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  • 1
    Call number: S 97.0506(674-2)
    In: Forschungsbericht
    Type of Medium: Series available for loan
    Pages: 84 S. : z.T farb. Ill.+ graph. Darst. , Ill., graph. Darst.
    Edition: Als Ms. gedr.
    ISBN: 9783941721272
    Series Statement: Forschungsbericht / DGMK, Deutsche Wissenschaftliche Gesellschaft für Erdöl, Erdgas und Kohle e.V. 674-2
    Classification:
    Geophysical Exploration, Geophysical Prospecting
    Location: Lower compact magazine
    Branch Library: GFZ Library
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  • 2
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Chaos 2 (1992), S. 469-472 
    ISSN: 1089-7682
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Orbits in the three-dimensional billiard of the form of a truncated ellipsoid ("barrel'') are studied both analytically and numerically. A special form of mapping is proposed to get the expression for Kolmogorov–Sinai entropy, and the transition from strong chaos to weak chaos is obtained.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 2774-2782 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Infrared holeburning has been observed from mixed crystals. NH3D+ ions were imbedded in (NH4)2SO4–K2SO4 mixed crystals, the sample irradiated at the N–D stretching frequency, and resulting spectral hole then continuously monitored by a Fourier-transform infrared (FTIR) spectrometer. The holewidth decreases proportionally to the center frequency of the hole; within the range of 2240–2300 cm−1, the width changes from 10 to 5 cm−1 at 7.5 K. A longer irradiation time ((approximately-greater-than)10 min), however, leads to a wider spectral hole and also comparatively larger antiholes. The holewidth also shows a T2 type increase with temperature over the range of 7.5–45 K. Decay of the hole (hole filling) is not exponential, indicating that there is a distribution of decay rates. The holeburning quantum efficiency remains almost unchanged with temperature. Similarly, it remains almost constant with the variation of the mole-fraction of (NH4)2SO4 in the solid solution [in the range of 5%–100% mole-fraction of (NH4)2SO4], while the hole decay rate varies more than 20-fold. The constant holeburning quantum efficiency is surprising, considering that the phonon density increases by several orders of magnitude in the experimental temperature range and that the variation of the (NH4)2SO4 concentration changes the height of the rotational barrier of the ammonium ion. Thus, the holeburning must occur by conformational change in the excited vibrational state.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 10068-10069 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The ND stretching bands of the title compound have been burned. The polymer is doped with deuterium and contains a small amount of NH3D+ ion. The resulting holes are similar to those produced in inorganic ammonium salts, but the hole burning efficiency of the burning process is lower in the polymer.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 5661-5667 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: [(NH4)x,Rb1−x]2SO4 mixed crystals (0.16≤x≤1) were doped with NH3D+. Four of the eight N–D stretching bands of the NH3D+ ion gradually disappear with increasing Rb+ ion concentration while the widths of the N–D stretching bands increase, indicating that Rb+ ions first substitute NH4+ ions only in one type of crystal site, and that addition of Rb+ ions introduces glasslike disorder into the (NH4)2SO4-type crystalline structure. Infrared hole burning has been demonstrated in the broadened N–D stretching band of NH3D+ ion using a combination of a diode laser and a Fourier-transform infrared spectrometer. The initial hole width decreases proportionally with the center frequency of the hole at all Rb+ ion concentrations and agrees with the measurements of the [(NH4)x,K1−x]2SO4 mixed crystals. The similar proportionality, long known for many hydrogen-bonded systems in solution, suggests that the widths observed in solution are homogeneous. A longer irradiation time ((approximately-greater-than)10 min), however, leads to a wider spectral hole. Measured hole decay rates decrease with decrease of the center frequency of the hole, showing that the rotational tunneling barrier increases with the strength of the hydrogen bond. The change of the rotational tunneling barrier with Rb+ ion concentration is also observed as a change of the hole decay rate (more than tenfold in the experimental range). On the other hand, the hole burning quantum efficiency shows little change with the Rb+ ion concentration, or temperature. The observed steady holeburning quantum efficiency supports the infrared hole burning mechanism proposed in our previous study: The configurational change of the hole burning must occur in the excited vibrational state.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 5 (1993), S. 1408-1412 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The calculation of the growth rate of tearing modes is extended to short scale lengths by including the Hall field. A unified dispersion relation is found that describes usual tearing modes at one limit and the Hall tearing modes with the enhanced growth rate at the opposite limit. The dispersion relation is valid for both collisional and collisionless plasmas.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 4 (1992), S. 3-5 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Drift tearing modes have a threshold Δ' for instability, which is increased by sheared poloidal rotation. Sheared rotation becomes important for v'θ≥ω*. The critical Δ' is approximately linear in ||v'θ||. The linear stability of tearing modes is relevant to tokamak edge conditions at the L- to H-mode transition.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 4 (1992), S. 934-937 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The L to H-mode transition is accompanied by a drop in the magnetic signal of a mode with low toroidal mode number, usually n=1. Quasilinear drift stabilization can cause a saturated tearing mode to collapse, under the conditions at the edge of a tokamak plasma. The criterion for stabilization gives a relation of temperature to magnetic field T∝Bα, with 6/7≥α≥2/3. The collapse of the island could trigger the H mode by reducing the stochastic magnetic field layer around the magnetic separatrix. This would improve edge confinement, helping to form a transport barrier. Improvement of electron edge confinement could make the electric field more negative, producing the rotation seen in experiments.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 5422-5431 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An analysis of the observed frequencies of the Raman-active longitudinal acoustic mode (LAM) bands of room-temperature crystalline n-alkanes in the chain-length range C33 to C246 indicates that, as the chains become longer, there is a significant decrease in interlayer interaction, this interaction being measured by the vibrational coupling between the ends of chains in adjoining layers. This conclusion is based mainly on LAM measurements on n-alkanes longer than 100 carbons that have recently become available. In the present analysis, the n-alkane crystals are modeled as collinear monatomic chains having end-to-end interactions to simulate interlayer interaction. One intrachain force constant (F) and one interchain coupling force constant (f ) were evaluated from the observed frequencies of the LAM-1 and LAM-3 bands for each of seven n-alkanes: C48, C62, C70, C72, C94, C150, and C192. As expected, the values found for F are essentially independent of chain length. However, the values of f were found to decrease in going to longer chains, contradicting the generally held view that the interlayer force constant is independent of chain length. The value of f is proportional to 1/n within experimental error. If we assume this proportionality, the observed Raman frequencies of the LAM-m modes can be accounted for quantitatively. This is not the case if f is assumed independent of chain length. The decrease in the interchain interaction with increasing chain length is attributed to an increase in the layer separation resulting from an increase in chain-end amplitudes associated with the low-frequency longitudinal vibrations of longer chains.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 94 (1990), S. 2801-2806 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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