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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 1302-1309 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Epitaxial {111} Ni0.82Fe0.18O films (NiFeO) were prepared by using solid-source metal-organic chemical vapor deposition on {0001} α-Al2O3. The exchange anisotropy between NiFeO and Ni80Fe20 (NiFe) was investigated. Structural and chemical analyses showed that NiFeO films were compositionally homogeneous. The 60-degree rotational twins formed in the NiFeO films. The epitaxial relationship between Ni0.82Fe0.18O and Al2O3 is the following: [111] NiFeO||[0001]α-Al2O3, [11¯0]NiFeO||[11¯00]α-Al2O3, and [112¯]NiFeO||[112¯0]α-Al2O3. The orientation relationship between NiFeO and NiFe is cube-to-cube. Misfit dislocations pile up at the interfaces significantly reduce the stress, and result in semi-coherent interfaces. In-plane tension and out-of-plane compression were developed in NiFeO films due to the thermal stress, which may force the magnetic moment of NiFeO to lie in the {111} planes parallel to the film surface, and may lead to a strong interfacial coupling between NiFeO and NiFe. The relative small exchange field possibly results from (1) a low anisotropy energy compared to the interfacial coupling energy in the NiFeO {111} plane, (2) an orientation distribution of the easy axes in the NiFeO {111} plane, and (3) the large domain size of NiFeO. The Malozemoff model was used to estimate the exchange field in this system. Based on the assumption that the domain size of the NiFeO is approximately equal to the twin size, the calculated exchange field agrees well with the experimental results. © 2001 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 6603-6605 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In-plane magnetic anisotropy was studied in Co films epitaxially grown on NiMn (001) films. The hysteresis loops measured in-plane perpendicular to the exchange field show double shifted loops, and the magnetization of Co to rotate coherently. Magnetic anisotropy constants can be determined from these double shifted loops. Exchange coupling in NiMn/Co not only induces a unidirectional anisotropy but also a uniaxial anisotropy. This induced uniaxial anisotropy may contribute to the enhancement of Co coercivity. © 2001 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 6928-6930 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetoresistance (MR) ratio is enhanced by 35% by inserting the nano-oxide layer (NOL) at the Ta/Co interface in the FeMn-based top spin valves (Ta/NOL/Co/Cu/Co/FeMn/Ta). The enhancement is attributed to specular reflection, resulting in a large resistance change and small sheet resistance. However, the formation of NOL at the interface of Ta/Co suppresses the (111) texture, resulting in small exchange fields. Top spin valves with NOLs show good thermal stability up to 200 °C annealing. The MR ratio is further increased after annealing at temperatures below 200 °C. Enhancement of the MR ratio by 61% can be achieved by annealing at 150 °C. For bottom spin valves (Ta/NiFe/FeMn/Co/Cu/NiFe/Ta), NOLs formed at FeMn/Co and NiFe/Ta interfaces increase MR ratios, but NOLs at Co/Cu or Cu/NiFe deteriorate the differential spin scattering and significantly reduce MR ratios. © 2001 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 7124-7126 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Spin valves composed of ferrimagnetic/Cu/ferrimagnetic layers were fabricated with the magnetization perpendicular to the film planes. By changing the composition of ferrimagnetic layers, both negative and positive giant magnetoresistance (GMR) can be observed in ferrimagnetic spin valves. For samples consisting of both transition-metal (TM-) rich TbFeCo and GdFeCo, negative GMR values were obtained. Due to the high resistivity of amorphous ferrimagnetic films, the shunting effect of Cu led to relatively small MR ratio. The negative MR effect was 1% for 1.7 nm Cu. For spin valves consisting of rare-earth (RE-)rich TbFeCo and TM-rich GdFeCo, positive GMR values were observed. A thin layer of Co was inserted between RE-rich TbFeCo and Cu to manipulate the sign of GMR. © 2001 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 7537-7539 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The exchange field and domain configurations were investigated in patterned polycrystalline and (100) NiO/NiFe films. The exchange field was enhanced in the polycrystalline patterns with the aspect ratio larger than one (the long edge parallel to the original easy axis). Exchange field of patterned (100) NiO/NiFe on MgO, in contrast, showed little dependence on the aspect ratio, but strong dependence on the pattern size. The exchange field increased from 8.6 Oe in the sheet film to 48.4 Oe in the 2 μm patterns. The different dependence of the exchange field of polycrystalline and (100) NiO/NiFe on the pattern size can be plausibly explained by the difference of the domain size in NiO, and the variation of the blocking temperature distribution. Magnetic force microscopy images of patterned polycrystalline NiO/NiFe showed two kinds of domain configurations (single-domain state and multidomain state) in the sample with the pattern size of 2 μm, which may be the direct observation of various exchange paths at the interface of NiO/NiFe. © 2001 American Institute of Physics.
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  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have grown epitaxial NiO {111} films of thicknesses ranging from 60 to 1200 A(ring), deposited 45 A(ring) NiFe films on these NiO substrates, and made measurements of exchange field and coercivity, of the effective uniaxial anisotropy, of rotational hysteresis, and of the training effect on these films. We find that the large coercive fields, ∼500 Oe, observed in these epitaxial systems can be understood using a model in which the magnetization reversal process is by rotation, with the coercive field determined by the effective uniaxial anisotropy of the system. This effective anisotropy is in turn determined by the anisotropy of the NiO and depends on NiO thickness. © 1996 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 81 (1997), S. 4990-4992 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Fe-doped NiO polycrystalline and {111} epitaxial films were grown by solid-source metalorganic chemical vapor deposition. The exchange field for NiFe on the polycrystalline Fe-doped NiO films increased with Fe content up to 18 at. % Fe, and then decreased with further increases in Fe content; the coercivity, blocking temperature, and grain size monotonically decreased with increasing Fe content. Similar results were observed in {111} films. The increase of the exchange field and the reduction of the blocking temperature are attributed to dissolved Fe atoms in the NiO. Low exchange coupling between NiFe and α-Fe2O3 may be responsible for the decrease of the exchange field in highly Fe-doped NiO films. Furthermore, 18% Fe-doped NiO showed an enhancement of exchange fields at thicknesses between 450 and 950 Å, and a considerable large training effect was observed. © 1997 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 83 (1998), S. 6816-6818 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ni0.82Fe0.18O{100} epitaxial films, ranging in thickness from 70 to 1200 Å, were grown by solid-source metal-organic chemical vapor deposition. The exchange field for 45 Å Ni80Fe20 on Ni0.82Fe0.18O films reached 250 Oe at 200 Å Ni0.82Fe0.18O and then stayed almost constant with increasing thickness of Ni0.82Fe0.18O. Furthermore, the coercivity for those films is only 55 Oe. The high exchange field and the low coercivity are attributable to the high in-plane anisotropy of Ni0.82Fe0.18O{100} and the uncompensated spins in the interface of Ni0.82Fe0.18O/Ni80Fe20. The blocking temperature of these films is 180 °C, lower than that of NiO/Ni80Fe20 (∼220 °C). The reduction of the blocking temperature may result from local Fe–O–Fe or Fe–O–Ni bonding, which loses the superexchange interaction at a lower temperature than the blocking temperature of NiO. © 1998 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 6600-6602 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The correlation between the exchange field of NiFe/NiMn and the phase transformation of NiMn was investigated. Transmission electron microscopy (TEM) dark-field images, contributed by the order phase of NiMn, were used to identify the location and volume fraction of the order phase. TEM selected area diffraction patterns showed the (110) superlattice diffraction rings of NiMn, verifying the existence of the order phase in the annealed samples. The order volume fraction can be calculated by the dark field image contributed by the (110) diffraction. The exchange field increased almost linearly with increasing order volume fraction. Energy dispersive x-ray spectroscopy attached to TEM indicated that Mn diffused into NiFe for annealing at 280 °C, leading to a larger coercivity and small coercivity squareness. Part of the NiMn still maintains the paramagnetic phase even after annealing at 280 °C. © 2001 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 87 (2000), S. 6656-6658 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Samples with the structure Mo (20 nm)/NiFe (t nm)/NiFeMn (12 nm)/Mo (2 nm) were grown on the Al2O3 (11–20) substrates by a MBE system. Although no magnetic field was applied during depositions, shifted hysteresis loops were observed in as-deposited samples, which were attributable to the stress-induced exchange anisotropy. With increasing thickness of NiFe, the residual stress on NiFe decreased, which resulted in the decrease of NiFe anisotropy. The exchange field decreased with increasing NiFe thickness but with a transition point at t=12nm, at which the residual stress on top of NiFe might be significantly released. © 2000 American Institute of Physics.
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