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  • Chemistry  (1)
  • PACS:21.60.Cs Shell model – 23.20.Lv Gamma transitions and level energies – 27.80.+w 190 ≤ A ≤ 219 – 25.70.-z Low and intermediate energy heavy-ion reactions  (1)
  • 1
    ISSN: 1434-601X
    Keywords: PACS:21.60.Cs Shell model – 23.20.Lv Gamma transitions and level energies – 27.80.+w 190 ≤ A ≤ 219 – 25.70.-z Low and intermediate energy heavy-ion reactions
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract: High spin states in nuclei around 208Pb were populated in deep inelastic collisions of 76Ge, 136Xe, and 208Pb projectiles with 208Pb targets at beam energies about 12% above the Coulomb barrier. New states in 209Pb were found by measuring γ-γ-coincidences. They are interpreted as the yrast states that originate from the coupling of one neutron to the lowest excitations of the 208Pb core. The results are discussed in the frame of the shell model.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 0044-2313
    Keywords: Strontium hydride imide nitride ; preparation ; crystal structure determination ; Chemistry ; Inorganic Chemistry
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Description / Table of Contents: Crystal Structure Determination of a Strontium Hydride Imide Nitride - Sr2(H)N/SrNH resp. Sr2(D)N/SrND - by X-Ray, Neutron, and Synchrotron RadiationStrontium reacts with nitrogen and hydrogen resp. deuterium under well defined conditions to a phase containing hydride, imide and nitride ions.Sr is evaporated at 1000°C. The Sr vapor reacts with N2 and H2 resp. D2 (p(N2) = p(H2/D2) = 50 mbar) in the gas phase. The product crystallizes as orange-yellow resp. black needles at 800°C.Neither X-ray single crystal nor X-ray and neutron powder diffraction data led to an acceptable model for the crystal structure. A high resolution diffraction experiment with synchrotron radiation gave the needed informations:Splitting of reflections led to a model in R3m with a = 3.870(1) Å and c = 18.958(3) Å. Further split reflections indicate, that the crystals contain areas where SrNH is a second phase besides Sr2(H)N. Neutron diffraction data (measured at 2 K, 10 K, 300 K and 505 K) were interpreted by a two phase model with Sr2(D)N/SrND: In a slightly distorted cubic close packing of Sr-atoms hydride and nitride resp imide ions occupy each by one third octahedral sites fully and in an ordered way.
    Notes: Strontium reagiert mit Stickstoff und Wasserstoff bzw. Deuterium unter definierten Bedingungen zu einer Phase, in der Hydrid-, Imid- und Nitridionen nebeneinander vorliegen.Sr wird bei bei 1000°C verdampft. Die Reaktion mit N2 und H2 bzw. D2 (p(N2) = p(H2/D2) = 50 mbar) findet in der Gasphase statt. Das Produkt kristallisiert als orange-gelbe bzw. schwarze Kristallnadeln bei 800°C.Weder aus Röntgen-Einkristall- noch aus Röntgen- oder Neutronenbeugungs-Pulverdaten konnte die Kristallstrukur eindeutig bestimmt werden. Erst ein hochauflösendes Beugungsexperiment mit Synchrotronstrahlung am Pulver gab entscheidende Hinweise auf ein Strukturmodell:Aufspaltungen von Reflexen können nur mit einem Modell in R3m mit a = 3,870(1) Å und c = 18,958(3) Å erklärt werden. Zusätzliche Reflexe zeigen, daß in den Kristallen neben Sr2(H)N Bereiche mit SrNH als zweiter Phase vorhanden sind. Die Verfeinerung von Neutronenbeugungsdaten (Messungen bei 2 K, 10 K, 300 K und 505 K) mit einem Zweiphasenmodell Sr2(D)N/SrND führt zu einem sinnvollen Ergebnis: In einer leicht verzerrten kubisch dichten Anordnung von Sr-Atomen besetzen schichtenweise in Domänen Hydrid- und Nitridionen bzw. Imidionen Oktaederlücken vollständig und geordnet jeweils zu einem Drittel.
    Additional Material: 13 Ill.
    Type of Medium: Electronic Resource
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