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  • 1985-1989  (4)
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Year
  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 65 (1989), S. 5068-5071 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Irradiating an ultraviolet (uv) laser on aluminum (Al) and gold (Au) thin targets, emissions from the rear side of the targets were temporally resolved. A clear difference was observed between the above two targets. Given the fact that absorbed laser energy can be converted with a very high efficiency to soft x rays in a high-Z plasma, a characteristic emission peak only observed for Au targets was attributed to the effect of soft x-ray energy transport. The observed results were compared with those computed by a one-dimensional hydrodynamic simulation himico. The ablation pressures estimated from the emissions indicate that the pressure scaling for Au is close to the one by x-ray drivers rather than by a uv laser.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 1787-1789 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Dependence of x-ray emission efficiencies on a plasma volume were obtained for a 527 nm laser with Cu targets and for 263 nm with Cu and Au targets using the same prepulse technique as the one used by Kodama et al. [Appl. Phys. Lett. 50, 720 (1987)]. 4ω results indicate that a maximum of three times increase was observed in soft x-rays(hν=100–200 eV), while no appreciable increase was observed in hard x rays(hν=1–3 keV). From 2ω results, a factor of 2 for the soft x rays and a factor of 3 for the hard x rays were observed.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 52 (1988), S. 786-788 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Emission from the rear side of 263-nm laser irradiated thin foil targets shows the temporal profile of rear surface heating by several processes with different energy transport mechanisms. Formation and decay of shock waves are observed by varying target thickness. Propagation of a thermal conduction wave is clearly separated from the shock propagation.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Journal of neurochemistry 44 (1985), S. 0 
    ISSN: 1471-4159
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Medicine
    Notes: The distribution of kinin in the CNS of the rat, which was extracted with n-butanol from an acidified homogenate, was determined using a bradykinin (BK) radioimmunoassay system. The immunoreactive kinin was widely distributed throughout the brain. The highest content was found in the pituitary gland (4,135 fmol BK Eq/g), followed by the medulla oblongata (912 fmol/g), cerebellum (549 fmol/g), and cortex (512 fmol/g). The kinin in the posterior pituitary was concentrated 4.5 times as much as in the anterior lobe. Serial dilution of brain extracts produced binding curves parallel to the standard radioimmunoassay curve. The purified brain kinin comigrated with authentic BK during CM-cellulose chroma tography and Sephadex LH-20 gel chromatography. Its molecular weight was estimated to be 1,127$45 by gel filtration, which coincides well with that of BK. Chymotrypsin degraded the extracted kinin and authentic BK, but trypsin did not. These data demonstrate that a peptide indistinguishable from BK exists in the rat brain. Furthermore, pituitary kinin was separated into BK (87%), Lys-BK (10%), and Met-Lys-BK (3%), using reverse phase HPLC.
    Type of Medium: Electronic Resource
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