• Title/Summary/Keyword: magnetics fields

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High Resolution Magnetic X-ray Microscopy Study of the Magnetization Reversal in CoCrPt Alloy Thin Films

  • Im, Mi-Young;Fischer, Peter;Eimiiller, Thomas;Shin, Sung-Chul
    • Journal of Magnetics
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    • v.9 no.3
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    • pp.75-78
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    • 2004
  • Magnetic transmission soft X-ray microscopy has been used to study element-specifically the magnetization reversal behavior of ${(Co_{84}Cr_{16})}_{87}Pt_{l3}$ alloy thin films with a lateral resolution of 35 nm. Our results indicate that the magnetization switching is carried out by a random nucleation process that can be attributed to the reversal of individual grains. We found evidence of a large distribution of the switching fields at the nanogranular length scale, which has to be considered seriously for applications of CoCrPt systems as magnetic high density storage materials.

Crystallographic and Magnetic Properties of Iron Oxide Nanoparticles for Applications in Biomedicine

  • Lee, Sang-Won;Woo, Kyoung-Ja;Kim, Chul-Sung
    • Journal of Magnetics
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    • v.9 no.3
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    • pp.83-85
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    • 2004
  • Magnetic nanoparticles have been investigated for use as biomedical purposes for several years. For biomedical applications the use of particles that present superparamagnetic behavior at room temperature is preferred [1-4]. To control the magnetic materials by magnetic field is essential locate particle to the suitable destination on feeding by injection. In order to use them properly, the particles should be nano size. However there are many difficulties in applications, because there is lack of identifications in nano magnetic properties. In our studies, structural and magnetic properties of iron oxide nanoparticles were investigated by XRD, VSM, TEM, and Mossbauer spectroscopy. At 13 K, hyperfine fields of ${\gamma}-Fe_2O_3$ were 516 kOe and 490 kOe, that of $Fe_3O_4$ were 517 kOe and 482 kOe. The saturation magnetizations were 21.42 emu/g and 39.42 emu/g. The particle size of powders is 5~19 nm.

MAGNETISM OF NANOPHASE IRON PARTICLES LASER EVAPORATED IN A CONTROLLED OXYGEN ATMOSPHERE

  • Turkki, T.;Jonsson, B.J.;Strom, V.;Medelius, H.;El-Shall, M.S.;Rao, K.V.
    • Journal of the Korean Magnetics Society
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    • v.5 no.5
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    • pp.745-748
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    • 1995
  • Magnetic nanoparticles of iron and iron oxide have been prepared in a modified upward thermal diffusion cloud chamber using pulsed laser evaporation. SEM/TEM studies of these particles reveal a size distribution with a mean diameter of about $60\;{\AA}$. FTIR spectrum measurements are used to investigate the difference in oxidation level between nanoparticles prepared at different partial oxygen pressures. The complex magnetic behaviour of these particles was studied using DC- and AC-susceptibility measurements. All samples exhibit superparamagnetism with blocking temperatures ranging from 50 K to above room temperature. The coercivity fields as well as the dependence of the blocking temperature on measuring frequency have been studied. magnetic anisotropy constants are found to be one order of magnitude higher than is known for the bulk values. The mean particle size estimated from the magnetic data is found to be in perfect agreement with the TEM observations.

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COERCIVE FIELD AND SPIN-GLASS BEHAVIOR OF AMORPHOUS Y-Fe ALLOYS

  • Fujita, A.;Fukamichi, K.
    • Journal of the Korean Magnetics Society
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    • v.5 no.5
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    • pp.762-766
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    • 1995
  • The coercive field $H_{c}$ of amorphous Y-Fe alloys in the spin-glass state has been investigated. Foramorphous $Y_{10}Fe_{90}$ alloy, the thermal variations of $H_{c}$ in the maximum external field $H_{max}=300,\;600$ and 1 k Oe exhibit a maximum. Since spin-glass behavior is strongly affected by external magnetic fields, the maximum point moves to lower temperature with increasing $H_{max}$. The appearance of the maximum in $H_{c}$ has been discussed in terms of the change of the spin-glass state in the external magnetic field. When the value of $H_{max}$ is 55 kOe, the temperature dependence of $H_{c}$ has no maximum and shows an exponential decrease with increasing temperature. Similar trends have been observed over a wide concentration range. The concentration dependence of $H_{c}$ is associated with the magnetic phase diagram.

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Spin-Motive Force Caused by Vortex Gyration in a Circular Nanodisk with Holes

  • Moon, Jung-Hwan;Lee, Kyung-Jin
    • Journal of Magnetics
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    • v.16 no.1
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    • pp.6-9
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    • 2011
  • Spin-motive force has drawn attention because it contains a fundamental physical property. Spin-motive force creates effective electric and magnetic fields in moving magnetization; a vortex is a plausible system for observing the spin-motive force because of the abrupt profile of magnetization. However, the time-averaged value of a spin-motive force becomes zero when a vortex core undergoes gyroscopic motion. By means of micromagnetic simulation, we demonstrates that a non-zero time-averaged electric field induced by spin-motive force under certain conditions. We propose an experimental method of detecting spin-motive force that provides a better understanding of spin transport in ferromagnetic system.

Recent Developments in Magnetic Measurements: from Technical Method to Physical Knowledge

  • Basso, V.;Fiorillo, F.;Beatrice, C.;Caprile, A.;Kuepferling, M.;Magni, A.;Sasso, C.P.
    • Journal of Magnetics
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    • v.18 no.3
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    • pp.331-338
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    • 2013
  • We present a few significant advances in methods and concepts of magnetic measurements, aimed both at providing novel routes in the characterization of hard and soft magnetic materials and at improving our basic knowledge of the magnetization process. We discuss, in particular, investigation methods and experimental arrangements that have been developed in recent times for: 1) Hysteresis loop determination in extra-hard magnets by means of Pulsed Field Magnetometry; 2) Broadband observation of domain wall dynamics by highspeed stroboscopical Kerr techniques; 3) Entropy measurements in magnetocaloric materials by calorimetry in magnetic field. While pertaining to somewhat independent fields of investigation, all these measuring techniques have in common a solid approach to the underlying physical phenomenology and have a potential for further developments.

The Effect of Crystal and Non-Crystal Structures on Shielding Material Behaviour Under A.C. Field Excitations

  • Rahman, Nazaruddin Abd;Mahadi, Wan Nor Liza
    • Journal of Magnetics
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    • v.18 no.1
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    • pp.9-13
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    • 2013
  • Shielding effects in conductive and magnetic materials were investigated as a function of properties, thickness and diameter. In this work, evaluations on passive conductive and magnetic shield specimens were achieved through experimentation set-up using 50 Hz single and three phase induction field sources. Analysis on material microstructure properties and characteristics of shielding specimens were performed with the use of vibrating sample magnetometer (VSM) and field emission scanning electron microscopy (FESEM). An induction field at $136{\mu}T$ of single phase system and $50{\mu}T$ of three phase systems were observed to the shield specimens with the thickness ranged of 0.2 mm to 0.4 mm. It is observed that shield specimen efficiency becomes inversely proportionate to the increment of induction fields. The decrease was attributed to the surface structure texture which relates to the crystallization and non-crystallization geometrical effects.

Giant interlayer tunneling magnetoresistance in layered manganite

  • Won, C.J.;Yang, J.J.;Cheong, S.W.;Hur, N.
    • Proceedings of the Korean Magnestics Society Conference
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    • 2015.05a
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    • pp.156-157
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    • 2015
  • we have presented the enhanced interlayer tunneling magnetoresistance in doped $La_{1+2x}Sr_{2-2x}Mn_2O_7$ single crystal below $T_C$. The drastically out-of-plane magnetoresistance observed in magnetic fields perpendicular to the bilayers indicates that spin-polarized magnetic layers in single crystal show as a stack of ordered spin valve.

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