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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 6901-6903 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Thin dysprosium c-axis films (40–400 A(ring)) were grown coherently between 500-A(ring) lutetium layers by molecular beam epitaxy. Bulk magnetization measurements show that these sandwich structures order magnetically at TN(approximately-equal-to)178 K (=TN of elemental Dy) and undergo ferromagnetic transitions at temperatures which range from 100 K (400 A(ring) Dy) to 175 K (40 A(ring) Dy), significantly enhanced from the bulk TC=85 K. The Dy basal plane lattice parameters in the films were determined by room-temperature x-ray diffraction. We observe a change in these values that correlates with the rise in TC, which suggests that this rise is due to epitaxial strain. The relatively small low-temperature magnetic susceptibility displayed by these samples indicates the presence of a large anisotropy in the basal plane. We address both the issues of the susceptibility and the high ferromagnetic transition temperature.
    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 73 (1993), S. 6904-6906 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have investigated magnetic order in superlattices of Dy and Sc grown along the hcp c axis by molecular beam epitaxy (MBE) techniques. Our neutron diffraction experiments reveal that individual Dy layers order ferromagnetically below Tc∼150 K. The magnetic coherence length along the growth direction is less than the Dy-layer thickness. Previous studies of rare-earth superlattices with Y or Lu as spacer layers have shown that magnetic coherence propagates through sufficiently thin nonmagnetic interlayers. This arises from the long-range exchange interaction that originates from nesting features in the Fermi surface of the spacer material. The lack of coupling in Dy/Sc superlattices reflects the very different Fermi surface of Sc, with much weaker nesting than Y and Lu.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A series of c-axis Er films ranging in thickness from 400 to 9500 A(ring) were grown on lutetium base layers to investigate the effects of epitaxial growth on the magnetic properties of bulk erbium. Neutron diffraction studies show that the basal plane lattice parameter of Er approaches the smaller Lu value as the films are made thinner. Below TN the phase angles of the Er spin modulation are diminished from bulk Er values in the thinner films. For all but two 800-A(ring) films, there is evidence from bulk magnetization and neutron data of a first-order transition to a conical ferromagnetic state, similar to bulk Er. These phenomena are compared to the properties of Er films grown on yttrium, whose basal plane spacing exceeds that of Er. In these systems the turn angles are greater than bulk and the ferromagnetic phase is suppressed. This contrasting behavior is consistent with predictions from a magnetoelastic energy model of epitaxial constraint developed to describe the Er/Y systems.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 6117-6117 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetoresistance (MR) measurements on four film samples of the ternary alloy CuNiCo were performed at room temperature in fields H≤20 kOe. Following growth by sputtering onto thermally oxidized Si substrates, the films (100–200 nm thick) were annealed between 1 and 6 h at temperatures TA=200, 350, 500, and 700 °C. The samples display anisotropic magnetoresistances (AMR) for H〈100 Oe of up to 3% at room temperature for Cu20Ni53Co27 (TA=350 °C). Despite the fact that in the bulk these alloys tend to phase separate into Co rich and Co poor regions, we find evidence for giant magnetoresistance (i.e., an isotopic negative component to the MR) in only one sample, Cu51Ni17Co31, after a 6 h, 700 °C anneal. In the as-deposited condition, samples Cu20Ni53Co27 and Cu13N41Co46 display a pronounced asymmetry between the resistance decrease for H applied perpendicular to the current I and the corresponding increase for H parallel to I which substantially exceeds the 1:2 ratio in bulk materials or the 1:1 ratio expected for a thin film. The large observed values of AMR (more evident in samples with low Cu concentrations) are likely linked to AMR in binary CuCo alloys, which are known to exhibit large AMR. The disparity between the MR for H parallel and perpendicular to the current we attribute to magnetic anisotropy induced during fabrication.
    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 76 (1994), S. 6209-6213 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Conflicting reports of large magnetoresistive and magnetoinductive effects in amorphous FeCoSiB wires and ribbons prompted the impedance measurements reported here. The spectra (0≤f≤3.2 MHz) were obtained at room temperature using a commercial impedance analyzer both as functions of axial magnetic field (−140〈HA〈140 Oe) and sense current (1≤Irms≤60 mA). The phase shift due to the test leads was carefully measured and subtracted from the raw data to resolve the spectra into resistive R(f ) and reactive X(f ) components. We find for the Fe4.3Co68.2Si12.5B15 wire (120 μm diameter) and ribbon (20 μm thick) that both R(f ) and X(f ) depend strongly on frequency and magnetic field. For HA=0, each component increases monotonically with frequency, with R(f=0)≈1 Ω/cm and X(f=0)=0. In high fields (HA=140 Oe), R(f ) and X(f ) are nearly frequency independent. The field-dependent response is sharply peaked about HA=0; the full width at half maximum is FWHM≤20 Oe, typically. The change in R(f ) and X(f ) between these two extremes is extraordinarily large; 4.5 Ω/cm at f=1 MHz is a typical value for the wire. The sensitivity of the magnetoresistive response is 44% of the dc resistance per Oe for f=1 MHz. Qualitatively similar phenomena were observed for the Fe7.5Co67.5Si15B10 ribbon, although the field and frequency dependences of the spectra are less pronounced than for the wire. We discuss a model which describes the spectra quantitatively, using classical electrodynamics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 64 (1994), S. 3652-3654 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The impedance of an amorphous Fe4.3Co68.2Si12.5B15 wire (100 μm diameter) exhibits an extraordinarily large frequency dependent resistance in addition to the previously reported frequency dependent wire reactance. The frequency response of both the resistance and reactance is almost entirely suppressed by an axial magnetic field HA〈150 Oe, resulting in a typical magnetoresistance for frequencies f〈1 MHz of the order of the dc wire resistance. The magnetoresistance at f=1 MHz is ΔR/Rsat=370%. As the bulk of the magnetic response occurs for HA〈5 Oe, this system shows great technological promise. We give a quantitative analysis of the phenomenon, which is rooted in classical electrodynamics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 68 (1996), S. 2753-2755 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The voltage V(t) induced by a sinusoidal drive current traversing a 125-μm-diameter BeCu wire plated with 1 μm NiFe is observed to be a very strong function of axial dc magnetic field. The basic physics of this phenomenon is explained classically in terms of Faraday's law of induction and Stoner–Wohlfarth magnetization reversal, which yield theoretical predictions that are in good agreement with experiment. For drive current amplitudes of the order of 100 mA, and frequencies of the order of 5 MHz, the field sensitivity dV/dH can be as large as 1 V/Oe (per cm of wire), which offers the potential for application in relatively simple, very high sensitivity magnetic field sensors. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 75 (1999), S. 250-252 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The asymmetric spin valve features a quiescent state in which the two ferromagnetic layers are antiparallel for any spacer thickness. It consists of AFM/FM/spacer/FM/AFM, where AFM is an antiferromagnet and FM is a ferromagnet. By cooling through the Néel temperature (TN) with a large current flowing, the FM layers are exchange biased in antiparallel directions. Current along is found to be sufficient to heat the device above TN. Devices with a 45 Å spacer layer were exchanged biased using a steady dc current which is turned down after T〉TN; devices with thinner spacer layers (20 and 30 Å) were destroyed by a steady dc current due to excessive heating. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Annals of the New York Academy of Sciences 669 (1992), S. 0 
    ISSN: 1749-6632
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Natural Sciences in General
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 6933-6933 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The soft magnetic properties of CoFe prompted an investigation of magnetoresistance in Co-Fe-Ag alloys. A series of (FeCo)xAg1−x (10〈x〈30) films were prepared by dc magnetron sputtering, followed by annealing in H2 at a variety of temperatures TA≤400 °C. The samples exhibit giant magnetoresistance (GMR) ratios which exceed 25% at a temperature of T=10 K, and 17% at T=300 K. The results of magnetization and x-ray scattering experiments indicate that FeCo alloy particles precipitate from the Ag matrix upon annealing. We note in particular that the full width at half maximum (FWHM) of the MR curves (approximately 2 kOe) is significantly less than that of Fe-Ag or Co-Ag sputtered films having comparable GMR ratios. We compare the sharp MR response of the (FeCo)xAg1−x system to that of heterogeneous (Ni80Fe20)xAg1−x films.
    Type of Medium: Electronic Resource
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