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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Measurements of the polar Kerr rotation and optical coercivity as a function of photon energy have been made on ≈2 μm thick ThMn12-type crystalline sputtered films of Sm(Fe,Ti)12. The optical coercivity for a Ti containing (222) textured film was 3.10 kOe at a photon energy of 1.25 eV, 2.96 kOe at 1.84 eV, and 2.92 kOe at 2.45 eV. The optical coercivity for a similar composition (002) textured Sm(Fe,Ti)12 film was relatively constant at 1.24 kOe. These samples were measured in air at 300 K without any protective overcoating. The polar Kerr rotation observed for these crystalline films versus the photon energy paralleled that observed for pure Fe. The magnetometer and optical coercivities for the (222) textured Sm(Fe,Ti)12 films were 1.5 and 2.5 times as large, respectively, as for similar composition (002) textured films. Differences in grain sizes incorporated during the direct synthesis of the films onto heated substrates are needed to account for the large differences observed in the coercivities for the (222) versus (002) textured films.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 70 (1991), S. 6386-6388 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Films of EuS have been doped with up to 34-at. % Tb by coevaporation. From lattice constant measurements we conclude that the films are defect rocksalt structure solid solutions with the general formula Eu1−xTbxS1−y(D'Alembertian)y, where (D'Alembertian) represents a vacancy. The magnetic properties change drastically between undoped films and the Tb substituted samples. The Curie point increases from 20 to about 135 K and the coercivity increases from 60 Oe to about 4 kOe in the x=0.34 sample. Our measurements indicate an increase in RKKY exchange because of the higher carrier concentration caused by Tb doping. The increased carrier density causes a decrease in resistivity of at least two orders of magnitude to about 10−3 Ω cm, the same order of magnitude as reported for bulk solid solutions of EuS-GdS. The peaks in the magneto-optic Kerr spectrum of EuS at about 2 eV are decreased in amplitude, broadened and shifted in energy with Tb doping.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 6109-6111 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Rocksalt structure solid solutions were prepared by coevaporating Eu2O3 and Tb metal. The films have the general formula Eu1−xTbxO1−y(D'Alembertian)y where y, the oxygen vacancy fraction, is given by y=(3x−1)/2. We have also prepared Tb-doped EuS solid solutions where y(approximately-equal-to)x so we can compare the effects of anion vacancies in both the oxide and sulfide systems. The coercivity, Hc, increases rapidly with Tb doping at about x=0.15 in the sulfide system and x=0.45 in the oxide system. The Hc of both systems falls on a universal curve, however, when plotted vs vacancies/RE ((D'Alembertian)/RE) with the rapid increase occurring at (D'Alembertian)/RE=0.15. This value is close to 1/6 (0.166) which in octahedral coordination corresponds to one anion vacancy/RE. This suggests that the near neighbor vacancy is producing a strong crystal field at the Tb site which causes strong single ion anisotropy and thus a high coercivity. The MO spectra of the oxides show a strong dependence on x. At x=0.25, peaks are observed at 1.5 eV (−3°), 2.2 eV (5.5°), and 2.7 eV (−2°). At x=0.33, the spectra change completely. A narrow peak with a rotation θK=−20° appears at 2.5 eV, dominating the spectrum. The reflectivity, R, goes through a sharp minimum at the same energy (R〈1%), possibly causing the enhancement in θK.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 70 (1991), S. 5855-5857 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Amorphous thin films of UxAs100−x are ferromagnetic for U-rich compositions, 49≤x≤75, with a magnetic moment of 0.2 to 0.4 μB per U atom and Curie temperatures, Tc, up to 120 K. Large resistivities are found at 5 K for compositions x〈51, indicating semiconducting properties for low U content. For the highest Tc, the anomalous Hall angle is θH = 12° and the anomalous Hall coefficient is RS ≈ 10−7 Ω cm/G. Maximum polar Kerr rotation for U62As38 is −2.0° at 1-eV photon energy. The properties of U-As amorphous films are similar in many respects to those of amorphous U-Sb, except that the maximum values of these properties occur at higher U contents. The results are discussed in terms of spin-orbit interactions.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 4750-4755 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Amorphous U-Sb alloys in the vicinity of the composition U3Sb4 have magneto-optic Faraday rotations of + 2 × 106 deg/cm. This is the highest rotation of any amorphous ferromagnetic material. These alloys also have relatively high Curie temperatures of about 140 K with magnetic moments per uranium of up to 1.4μB. These properties are unexpected since it is known from intermetallic compounds that U atoms must be isolated from each other in order to develop a magnetic moment. In a concentrated random amorphous alloy, no magnetic moment on the uranium would be expected because of the high probability of uranium near neighbors. In the U-Sb amorphous alloys, however, there appears to be chemical short-range order which tends to favor Sb nearest neighbors for uranium. The amorphous U-Sb alloys have Kerr rotations of about −3°. This value is comparable in magnitude but opposite in sign to that of the single-crystal rock salt compound USb in the visible. In these amorphous alloys the Hall angle from the spontaneous Hall effect can be as much as 17°. Similar large magneto-optic and Hall coefficients have also been found in amorphous U-Bi, U-Sb-Mn, and U-Sb-Co alloys.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 4784-4786 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Multilayers of Co and Au with perpendicular hysteresis loop squareness ratios of ∼1 have been prepared by e-beam evaporation. These films have perpendicular anisotropy in the as-deposited condition in contrast to other work in which Co/Au multilayers, prepared by ion beam sputtering, showed perpendicular anisotropy only after annealing at 300 °C. The Faraday rotation of these square-loop multilayers is about 9×105 deg/cm of Co or 1×105 deg/cm of total thickness at a wavelength of 633 nm. These values indicate an enhancement of the Faraday rotation of Co at this wavelength by about a factor of 2. This may be a plasma-edge enhancement effect similar to that reported by Katayama et al. [Phys. Rev. Lett. 60, 1426 (1988)] in the Kerr effect of Fe/Au multilayers.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 6285-6285 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Permalloy has been widely studied and used in industry for magnetic recording heads and sensors. This article presents a study of the magnetoresistance of (NiFe/Au)n multilayer films and NiFe/Au/NiFe sandwich structures. Gold is used as the spacer layer because of its low solid solubility in NiFe and the tendency of NiFe and Au to phase separate. Films were grown by dc sputtering with a series of different permalloy and Au thickness. In the multilayer films, the thickness of permalloy varies from 20 to 40 A(ring) and Au varies from 8 to 25 A(ring). A difference in the sign and magnitude of magnetoresistance for transverse and longitudinal field directions with respect to current indicates the presence of anisotropic magnetoresistance (AMR) effect. The magnitude of Δρ/ρ is small because of shunting by Au layers. In the sandwich structures, the thickness of permalloy layers is different on each side of the Au and varies from 150 to 800 A(ring). The Au spacer layer varies from 20 to 60 A(ring). The measurements show mainly anisotropic magnetoresistance. There was a small opposite jump at ∼8 Oe on resistivity measurement, which indicates spin valve effect superimposed on the AMR effect. After annealing, the change in magnetoresistance is much more sensitive in low field ∼15 Oe, a property which is critical to many applications. © 1996 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 5253-5255 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The phase equilibria in the system Co–Mn–Sn have been studied with compositions along the join Co–CoMnSn. This is part of an effort to form a macroscopic ferrimagnet with two metallic ferromagnetic phases, Co and Co2MnSn. As-cast arc melted alloys have been made with Co compositions from 33 to 78 at. %. Three different phase and magnetization regions are observed with increasing Co composition. Cobalt becomes the primary phase at more than 71 at. % Co and crystallizes out of a Co2MnSn rich matrix. It is shown from x-ray diffraction analysis and the Tc change with Co compositions that the Co phase in Co2MnSn matrix is probably a Co–Mn solid solution. From the break in the magnetization vs temperature curves of two phase magnets with two different compositions, Curie temperatures are determined as approximately 160 °C and 175 °C for the Co–Mn solid solution phase. The exchange coupling at phase boundary is proposed by the analysis of coercivity vs temperature data. © 1996 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 5929-5931 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Polar Kerr-rotation spectra and hysteresis loops have been measured in Co1−x−yTbx(EuS)y, with 0≤x≤0.21 and 0≤y≤0.21, and compared to the macroscopic ferrimagnet Co1−y(EuS)y and to amorphous Co1−xTbx. The measurements were taken at room temperature and at 7 K over a wide photon energy range of 1.1–4.6 eV in fields up to 2.77 T. The addition of Tb retains the phase-separated nature yielding a material consisting of a Co–Tb matrix containing crystalline EuS precipitate particles with about 2 nm diameter. Up to 8% Tb is substituted for Eu in the EuS phase. The Kerr rotations are rather small reaching −0.25° at room temperature and increasing to −0.85° at 7 K, i.e., no optical enhancement is observed as in Co(EuS). This is most likely due to the much smaller size of the EuS crystallites. An "s''-shaped feature in the Kerr-rotation spectra can be assigned to an Eu2+ 4f→5d transition while a contribution from the Tb3+-4f states shows up as a decrease with increasing photon energies. At 7 K, the Tb and Eu magnetic moments are found to be parallel while the Co moment is believed to be antiferromagnetically exchange coupled to both. At room temperature, the Co moment is dominating the Tb moment which is antiferromagnetically coupled as in Co1−xTbx. © 1996 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 6025-6027 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Impregnating transition metallic compounds into porous glass is a simple way to form ultrafine particles in a glass matrix. In our studies, ultrafine particles were prepared by impregnating Fe compounds into porous glasses (pore size 70±21 A(ring)) and annealing. After annealing, the samples were studied at different temperatures with a vibrating sample magnetometer. In the annealed glasses two types of particles were formed: (a) superparamagnetic particles and (b) ferromagnetic particles with exceedingly high coercivity (Hc=13 kOe at 298 K). The ratio between superparamagnetic and high coercivity particles depends on the annealing temperature and time. In samples annealed at lower temperatures or at high temperature for short times, only superparamagnetic particles were found. In those annealed at high temperatures after certain times, only high coercivity particles were found. It was also found that the blocking temperature TB of the high coercivity particles depends on the annealing process. Moreover it was found that the Curie temperature of the high coercivity particles is below 520 K. © 1996 American Institute of Physics.
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