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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Cellular and molecular life sciences 26 (1970), S. 562-563 
    ISSN: 1420-9071
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology , Medicine
    Notes: Summary Culturing amphibian embryonic cells on different supports suggests the important role played by the contact between support and cellular membrane in spreading and morphological differentiation of these cells. They spread on glass but do not spread when glass is covered by acrylamide gels (3%, 7% and 9%), by acrylamide-carboxymethylcellulose, or acrylamide-hydroxyethylcellulose gels, or by agarose gel (1,5%). Nevertheless, cells spread and differentiate on mixed acrylamide (7% or 9%) agarose (0.80%) gels.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Il nuovo cimento della Società Italiana di Fisica 12 (1990), S. 673-684 
    ISSN: 0392-6737
    Keywords: Kinetic and transport theory ; Classical, semiclassical, quantum theories of liquid structure ; Neutron determination of structure
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Description / Table of Contents: Riassunto La dispersione di fluttuazioni di densità (modi di suono estesi) è stata misurata in miscugli di metalli alcalini liquidi con corrispondenti sali fusi di alogenuri alcalini. Miscele con concentrazioni saline da 10 a 40% sono state studiate per impulsi trasferitiQ da 4 a 14 nm−`. Per valori diQ piú grandi di 11 nm−1 i modi collettivi potrebbero anche nel caso piú favorevole non essere piú separati dal picco quasi elastico, l'ampiezza del quale aumenta di circaQ 2 in questa regione di impulsi trasferiti. Ad una concentrazione al 10% di RbCl in Rb si trova una dispersione che corrisponderebbe ad R liquido espanso alla temperature della miscela (∼1000 K), che dimostra il carattere dominante di metallo della miscela (schermatura mediante elettroni quasi liberi) e questa concentrazione salina. Ad alte concentrazioni saline, alle quali interagiscono influenze da differenti fattori dinamici parziali di struttura le dispersioni si discostano da questa semplice curva di dispersione strutturata, molto probabilmente a causa dell'influenza di una iniziale comparsa di qualche tipo di schermatura ionica nel liquido.
    Abstract: Резюме В смесях жидких щелочных металлов и соответствующих расплавленных щелочно-галоидных солей измерена дисперсия коллективных флуктуации плотности (протяженные звуковые моды). Были исследованы смеси с концентрациями солей от 10 до 40% при передаваемых импульсахQ между 4 и 14 нм−1. Для величинQ, большечем 11 нм−1, коллективные моды даже в наиболее благоприятном случае не выделяются из квазиупругого пика, ширина которого увеличивается приблизительно как ∼Q 2 в этой области передаваемых импульсов. При концентрациях 10% RbCl в Rb мы получчили дисперсию, которая соответствует жидкому Rb при температуре смеси (∼1000 K), что, демонстрирует доминирующих металлический характер смеси (экранирование обусловлено почти свободными электронами) при этой концентрации соли. При более высоких концентрациях соли, где существенно влияет взаимодействие различных парциальных динамических структурных факторов, дисперсии отличаются от простой структурной дисперсионной кривой, по-видимому, вследствие раннего возникновения ионного типа экранирования в жидкости.
    Notes: Summary The dispersion of collective density fluctuations (extended sound modes) has been measured in mixtures of liquid alkali metals and the corresponding molten alkali-halide salts. Mixtures with salt concentrations from 10 to 40% were investigated for momentum transfersQ between 4 and 14 nm−1. ForQ-values larger than 11 nm−1 the collective modes could even in the most favourable case no longer be separated from the quasi-elastic peak, the width of which increases roughly ∼Q 2 in this region of momentum transfers. At a concentration of 10% RbCl in Rb we find a dispersion which would correspond to expanded liquid Rb at the temperature of the mixture (∼1000 K), demonstrating the dominant metallic character of the mixture (screening by nearly free electrons) at this salt concentration. At higher concentrations of salt, where influences from different partial dynamic structure factors interplay, the dispersions deviate from this simple structured dispersion curve, most likely due to the influence of an early onset of some ionic type of screening in the liquid.
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  • 3
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Analytical Biochemistry 127 (1982), S. 1-8 
    ISSN: 0003-2697
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Biology , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Carbohydrate Research 151 (1986), S. 147-156 
    ISSN: 0008-6215
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 88 (1984), S. 3826-3833 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 1145-1149 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The exchange stiffness constant A of evaporated (Gd,Tb)-(Fe,Co) amorphous alloys with constant Curie temperature of 465±25 K was determined with two different methods for a large composition and temperature range. One is the excitation of standing spin waves using Brillouin light scattering. The other method is the deviation of A from measurements of the wall energy density σw and the uniaxial anisotropy Ku using the Bloch wall energy equation. σw could be determined from the applied magnetic field difference for collapsing and expanding of thermomagnetically written domains. The compositional and experimental limits of this method are described. The uniaxial anisotropy Ku was measured with a torque magnetometer. In GdTb-FeCo the resulting exchange stiffness constant of A=(2.6±0.6)×10−12 J/m was found to be independent of the Tb content. The results obtained from Brillouin light-scattering measurements on Gd21.2 Co78.8 and Gd13.5Tb6.2Fe80.3 are in good agreement.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6648-6651 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on the exchange bias effect as a function of the in-plane direction of the applied field in twofold symmetric, epitaxial Ni80Fe20/Fe50Mn50 bilayers grown on Cu(110) single-crystal substrates. An enhancement of the exchange bias field, Heb, up to a factor of 2 is observed if the external field is nearly, but not fully aligned perpendicular to the symmetry direction of the exchange bias field. From the measurement of the exchange bias field as a function of the in-plane angle of the applied field, the unidirectional, uniaxial and fourfold anisotropy contributions are determined with high precision. The symmetry direction of the unidirectional anisotropy switches with increasing NiFe thickness from [11¯0] to [001]. © 1999 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 83 (1998), S. 2863-2865 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: All contributing magnetic anisotropies in (110)-oriented exchange biased Ni80Fe20/Fe50Mn50 double layers prepared by molecular beam epitaxy on Cu(110) single crystals have been determined by means of Brillouin light scattering. Upon covering the Ni80Fe20 films by Fe50Mn50, a unidirectional anisotropy contribution appears, which is consistent with the measured exchange bias field. The uniaxial and fourfold in-plane anisotropy contributions are largely modified by an amount, which scales with the Ni80Fe20 thickness, indicating an interface effect. The strong uniaxial anisotropy contribution shows an in-plane switching of the easy axis from [11¯0] to [001] with increasing Ni80Fe20-layer thickness. The large mode width of the spin wave excitations, which exceeds the linewidth of uncovered Ni80Fe20 films by a factor of more than six, indicates large spatial variations of the exchange coupling constant. © 1998 American Institute of Physics.
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  • 9
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Static and dynamic magnetic properties of epitaxial Fe(001) films with Pd overlayers have been measured by means of Brillouin light scattering and magneto-optic Kerr effect magnetometry. From low energy electron diffraction studies, the initial growth of Pd [dPd〈2 monolayer (ML)] is identified as a self-formation process of quasione-dimensional Pd structures. Auger electron spectroscopy examinations proved that for dPd≥2 ML the Pd overlayers cover the Fe films almost completely. The measured frequencies of the dipolar spin wave mode and the derived anisotropy constants show a linear change with increasing dPd up to 5 ML with following saturation. The M(H) curves show pronounced anomalies in the coercive field for dPd〈2 ML accompanied by large tails in the hysteresis loops. The results are interpreted as a strong pinning of domain walls caused by large local changes in the surface anisotropy due to the inhomogeneous Pd cover layer in this regime. © 1997 American Institute of Physics.
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  • 10
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have investigated the propagation of surface and backward volume spin waves (BVSW) with the in-plane wavevector k(parallel)=10–900 cm−1 excited by microwaves in YIG and Lu2.04Bi0.96Fe5O12 (LBIG) films with the film thicknesses 5 and 1.5 μm, respectively. In all cases the magnetization and k(parallel) were in the film plane. The frequencies of the spin wave excitations as well as the spatial distribution of their intensities in the linear and in the nonlinear excitation regime were measured by means of a fully automated, high-stabilization, small-angle Brillouin light scattering (BLS) setup with a spatial resolution of 30 μm. It is well known1 that in the case of BVSW modes, the Lighthill criterion2 for modulational instability is fulfilled for both the longitudinal and the transverse perturbations of the initially constant-amplitude wave beam. Therefore, this mode is very much suitable for the investigation of the evolution of a plane-front, constant-amplitude initial beam, and for a direct experimental study of two-dimensional nonlinear diffraction effects of the beam leading to self-focusing. The garnet films with in-plane dimensions of 2×10 mm2 were grown by liquid phase epitaxy onto a single crystalline (111)-oriented gallium gadolinium garnet substrate. Two strip antennas, 35 μm wide and situated at the ends of the films, were used for the excitation of the spin waves and for monitoring. The working frequency was 8.10 GHz. Special efforts were taken to minimize the beam divergence due to the finite length of the input antenna. For all nonlinear studies the initial angular beam divergence was not larger than aitch-thetamax=0.05 rad. In the linear regime the attenuation factor was measured, and the reflection of the spin waves from the sample boundaries was studied. We also observed the interference between the two lowest order lateral modes having different initial spatial distributions of the magnetization. The BLS technique was shown to provide a signal to noise ratio exceeding 60 dB. In the nonlinear regime the propagation of the BVSW mode was thoroughly investigated. We have found clear evidence for the self-focusing effect, which exists in a narrow interval of input powers. In these studies overheating of the sample by the microwave power was carefully avoided by using an intermittent source of maximum average power of 100 mW working at a frequency of 4 kHz. That allowed us to claim that the observed focusing of the spin waves was not an artifact caused by sample heating. The distance between the focusing maximum and the antenna was 1.5 mm for LBIG sample and 6 mm for YIG sample. These values are in a good agreement with our theoretical calculations, if one takes into account the thicknesses of the films. For a comparison of the observed values of the width and the length of the focusing spot and their dependence on the microwave power with the theory, more numerical calculations are needed. Our results demonstrate the wide applicability of an advanced combined microwave-BLS technique for a two-dimensional mapping of the spin wave amplitudes in the media. © 1997 American Institute of Physics.
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