kerosene rocket fuel. We have studied the formation of positive ions of QC by electron impact and by charge-transfer reactions, using Fourier-transform mass spectrum (FTMS) techniques. The electron ionization cross sections in the energy range of 10-200 eV have been measured. The total cross section reaches a maximum of 2.3x10$^{-15}$ cm$^{2}$ at 60 eV. Parent ion C$_{7}$H$_{8}^{+}$ and 21 fragment ions including C$_{5}$H$_{6}^{+}$ and C$_{5}$H$_{5}^{+}$ that dominate the dissociation channels at low energies ($<$25 eV) are observed. Ar$^{+}$ charge-transfer reaction with QC produces C$_{5}$H$_{5}^{+}$ and C$_{7}$H$_{7}^{+}$ as the major ionic species. Some selected hydrocarbon ions, i.e., C$_{3}$H$_{3}^{+}$, C$_{5}$H$_{3}^{+}$, C$_{5}$H$_{5}^{+}$ and C$_{5}$H$_{6}^{+}$, which are formed from QC by electron ionization, are found to react with QC forming C$_{7}$H$_{7}^{+}$ and C$_{7}$H$_{8}^{+}$ as the major product ions, while the latter two ions are unreactive with QC. The relative rates of the hydrocarbon ion reactions, compared to the Ar$^{+}$ charge-transfer reaction, are rather low; while the rate for C$_{3}$H$_{3}^{+ }$is less than 20 percent of the Ar$^{+}$ reaction rate, the rates for C$_{5}$H$_{3}^{+}$, C$_{5}$H$_{5}^{+}$ and C$_{5}$H$_{6}^{+}$ are less than 3 percent.

Authors

  • C.Q. Jiao

    Innovative Scientific Solutions, Inc., Dayton, OH

  • C.A. DeJoseph, Jr.

    Air Force Research Laboratory, Wright-Patterson AFB, OH 45433, Air Force Research Laboratory, Wright-Patterson AFB, OH

  • Shunji Kuroiwa

    PSAC/NIE/NTU, Singapore, School of Physics, The University of Sydney, Sydney NSW 2006, Australia, Nantes University, France, Varian Semiconductor Equipment Associates, Gloucester, MA01930, USA, Institute of Physics, POB 68, 11080 Zemun, Belgrade, Serbia and Montenegro, Department of Aeronautics and Astronautics, Kyoto University, Japan, Institut fur Kernphysik, Universitat Frankfurt, University of Missouri - Rolla, University of Maryland, Department of Physics, Department of Physics and Astronomy, Drake University, Des Moines, Iowa 50311, USA, CSIRO Molecular Science, Organic Chemistry Institute, University of Heidelberg, Centre for Molecular Simulation and School of Information Technology, Swinburne University of Technology, Department SBG, Limburgs Universitair Centrum, The Open University, Department of Mechanical Engineering, University of Minnesota, INP-Greifswald-Germany, LACE-Lyon-France, California State Polytechnic University, Pomona, Dublin City University, Ireland, OSRAM GmbH, D-81536 Munich, Germany, Institute of Low Temperature Plasma Physics, 17489 Greifswald, Institut of Physics, University of Greifswald, Germany, Instituto de Ciencias Nucleares, UNAM, UAM, Acopotzalco, Centro de Ciencias F\&#039;{i}sicas, UNAM, Eindhoven University of Technology, Sandia National Lab, Air Force Research Laboratory WPAFB, School of Electrical Engineering, Bulevar Kralja Aleksandra 73, 11000 Belgrade, Serbia and Montenegro, Advanced Energy Incorporated, Applied Materials Incorporated, National Centre for Plasma Science and Technology, Dublin City University, Ireland, Institute for Plasma and Atomic Physics, Ruhr-University Bochum, Germany, Institute for Plasma and Atomic Physics, Ruhr University Bochum, Germany, OSRAM Sylvania, HanYang University, Ruhr-University of Bochum, Nagoya University, Stanford University, Department of Physical Electronics -- Masryk University, Brno, Czech Republic, Hypertherm Inc., University of Minnesota, Los Alamos National Laboratory, LPTP Ecole Polytechnique 91120 Palaiseau, LACE UCB-Lyon1 UMR CNRS 5634 blvd 11Nov.1918 69100 Villeurbanne France, Lawrence Berkeley National Laboratory, University of California, Davis, Multicharged Ions Spectra Data Center of VNIIFTRI, Advanced Photon Research Center, Japan Energy Research Institute, Applied Physics Division, Los Alamos National Laboratory, Theoretical Division Los Alamos National Laboratory, Gaseous Electronics Inst., Nagoya Institute of Technology, Department of Electrical Engineering and Computer Sciences, University of California, Berkeley, CA 94720-1770, Science Institute, University of Iceland, Reykjavik, Iceland, Australian National University, Flinders University, KAIST, Plasmart Co., Samsung Electronics, St Petersburgh State University-Russia, Trinity College Dublin, Ireland, School of Physics, The University of Sydney, Australia, INP Greifswald, F.-L.-Jahn-Str. 19, 17489 Greifswald, Germany, Sungkyunkwan University, Korea, National University of Ireland, Maynooth, Ireland, Applied Materials, Tokyo Institute of Technology, LPTP, Ecole Polytechnique, LPTP, Ecole Polytechnique, 91128 Palaiseau, France, School of Physics, University of Sydney, Physics Dept, Macquarie University, Australia, Department of Applied Science, University of California at Davis, Stevens Institute of Technology, Department of Electrical Engineering and Computer Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan, Shibaura Mechatronics Corp.

  • A. Garscadden

    Air Force Research Laboratory, Wright-Patterson AFB, OH