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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 4512-4515 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ferromagnetic resonance (FMR) and high field effective (HFE) linewidth measurements have been made at 10–90 GHz for low conductivity Mn substituted single crystal barium ferrite, BaFe12−xMnxO19, with x=0.1. The manganese compensates excess Fe2+ and reduces conductivity. Measurements were made on c-plane thin disks magnetized to saturation along the disk axis. A shorted waveguide technique was used to measure the FMR profiles and linewidths in the 55–90 GHz frequency range. High Q cavity techniques and an analysis procedure for the FMR high field tail response were used for the HFE linewidth determinations in the 10–60 GHz frequency range. The FMR linewidths increase linearly with frequency at 0.3 Oe/GHz and have a zero frequency intercept of 20 Oe. The HFE linewidths increase linearly with frequency at 0.4 Oe/GHz and have a zero frequency extrapolation of 4 Oe. This lower zero frequency extrapolation for the HFE linewidth supports an inhomogeneity origin for the 20 Oe FMR linewidth extrapolation. These data indicate intrinsic linewidths for barium ferrite of 0.3–0.4 Oe/GHz, a factor of 6–8 larger than intrinsic linewidths in single crystal yttrium iron garnet.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 74 (1993), S. 1218-1228 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Butterfly curves of the subsidiary absorption spin wave instability threshold microwave field amplitude versus static field have been measured at 10 GHz on a 12.8-μm-thick single crystal yttrium iron garnet film for two field configurations, one with the static magnetic field in plane and the microwave field out of plane (IP case) and the other with the static field normal to the film plane and the microwave field in plane (PI case). The results for the IP case are similar to earlier results which show a "kink'' in the butterfly curve accompanied by a jump of the critical mode wave number k at the kink field. For the PI case, however, there is no observed kink effect. The different butterfly curves for the IP and PI cases are explained on the basis of a new theory for thin films which takes into account the discrete standing wave modes in the film. For the IP case, the theory yields critical modes with wave vectors in the film plane and the kink effect as before. For the PI case, the critical modes have wave vector k components perpendicular to the film plane, the minimum threshold critical modes are modified significantly, and the theory yields smooth butterfly curves with no kink. Quantitative fits to the data were obtained, based on a single trial function for the k-dependent spin wave linewidth.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5987-5987 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Brillouin light scattering (BLS) was used to measure magnon frequency versus in-plane field H and in-plane wave vector for a Fe(38 A(ring))/Cr(13 A(ring))/Fe(38 A(ring)) thin film. Both easy [100] and hard [110] field directions were used. The in-plane wave vector was perpendicular to the field. The data were obtained with a high contrast multipass tandem 3+3 Sandercock Fabry–Perot interferometer, with a free spectral range of 30 GHz. The results were correlated with previous hysteresis measurements.1 In the low field region (H〈200 Oe), the magnon frequency decreases with increasing field in a manner consistent with soft mode behavior. The mode frequency in this low field region is slightly different on the Stokes (S) and anti-Stokes (AS) sides of the BLS spectra. At fields of 150–200 Oe one sees a cusp-like minimum in the magnon frequency field dependence. The S and AS frequencies also converge at this point. This is evidence for the antiparallel alignment of the two magnetizations of the Fe layers and the onset of canting.2 At higher fields (250–350 Oe) one sees a jump in frequency, followed by an apparent approach to saturation, and a further increase above 2 kOe. This behavior is basically the same for both field directions, but the frequencies are downshifted somewhat for the hard [110] direction. The wave-number k dependence is weak in the low field region. Above the jump, the magnon frequency shows a distinct increase with k. The substantial frequency increase with field above 2 kOe may indicate conversion to a surface mode character. This is consistent with the k dependence seen at high fields.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 5721-5723 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A Brillouin light-scattering study of surface magnons in permalloy thin films shows a distinct oscillation in the Stokes–anti-Stokes intensity ratio as a function of the in-plane wave number in the 0– 2.5×105 cm−1 range. This result differs from the previously reported monotonic dependence for thin iron thin films.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 1569-1573 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Subsidiary absorption butterfly curves of spin-wave instability threshold versus static in-plane field have been obtained for yttrium iron garnet (YIG) thin films at 3 GHz. The butterfly curves have been found to be rather anomalous, typically displaying a pronounced dip and a very low minimum threshold. These anomalous features are attributed to the overlap of the subsidiary absorption field region with ferromagnetic resonance (FMR). First-order instability theory was extended to include the uniform mode response near FMR. The extended theory yields good fits to the data for reasonable values of the YIG FMR linewidths. The theoretical analysis also shows a predicted flip in the azimuthal propagation angle φk for the unstable spin waves in the region of FMR overlap. With increasing field, there are predicted discontinuous changes in φk from 90° to 0° and back to 90° in the region of FMR.
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  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A simple technique to analyze the effective linewidth at high field, corresponding to the far field tail of ferromagnetic resonance (FMR) absorption, was recently reported. This technique has now been applied at 10, 20, and 35 GHz to single crystal Zn2Y hexagonal ferrite with planar anisotropy. Far field effective linewidth (ΔHeffFF) measurements were made for a series of 2–3 mm-diam, 0.08–1.33-mm-thick c-plane disks. The ΔHeffFF is taken to represent the intrinsic linewidth, in the sense that there are no two magnon or inhomogeneous linebroadening contributions to the losses on the far-field FMR tail. ΔHeffFF at each frequency increases with the square of the disk thickness. This increase is consistent with an eddy current loss process. A fit of the data to a simple eddy current model yields resistivities of 10.3, 9.7, and 8.3 Ω cm at 10, 20, and 35 GHz, respectively. These values are consistent with a resistivity of 2 Ω cm from 10 GHz dielectric measurements and 20 Ω cm from the resistivity measurements.These results are similar to previous results for barium ferrite. However, the microwave response in these Zn2Y materials also shows many anomalies. First, ΔHeffFF is larger, not smaller, than the corresponding FMR linewidth. Second, ΔHeffFF also depends on the orientation of the microwave field relative to the crystallographic c plane. The losses for out-of-plane microwave pumping are larger by a factor of 2–3 than for in-plane pumping. Research sponsored by the United States Office of Naval Research, Contract N00014-90-J-4078. The single crystal samples were kindly provided by M. A. Wittenauer, Purdue University.
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  • 7
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The frequency dependence of the ferromagnetic resonance (FMR) linewidth and effective linewidth has been measured in Mn doped single crystal barium hexaferrite (BaFe12−xMnxO19) with x=0.1. Mn doped samples were used to minimize conductivity losses. Measurements were made on c-plane thin disks magnetized to saturation along the disk axis and c direction. A shorted waveguide technique was used to measure the FMR profiles in the range of 55–90 GHz. The FMR field position increased linearly at 0.35 kOe/GHz, with a zero field extrapolation of 34.7 GHz as expected for uniform mode FMR in barium ferrite. The linewidth ΔH increased linearly with frequency at 0.29 Oe/GHz with a zero frequency extrapolation of 18 Oe. A high-Q cavity method was used to measure the high field effective linewidth, ΔHeffFF at 10, 20, 35, and 60 GHz. The effective linewidth increased linearly with frequency at 0.4 Oe/GHz, with a zero frequency extrapolation of 4 Oe. There were no dependencies of ΔH or ΔHeffFF on sample thickness. These results indicate that (1) eddy current contributions to ΔH and ΔHeffFF in these Mn doped barium ferrite materials are absent, (2) ΔHeffFF is significantly lower than ΔH and appears to be a good measure of the intrinsic losses, and (3) both linewidths increase linearly with frequency at about the same rate.These intrinsic linewidths in barium ferrite are still significantly greater than linewidths in yttrium iron garnet. Research sponsored in part by the United States Office of Naval Research, Contract No. N00014-90-J-4078. The single crystal samples were kindly provided by M. A. Wittenauer, Purdue University.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 5521-5523 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An effective linewidth technique for characterizing microwave losses in thin ferromagnetic metal films, similar to the technique for ferrites, has been developed. The extension to metal films is nontrivial. A numerical solution of the electromagnetic boundary value problem for the fields inside the film must be used to evaluate the on- and off-resonance losses, and these calculated losses must be directly related to changes in the microwave cavity Q on an absolute scale. Specific measurements and analyses were done for polycrystalline permalloy on glass. Measurements at 10 GHz yield a change in 1/Q with field which is in accord with theory and can be modeled off resonance to obtain intrinsic losses. The analysis yielded an intrinsic Landau–Lifshitz damping parameter of 5.5×107 rad/s for permalloy. This corresponds to a half-power effective linewidth of 27 Oe, which is comparable to the best published 10 GHz linewidth for single-crystal iron films.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 63 (1992), S. 3156-3166 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: An inexpensive alternative to commercial high-power microwave pulse generators is described. The present high-power microwave pulse generator utilizes a surplus MIT model 3 Mark II hard tube modulator and 2J51 magnetron. The basic design and technical details of the pulse generator are presented. The pulse generator is designed to produce 8.5–9.6 GHz pulses with pulse lengths ranging from 2 to 4 μs, with a nominal power output of 20 kW and a maximum duty cycle of 0.001.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 80 (1996), S. 3962-3971 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Combined Brillouin light-scattering (BLS) and microwave pumping techniques were used to measure the second-order spin-wave instability threshold microwave field amplitudes and characterize the critical modes for ferromagnetic resonance (FMR) saturation in 4.15 μm-thick yttrium iron garnet films at 8.47 GHz with the static magnetic field in-plane. To the best of our knowledge, this work represents the first BLS measurements for second-order FMR saturation processes in ferrite materials. Several new results were obtained: (1) A new type of butterfly curve for second-order processes. (2) Strong scattering from modes at low wave numbers in the 104 rad/cm range. (3) An observed in-plane propagation direction for these low wave number modes at 90° to the in-plane static field direction. These results differ significantly from the behavior expected from the bulk sample instability theories of Suhl and Schlömann, which predict critical modes at wave numbers and propagation directions in the 105–106 rad/cm and 0° ranges, respectively, and a sharp cusplike response centered at FMR. These results indicate that significant modifications of the bulk theory, which take into account the real modes supported by the film, are needed to realistically model second-order instability processes in films. © 1996 American Institute of Physics.
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