Chapter 9. Novel Magnetic Phenomena
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T. Ikeda, H. Fujioka, K. Ono, M. Oshima, H. Akinaga, M. Yoshimoto, H. ...
1999 Volume 23 Issue 1_2 Pages
685-687
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We have grown ferromagnetic MnSb thin films on (111), (110), and (100) Mn-Zn ferrite substrates by molecular beam epitaxy (MBE). Epitaxial monocrystalline MnSb films with the growth plane of (0001) have been obtained on the (111) Mn-Zn ferrite substrates. The MnSb epitaxial films have shown in-plane alignment of [11-20] MnSb // [1-10] Mn-Zn ferrite. On the other hand, polycrystalline MnSb growth has been observed on (110) and (100) Mn-Zn ferrite substrates even under the same growth conditions.
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K. Ono, T. Uragami, M. Mizuguchi, H. Fujioka, M. Oshima, M. Tanaka, H. ...
1999 Volume 23 Issue 1_2 Pages
688-690
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We have successfully grown manganese pnictides epitaxial multilayers [MnSb/MnAs]5 on GaAs by molecular beam epitaxy. The structural and magnetic properties of the multilayers have been investigated by reflection high energy electron diffraction, X-ray diffraction, and superconducting quantum interference device.
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K. Ono, M. Mizuguchi, T. Uragami, T. Mano, H. Fujioka, M. Oshima, M. T ...
1999 Volume 23 Issue 1_2 Pages
691-693
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We report the formation of nanosize ferromagnetic MnAs dots on S-passivated GaAs by molecular beam epitaxy. The structural and magnetic properties of the dots have been characterized by high resolution scanning electron microscopy, and superconducting quantum interference device magnetometer. The average size and the density of these MnAs dots were 16.3nm and 2.3×10
10/cm
3 respectively. These dots show ferromagnetism at low temperature and the Curie temperature is lower than the bulk value.
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T. Uragami, K. Ono, M. Mizuguchi, T. Mano, H. Fujioka, M. Oshima, M. T ...
1999 Volume 23 Issue 1_2 Pages
694-696
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We have grown ferromagnetic MnAs thin films on S- and Se-passivated GaAs substrates by molecular beam epitaxy (MBE). Growth modes of MnAs films on GaAs(100) substrates were changed by the surface treatment. We found that on the clean and the Se-passivated surfaces, MnAs films grow by a layer-by-layer mode. In contrast, on the S-passivated surface MnAs grows by an island growth mode. and polycrystalline films are obtained. We also found that the magnetization of the MnAs film on Se-passivated surface is larger than that on clean and S-passivated surfaces
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K. Motohashi, T. Ono, T. Hinoue, H. Miyajima
1999 Volume 23 Issue 1_2 Pages
697-699
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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Magnetic properties of ferromagnetic and superconducting hybrid films were investigated. The magnetization process of the hybrid films exhibits peculiar behavior which suggests the existence of the magnetostatic interaction between the ferromagnetic and the superconducting layers.
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A. Kirilyuk, V. Mathet, P. Beauvillain, Th. Rasing
1999 Volume 23 Issue 1_2 Pages
700-702
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We report a detailed study of the nonlinear magneto-optical response from wedge-shaped (111)-oriented films of noble metals Cu, Au and Ag grown on top of an ultra thin Co film. The spectral dependencies of the oscillatory part of the total optical second harmonic response indicate a dominating role of the free-electron contribution in the optical response from quantum well states.
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E. E. Shalyguina, N. I. Tsidaeva, I. A. Pogrebnaya, O. A. Shalyguina, ...
1999 Volume 23 Issue 1_2 Pages
703-705
Published: January 20, 1999
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The investigation of Cu-thickness dependence of magnetic and magneto-optical properties f Au/Cu-wedge/NiFe sandwiches were performed with help of the magneto-optical method with micron resolution. It was discovered that the magnitude of the transverse Kerr effect (TKE) oscillates, as Cu-wedge thickness is variable. It was found the period of these oscillations is equal to ∼ 6Å. It was proved that TKE oscillations are caused by the influence of finite-size effect.
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Chapter 10. Novel Scientific Instrumentation & Processing
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Valentin Kottler, Noureddine Essaidi, Yong Chen, Claude Chappert
1999 Volume 23 Issue 1_2 Pages
706-711
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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An apparatus combining various scanning probe microscopy techniques is presented. It is dedicated to near-field magneto-optical (MO) and optical transmission imaging, and simultaneously gives topographical information. This MO scanning near-field optical microscope (SNOM), working in transmission-collection mode, measures the magneto-optical circular dichroism (MOCD) effect of the samples, using a tapered and metal-coated optical fiber probe. The performance of the apparatus is mainly determined by this fiber probe. Resolution of about 200 nm was obtained on 200 Å thick Co/Pt and CoNi/Pt multilayer samples. MOCD-SNOM imaging artifacts are presented and discussed.
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T. Ishibashi, T. Yoshida, J. Yamamoto, K. Sato, Y. Mitsuoka, K. Nakaji ...
1999 Volume 23 Issue 1_2 Pages
712-714
Published: January 20, 1999
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A polarization modulation technique has been applied to a scanning near-field optical microscope (SNOM), in order to improve sensitivity and resolution of a magneto-optical (MO) imaging. Polarized light modulated by a photoelastic modulator (PEM) was introduced into a bent-type optical fiber probe operated as an AFM cantilever, and transmitted MO signals were detected using a lock-in amplifier. Ar ion laser (488 nm) was used as a light source. By using this technique. images of recorded marks on a Pt/Co disk were successfully obtained. which were written by a magnetic field modulation method with a length of 1μm and a track pitch of 1.6 μm on a multilayer of Pt (0.8 nm) / Co (0.3 nm) with thickness of 15 nm. A resolution of approximately 90 nm was obtained in the MO imaging.
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V. Kirilyuk, A. Kirilyuk, Th. Rasing
1999 Volume 23 Issue 1_2 Pages
715-717
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We report the development of a new magnetic imaging technique: nonlinear magneto-optical microscopy. Magnetization induced second harmonic generation (MSHG) is used to image the domain structure in ultrathin CoNi/Pt films. Due to both very high magneto-optical contrast and enhanced interface sensitivity, fine details of magne-tization reversal on CoNi/Pt interfaces become visible with the MSHG imaging that are not detectable by usual magneto-optics. The problem of separating the images from different multilayer interfaces is discussed.
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Koji Yamada, Sinnichi Shoji, Yosinori Tanaka, Yosihito Uno, Hiroyuki T ...
1999 Volume 23 Issue 1_2 Pages
718-720
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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Nondestructive evaluations of iron-based material (A533B) have been investigated on the leakage flux from the surface by using Hall elements, on magnetic noises, on sub-micron deformations by Ar-laser speckle interferometry and on residual stresses by X-ray diffraction. A high resolution and high sensitivity for spatial inhomogeneity observation were attained as small as 200μm for residual strains less than 0.5 %.
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Makoto Sawamura, Tomohide Maruyama, Koichi Mukasa
1999 Volume 23 Issue 1_2 Pages
721-723
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We investigate spin electronic structures of GaN probes, using first principles molecular orbital calculations. It is found that at the pyramidal heads of the probes with the axes parallel to the crystallographic axes [100] and [111] in the zincblende GaN, electron spins are polarized at the lowest energy states. Nearly 8%∼16% of electrons in the valence band are spin-polarized at the proximity of the head depending upon the sort of the atom on the apex and the crystallographic axis of the probe. It is observed that spin polarizability depends on the difference of electronegativities of the elements in a compound and on a highly symmetric nanostructure of the probe. It is due to Jahn-Teller effect of the tip configuration.
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K. Nakamura, T. Oguchi, H. Hasegawa, K. Sueoka, K. Hayakawa, K. Mukasa
1999 Volume 23 Issue 1_2 Pages
724-726
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We calculated the exchange force between two magnetic Fe films by first-principles calculations. It is shown that the exchange force is sensitive to the film-film separation and relative atomic site on the surface for
d/
a<1, where
d is the distance between surfaces of the two films and
a the lattice constant of bulk Fe. Based on their results, the feasibility of exchange force microscopy (EFM), which probes the exchange force between the tip and the sample, was discussed.
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Y. Kuraoka, K. Sueoka, T. Iwata, K. Mukasa, R. Aihara, K. Hayakawa
1999 Volume 23 Issue 1_2 Pages
727-729
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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We developed a retarding-type Mott analyzer, of which the figure of merit and the size were improved as compared with our previously designed analyzers. The figure of merit of the new analyzer is sufficient to be used in a spin-polarized secondary electron microscope (SP-SEM) system. Equipping a UHV-SEM system with the analyzer and a secondary electron collector, we constructed an SP-SEM system. The proper operation of the system was confirmed by observing a single Fe crystal and we got clear images of domain structures on the Fe (001) surface. We also got a magnetic domain image of a patterned permalloy thin film.
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J. Fujii, Y. Suzuki, T. Mizoguchi
1999 Volume 23 Issue 1_2 Pages
730-732
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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The soft x-ray emission intensity from Ni(110) surface was measured by appearance potential spectroscopy with spin polarized electrons near 2p electron threshold energy. The pulse count measurements of x-ray intensity instead of ordinary SXAPS measurements with lock-in technique made it possible to obtain knowledge of effects not only the characteristic x-ray but bremsstrahlung x-ray on spectra. The spectra reveal the invalidty of ordinary APS theory based on one electron approximation for Ni.
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Pill-Soo Kim
1999 Volume 23 Issue 1_2 Pages
733-735
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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This paper describes the method for exact parameter estimation of impulse magnetizer system. As the detailed contact resistance of impulse magnetizer can be obtained, the efficient design of magnetizer which produce desired magnet will be possible using our estimation procedure. As the parameter estimation method of impulse magnetizer, two different estimation methods (a method considering contact resistance and a method using air-core test coil) are presented. The application example has been achieved using a high-voltage, middle-energy capacitor discharge impulse magnetizer and 2-pole iron-core fixture.
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B. Bian, K. Sato, T. Ohkubo, Y. Hirotsu, A. Makino
1999 Volume 23 Issue 1_2 Pages
736-738
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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Granular thin films of oriented α-Fe nanoparticles were prepared by taking advantage of the epitaxial growth of α-Fe on <100> oriented Au "seed" nanoparticles, which were epitaxially grown on a (100) NaCl substrate. The crystallographic orientation between α-Fe and Au nanocrystals is <100>Au//<100>Fe with {010}Au//{011 }Fe. It is shown that this method can be applied to control the size and inter-particle distance of oriented Fe nanocrystals in granular films. Effects of the α-Fe particle size and inter-particle distance on the coercivity of the films have been studied.
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M. Takahashi, A. Kikuchi, N. Iwata, S. Yoshimura, K. K. Tham, H. Shoji
1999 Volume 23 Issue 1_2 Pages
739-741
Published: January 20, 1999
Released on J-STAGE: January 25, 2008
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The effect of film thickness of magnetic layer on Hc for Co based thin film media prepared under ultra clean process (UC-CoCrTa) and normal process (n-CoCrTa) was discussed in connection with their microstructure. In the case of UC-CoCrTa media, the main factor for decrement in H
c for the media with the film thickness of 10∼16 nm is the thermal agitation. On the other hand, for n-CoCrTa, decrement in H
c is mainly caused by the insufficiencies in microstructure such as Cr segregated grain boundary structure and homogeneity in grains diameter.
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