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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Radio-frequency-sputtered Co/Fe multilayers with layer thicknesses varying in the 8–100 A(ring) range were studied by extended x-ray absorption fine structure (EXAFS), x-ray absorption near edge spectroscopy (XANES), and nuclear magnetic resonance (NMR) techniques. While the Fe environment is body-centered-cubic (bcc) in all the samples, the Co environment depends drastically on the Co layer thickness. Under (approximately-equal-to)20 A(ring), investigation at the Co K edge by XANES provides a bcc fingerprint in both polarization directions. The XANES profile becomes typical of a full hcp stacking only for Co layer thicknesses larger than 98 A(ring). This behavior is confirmed by EXAFS spectra at the Co K edge and NMR analysis. For Co layer thickness between 6 and 18 A(ring), eight first neighbors at 2.48 A(ring) and six second neighbors at 2.83 A(ring) are detected which match the bcc phase. Resonance peak at a very low frequency is also observed (198 MHz). The second shell radius appears at 2.78 A(ring) only for larger Co layer thicknesses. This effect goes along with the NMR peak shift to higher frequency (220 MHz). All these results are consistent with a Co-bcc-like structure which changes into a hcp phase when the Co layer thickness increases.
    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 72 (1992), S. 4710-4713 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on structural and magnetic properties of diode rf-sputtered fcc Cu/Co(100) multilayers. All the samples exhibit a pseudo-epitaxial structure with interface roughness of the order of 6 A(ring). As the Cu layer thickness is varied, we observe oscillations of magnetoresistance corresponding to oscillations of the interlayer coupling. The maximum of magnetoresistance is found for tCu=18.5 A(ring) (up to ΔR/R≈6%). We furthermore measure a very high differential magnetoresistance (ΔR/RΔH=1.4 kOe−1). A combination of antiferromagnetic coupling and quadratic in-plane anisotropy is responsible for this large value of magnetoresistivity.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Single crystals of La1−xSrxMnO3 with x ranging from 0.06 to 0.42 have been investigated by various techniques: resistivity and magnetoresistance, superconducting quantum interference device magnetometry, and 55Mn nuclear magnetic resonance. In addition, for two Sr concentrations, x=0.13 and 0.25, the I(V) characteristic of the oxide-metal junction has been measured versus temperature. Semiconductor-metal transition occurring just below the Curie temperature Tc was observed for x≥0.175 whereas, for x≤0.15, the crystals exhibits only semiconducting behavior, in agreement in the previous studies. These transport properties are closely connected with the electron transfer mediated by the double exchange interaction between Mn3+ and Mn4+, as revealed by 55Mn spin-echo experiments. A cusp in the magnetoresistance (MR) was observed near Tc for the crystals with x≥0.13 with typical maximum resistivity ratio R(0)/R(10 T)≈10; for the sample with x=0.1, the huge MR persists well below Tc≈140 K, which is probably due to a noncollinear spin configuration. The I(V) characteristic of the oxide-aluminum junction is strongly dependent on temperature and applied magnetic field. In the semiconducting phase, a nonlinear behavior reminiscent to that of a strongly doped dirty semiconductor is observed. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effect of substitution of Si to Ge in CuGe1−xSixO3 single crystals has been studied by magnetic susceptibility, Cu nuclear magnetic resonance, and neutron scattering measurements. The phase diagram in the (x,T)-plane is characterized by an initial rapid decrease of the spin-Peierls temperature, TSP, on increasing x and by the occurrence of a three-dimensional long range ordered antiferromagnetic phase at T=TN in the range 0.005≤x≤0.05. This phase diagram is qualitatively discussed. The neutron scattering data for x=0.007 show that the dimerization which takes place below TSP is not suppressed below TN. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 4119-4120 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have carried out at 4-K spin-echo studies (of 55Mn, 63Cu) on sputtered Heusler alloy (Cu2MnAl) films with substrate temperature Ts in the range of 50–300 °C in order to obtain microscopic information on the magnetic structure. For Ts =60 °C a very broad spectrum is obtained, revealing incomplete (disordered) formation of Cu2MnAl. For Ts =158, 167, 170, and 210 °C, well-defined spectra are observed with Mn at 227 MHz and Cu at 241 and 259 MHz, respectively. Signal intensity studies reveal a maximum for Ts =167 °C in general agreement with the magnetization results of Morisako, Matsumoto, and Naoe. The signal frequencies are also in agreement with those obtained for the bulk alloy. For Ts =300 °C, the spectrum is broadened but the signal frequencies of Mn and Cu remain practically the same. This spectrum is also quantitatively different from that observed for the film with Ts=60 °C, where a low-frequency tail is observed. The effect of post-annealing the films is also presented.
    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 63 (1988), S. 2992-2994 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have prepared amorphous Fe40−xNi40Mnx B12Si8 ribbons by melt spinning and investigated them using magnetometry and spin echo spectrometry. The magnetization increases with the addition of Mn, by 17% for x=0.5. Such an increase is not observed for Ni concentration in less than 40. The NMR frequency of 55Mn at 4 K for x=0.5 is 380 MHz (μMn=3.3μB) and it decreases to 340 MHz for x=5.5. The Mn moments are found to be aligned ferromagnetically to that of the alloy. The presence of Mn also leads to an increase in the magnetic moment of Fe+Ni. After crystallization, one observes in the alloy with x=5.5, two 55Mn impurities in two different compounds. The former should be a canted antiferromagnet and the latter a normal ferromagnet. The temperature-dependence results are also discussed.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 62 (1987), S. 3328-3330 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The transverse susceptibility was measured in Co86Ti14 ferromagnetic thin films which possess an induced in-plane uniaxial anisotropy, as a function of a dc magnetic field H applied parallel to the hard axis. The susceptibility reaches a sharp maximum when H is close to the value of the anisotropy field HK previously determined. A theoretical model based upon a small deviation of H from the hard axis is developed to evaluate the angular dispersion of HK.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 63 (1993), S. 108-110 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The saturation magnetoresistance (MR) and Co nuclear magnetic resonance (NMR) spin echo have been measured in a series of sputtered Co/Cu multilayers, with Co thicknesses ranging from 10 to 30 A(ring). The multilayers were grown on 50 A(ring) Cu or Fe buffer layers. A clear correlation has been established between the MR and the Co NMR line profile. The sample with the highest MR exhibits a single fcc Co line with weak-intensity wings. Increasing the number of (111) layer stacking faults and grain boundaries leads to decreasing MR.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 61 (1992), S. 994-996 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Multilayered Co/Pt films with Co layer thickness ranging from 10 to 26 A(ring) have been studied by the NMR spin-echo method at 2 K. The rapid increase of the signal around 210 MHz as the Co layer thickness is decreased indicates the alloy formation at the interfaces. This signal coincides with the resonance spectrum of Co3Pt alloy. The latter corresponds to a disordered alloy and is coherent with the shifts of the satellite lines observed in a dilute alloy. The layer thickness of Co forming Co3Pt alloy at each interface is estimated to be about 4 A(ring).
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 69 (1996), S. 1160-1162 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Substitution of magnesium for manganese in mixed perovskite La1−xSrxMnO3was found to reduce the electrical conductivity and the Curie temperature Tc. A remarkable jump in the resistivity ρ was observed in the 6% Mg-doped crystal with x=0.175. This sample remains semiconducting at low temperatures, contrary to the Mg-free crystal. The abrupt change of ρ reflects a first-order structural transition at a temperature Ts just below Tc. An applied magnetic field decreased Ts, leading to an enhancement of the magnetoresistance between Ts (0) and Ts (H). The microscopic properties of Mn3+ and Mn4+ ions due to Sr2+and Mg2+ substitutions were illustrated by 55Mn nuclear magnetic resonance study. © 1996 American Institute of Physics.
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