共查询到20条相似文献,搜索用时 15 毫秒
1.
S. W. Kim S. S. Lee R. D. Gomez E. J. Hahn D. G. Hwang 《physica status solidi (a)》2006,203(8):2078-2082
The magnetic domain walls at the edges of a large patterned and exchange‐biased NiO (10–60 nm)/NiFe (10 nm) bilayers and their motions with applied field were investigated by MFM. Three kinds of domain walls were found at the edges of the NiO (30 nm)/NiFe (10 nm) bilayer having the exchange biasing field ( H ex) of 21 Oe. Two zigzag charged walls and Néel wall appeared at the edges perpendicular and parallel to H ex, respectively. The zigzag charged walls are nearly a factor of three wider than the Néel wall, and were not observed for the strong exchange‐biased bilayer (60 nm NiO, H ex = 75 Oe). We investigated the subsequent motion of the walls, and identified the pinning and nucleation sites during magnetization reversal. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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In this work, investigations of the magnetic microstructure of anisotropic sintered SmCo5 permanent magnets with high coercivity have been made using the colloid-scanning electron microscopy (SEM) technique and magnetic force microscopy (MFM). The magnets were produced by powder metallurgy (sintering) process and consisted of oriented grains with an average size of about 20 μm. They were studied in the thermally demagnetized state. Owing to the application of digital image recording, enhancement and analysis, high-quality images of the magnetic microstructure were obtained and analyzed not only qualitatively but also quantitatively. Improvements over previous results were achieved. The grains show the presence of magnetic domains, as expected. At the surface perpendicular to the alignment axis, the coarse domain structure in the form of a maze pattern with surface reverse spikes is observed. The main (maze) domains had typical widths 3–5 μm. The reverse spike domains were imaged as circles typically 1–2 μm in diameter or as elongated regions up to about 6 μm in length. Interestingly, in addition to the coarse maze domains and reverse spikes near the surface, a fine surface domain structure is revealed with MFM. The fine scale domains are found to be magnetized perpendicular to the surface and their occurrence is attributed to further reduction of the magnetostatic energy at the cost of a larger domain wall energy. On the surface parallel to the alignment axis, the main domains within individual grains are imaged as stripe domains with domain walls running approximately parallel to the alignment axis, while reverse spike domains are displayed in the form of triangular domains and occur near some grain boundaries, pores or precipitations. The magnetic alignment of grains was found to be good, but certainly not perfect. In most cases the domain structures within grains were independent of their neighbors, but in some cases (not so rare) observations indicated the existence of significant magnetostatic coupling between neighboring grains. The main and surface domain widths were determined by digital means using the stereologic method of Bodenberger and Hubert. Moreover, the domain wall energy and other intrinsic parameters for the studied magnets were determined. 相似文献
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Witold Szmaja Jarosaw Grobelny Micha Cichomski Ken Makita Werner Rodewald 《physica status solidi (a)》2004,201(3):550-555
Magnetic force microscopy (MFM) was used to investigate the domain structure of sintered Nd–Fe–B and SmCo5 permanent magnets at the surfaces perpendicular to the alignment axis. The studied magnets had average grain sizes of about 10 μm and 20 μm, respectively. The observed domain structures resembled those present in bulk uniaxial crystals with strong magnetocrystalline anisotropy. Nevertheless, the main domains in the Nd–Fe–B magnets were approximately three times smaller than those in the SmCo5 magnets. The differences in the domain structures were attributed to different values of the relative magnetic anisotropy as well as to different grain sizes for the two mentioned types of magnets. A comparison was made between theoretical and experimentally determined values of the domain width. The effect of tip‐specimen distance on the MFM image was demonstrated and explained. The magnetic images were correlated with the surface topography revealed by atomic force microscopy (AFM). (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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We have prepared hard–soft spin‐valve systems by ultra‐high vacuum evaporation. These spin‐valves use a CoFe1.5nm/Ir0.5nm/CoFe3nm artificial ferrimagnet (AFi) as a hard magnetic layer, and a Fe/Co bilayer as a detection layer. The Fe layer presents a strong anisotropy and a small interaction with the hard magnetic layer. The AFi is fully antiparallel and is stable up to 330 Oe and 530 Oe, respectively, along the easy (bcc Fe[100]) and the hard (bcc Fe[110]) magnetization axes. These characteristics are correlated with MFM observations made under magnetic field. By increasing the field from zero, ripple features are observed along the Fe[110] axis, and above 530 Oe, 360° domain walls start to develop. Along the Fe[100] axis the ripple features are not observed, but the domain walls characterizing the switching of the AFi are still present. Such magnetic structure plays an essential role in the interaction between the soft and the hard magnetic layers of the spin‐valve, which is unfavorable for sensor applications. 相似文献
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We discuss the magnetostatic energy of checkerboard domain structures in ultrathin magnetic films (of a few monolayer thickness) and in an atomic monolayer using simple magnetostatic considerations where the easy direction of magnetization is perpendicular to the film. The checkerboard domain size, D, the domain-wall width, ω, the ratio f of the uniaxial surface anisotropy, Ks, to the dipolar energy and the binding energy, (BE), have been calculated numerically with the variational parameter δ and the number of atomic layers, nl, as parameters. 相似文献
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M. Ziese 《physica status solidi b》2006,243(6):1383-1389
The micromagnetic structure of a La0.7Sr0.3MnO3 film was studied using magnetic force microscopy and micromagnetic simulations. For a 150 nm thick epitaxial, strain relaxed film grown on SrTiO3 evidence is presented from experiment and simulation that magnetic domains have a typical size of 1 µm at room temperature. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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M. Dreyer M. Kleiber R. Wiesendanger 《Applied Physics A: Materials Science & Processing》1999,69(3):359-361
We have applied magnetic force microscopy in ultrahigh vacuum to study the correlation between the atomic step and magnetic
domain wall structure of ultrathin Co films prepared in situ on Au(111) substrates. For the first time we were able to achieve
high-resolution images showing simultaneously a clear domain wall contrast and the underlying atomic step structure. Although
for in-plane magnetized Co films the domain walls were found to run preferentially in a direction perpendicular to the steps,
no such correlation could be observed for out-of-plane magnetized Co films.
Received: 3 June 1999 / Accepted: 4 June 1999 / Published online: 29 July 1999 相似文献
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The interaction of stray fields and the eddy currents inherent in a sandwich domain structure is studied. This interaction allows us to control the existence of a sandwich domain structure in an amorphous ribbon. The formation of non-uniform magnetic anisotropy in an amorphous ribbon as a result of its annealing in a helical magnetic field is also investigated. 相似文献
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We report here a size dependence of the coercive field in the millimeter–centimeter range length scale of ribbon like samples prepared from ultra soft amorphous and nanocrystalline alloys. A model is proposed where surface pinned domain walls are considered having an effective stiffness constant linearly increasing with the demagnetization factor. 相似文献
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The magnetic domain structures of Fe78.8−xCoxCu0.6Nb2.6Si9B9 (x=0, 20, 40, 60) alloys are investigated by Lorentz microscopy coupled with the focused ion beam method. The specimen prepared using the FIB method is found to have a considerably more uniform thickness compared to that prepared using the ion-milling method. In Fe38.8Co40Cu0.6Nb2.6Si9B9 and Fe18.8Co60Cu0.6Nb2.6Si9B9 alloys, 180° domain walls extending in the direction of the induced magnetic anisotropy are observed. Analysis with Lorentz microscopy reveals that the width of the magnetic domains decreases with an increase in the cobalt content or the induced magnetic anisotropy Ku, that is, the domain width d is proportional to the induced magnetic anisotropy (Ku)−1/4. On the other hand, in the in situ Lorentz microscopy observation as a function of temperature, magnetic ripple structures are found to appear in a localized area due to the fluctuation of magnetization vectors from 423 K. It is observed that the induced magnetic anisotropy caused by the applied magnetic field at 803 K is not suppressed by the magnetic ripple structures observed at 423–443 K. 相似文献
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In ultrathin films, due to the thermal activation and temperature dependencies of the magnetic parameters, magnetization reversal processes are strongly affected by thermal effects. We analyze changes of domain periods of ultrathin cobalt and L10 films in a wide temperature range. With regard to the temperature dependencies of the film magnetic parameters we calculate the equilibrium stripe period as a function of temperature. It is shown that on film heating the equilibrium domain structure (DS) period decreases and at the reorientation phase transition (RPT) approaches its minimal value corresponding to the temperature independent period of the sinusoidal domain structure. Just below the RPT temperature (or thickness) the stripe domain period was found to exponentially decrease with temperature. Irreversible temperature changes of the domain period affected by coercivity are also discussed. 相似文献
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Magnetic Force Microscopy Study of Alternate Sputtered (001) Oriented L1o Phase FePt Films
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We present a magnetic force microscopy study of alternate sputtered (001) oriented L1o phase FePt films. It is found that the root-mean-square value of phase shift of magnetic force images, ( △Ф)rms, can be used to characterize the perpendicular anisotropy for a series of specimens. Therefore, the considerable improvement of the perpendicular anisotropy after post-annealing can be characterized. In addition, the magnetic properties, magnetic and crystalline microstructures before and after post-annealing are compared for the typical [Fe5nm Pt5 nm]10 film with substrate temperature T8 = 500℃, single layer thickness d = 5 nm and total layer thickness D=100 nm to confirm the effect of post-annealing on improving the perpendicular anisotropy for Fe-Pt films. 相似文献
15.
P.J. Metaxas J.P. Jamet J. Ferré B. Rodmacq B. Dieny R.L. Stamps 《Journal of magnetism and magnetic materials》2008
We investigate thermally activated domain wall creep in a system consisting of two ultrathin Co layers with perpendicular anisotropy coupled antiferromagnetically through a 4 nm thick Pt spacer layer. The field driven dynamics of domain walls in the softer Co layer have been measured while keeping the harder Co layer negatively saturated. The effect of the interlayer interaction on the soft layer is interpreted in terms of an effective coupling field, HJ, which results in an asymmetry between the domain wall speeds measured under positive and negative driving fields. We show that creep theory remains valid to describe the observed wall motion when the effective coupling field is included in the creep velocity law as a component of the total field acting on the wall. Using the resultant modified creep expression, we determine a value for the effective coupling field which is consistent with that measured from the shift of the soft layer's minor hysteresis loop. The net antiferromagnetic coupling is attributed to a combination of RKKY and orange-peel coupling. 相似文献
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The magnetic contrast images of a soft magnetic metallic glass Fe79Si6B14Cu1 subjected to a periodic magnetic field were recorded with a scanning electron microscope by using a stroboscopic technique. An image processing method for the extraction of domain patterns from these images is presented. By this technique, delicate details of the dynamic magnetization process can be investigated and differences in the local magnetisation and domain wall movement can be analysed. 相似文献
17.
S.J. May 《Applied Surface Science》2006,252(10):3509-3513
Variable-temperature magnetic force microscopy (MFM) has been performed over the temperature range of 298-348 K on ferromagnetic (In,Mn)As thin films deposited by metal-organic vapor phase epitaxy (MOVPE). Ferromagnetic domains were observed with submicron resolution in both single and two phase (In,Mn)As films, persisting up to 328 K. Isolated cylindrical domains ranging from 100 to 350 nm in diameter with densities of 2-5 × 108 cm−2 were observed in phase pure films. Longer range magnetic order, in the form of ribbon-like domains up to 1 μm in length, are present in the regions between the cylindrical domains. Two phase (In,Mn)As films produced a well-resolved complex domain structure consisting of 180° parallel and antiparallel domains. Excellent agreement between the temperature dependence of the relative magnetization obtained by MFM and superconducting quantum interference device measurements was observed. 相似文献
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Y.L. Iunin Y.P. Kabanov V.I. Nikitenko X.M. Cheng C.L. Chien A.J. Shapiro R.D. Shull 《Journal of magnetism and magnetic materials》2008
We studied the magnetization reversal in ultrathin [Co/Pt]n films (n=1, 2, and 4) using magneto-optical Kerr microscopy. These materials demonstrate unusual asymmetries in the activity of nucleation centers and domain wall motion. It was found that application of very high holding magnetic field prior to magnetization reversal, exceeding some critical value much larger than the apparent saturation field, suppresses the subsequent ‘asymmetric’ nucleation centers, activity. We revealed that the ‘asymmetric’ nucleation centers become active again after subsequent reversal cycles coming from a smaller holding field and studied how the asymmetry returns with the decrease of applied holding field. It was found that in low-coercivity ultrathin Co films, the asymmetry in domain wall velocity decreased sharply with the applied field increase and disappeared when the reversal field is greater than μ0H=1.5 mT. 相似文献
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We use a simple magnetization model to determine domain structures of ultrathin magnetic nanobelts. A train of alternate domains are formed along the length direction. Optimal domain length decreases with belt width. Experimental domain length distributions of Fe bilayer nanobelts can be naturally explained. This approach should be applicable to similar nanomagnets. 相似文献