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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 6695-6697 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ferromagnetic resonance (FMR) was observed in epitaxial thin films of CrO2 grown on TiO2. FMR spectra were taken at 9.5 and 35 GHz and at temperatures from 4 K to above the ordering temperature of 393 K. The spectra of these films are generally complicated because of surface roughness and the distribution of stresses and anisotropies through their thickness. The thinnest films, however, display typical spin wave spectra, which could be approximated using uniform magnetic material analyses. The exchange constant at 300 K, D∼70 meV Å2, is consistent with values derived from the temperature dependence of M at low temperatures. The temperature dependence of D was extracted from the spin wave spacing and is similar to other magnetic metals. Our data indicate a room temperature Gilbert damping parameter of at most 0.0023 near 300 K, which is less than those of metallic magnetic materials except possibly Fe. The small damping parameter suggests that intrinsic losses seen in other magnetic metals, which may arise from electronic transitions between bands of different spin character, are small in CrO2. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 79 (2001), S. 4396-4398 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic, structural, and transport properties of the Heusler alloy Co2MnSi are reported for sputtered thin films and a single crystal. X-ray diffraction reveals a phase pure L21 structure for all films grown between 573 and 773 K. Films grown at 773 K display a four-fold decrease in the resistivity relative to those grown at lower temperatures and a corresponding 30% increase in the residual resistivity ratio (ρ300 K/ρ5 K). We show that the higher growth temperature results in lattice constants, room temperature resistivities, and magnetic properties that are comparable to that of the bulk single crystal. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 83 (1998), S. 4848-4854 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The interlayer coupling, domain structure, and microstructure of ion beam sputtered multilayers, were investigated by magnetization, optical microscopy using magnetic colloids, small and wide angle x-ray scattering, and atomic force microscopy measurements. The study focused on multilayers that were composed of ten repeats of Co(1.5 nm)/Cu(tCu)/permalloy(2.6 nm)/Cu(tCu) with tCu=2.6 and 5.0 nm. The top surface rms roughness of the multilayers was 0.31 and 0.96 nm for samples with tCu=2.6 and 5.0 nm, respectively. The maximum peak to peak roughness in a 1 μm2 scan was 3.0 and 8.9 nm for samples with tCu=2.6 and 5.0 nm, respectively. The lateral feature size was 30–40 nm and 70 nm for samples with tCu=2.6 and 5.0 nm, respectively. The multilayers with tCu=2.6 had sharper, flatter interfaces than those with tCu=5.0 nm. Magnetization measurements and the domain structure at room temperature showed that when tCu=2.6 nm the Co and permalloy layers were ferromagnetically coupled, while if tCu=5.0 nm, the Co and permalloy layers were largely uncoupled. Twin walls present for tCu=2.6 nm clearly indicated locked-in domains of the ferromagnetically coupled Co and permalloy layers; for tCu=5.0 nm, such coupled wall structures were almost nonexistent. Modeling the magnetization, it is estimated that the ferromagnetic coupling only has to be greater than 0.0047 mJ/m2 for the Co and permalloy layer magnetizations to be nearly parallel at all field values. Since not much coupling is needed, the coupling in the samples with tCu=2.6 nm could be due to the magnetostatic coupling which exists even in perfectly flat films or to the magnetostatic coupling of surface magnetic dipoles created by roughness. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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