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Journal articles on the topic 'Magnetic anisotropy of thin films'

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1

Maksymowicz, L. J., M. Lubecka, R. Jabłoński, and J. Sokulski. "Magnetic anisotropy of semiconductor thin films." Journal of Magnetism and Magnetic Materials 196-197 (May 1999): 418–19. http://dx.doi.org/10.1016/s0304-8853(98)00787-2.

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2

Parker, Michael Andrew. "Applications of TEM to microstructure, epitaxy, and preferred orientation in magnetic thin films." Proceedings, annual meeting, Electron Microscopy Society of America 51 (August 1, 1993): 1014–15. http://dx.doi.org/10.1017/s0424820100150903.

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J. Kent Howard, some years ago, published an extensive review of the phenomenon of what he referred to as “grain-to-grain” or “polycrystalline” epitaxy in thin films. Of the six or so different applications of this phenomenon, from superconductors to magnetics, none has greater technological significance than applications to magnetic thin films. This derives from the magnetic anisotropy of these thin films which has such a profound influence on their magnetic properties. In particular, magnetocrystalline anisotropy is often used to engineer thin films with the desired orientation of the easy axis of magnetization for magnetic record ing media applications. Magnetocrystalline anisotropy is intimately connected to the the crystallographic preferred orientation of the grains composing the magnetic layer which can be controlled through the skillful use of epitaxy with a suitable sublayer. The techniques of AEM, especially elongated probe microdiffraction (EPMD), have proven themselves invaluable for characterizing the micro-structure of such thin films.
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3

YANG, T. R., G. ILONCA, A. V. POP, V. TOMA, I. MATEI, and F. BEIUŞAN. "MAGNETORESISTIVITY AND MAGNETIC PROPERTIES IN MgB2 THIN FILMS." International Journal of Modern Physics B 19, no. 24 (September 30, 2005): 3723–29. http://dx.doi.org/10.1142/s0217979205032449.

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Magnetotransport data on MgB 2 thin films, fabricated on Al 2 O 3 substrates using electron–bean deposition and Mg diffusion method are reported for applied magnetic fields up to 9 T. The upper critical field anisotropy, lower critical field and irreversibility field versus temperature are determined. The Hall coefficient is slightly temperature-dependent and positive in the normal state. Using the extracted data, the electronic mean free path, coherence length ξ0, anisotropic coefficient γ and penetration depth λ are calculated.
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4

Pick, Š., and H. Dreyssé. "Magnetic anisotropy of transition-metal thin films." Physical Review B 48, no. 18 (November 1, 1993): 13588–95. http://dx.doi.org/10.1103/physrevb.48.13588.

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5

Zhao, Siqian, Toshiya Hozumi, Patrick LeClair, Gary Mankey, and Takao Suzuki. "Magnetic Anisotropy of $\tau $ -MnAl Thin Films." IEEE Transactions on Magnetics 51, no. 11 (November 2015): 1–4. http://dx.doi.org/10.1109/tmag.2015.2436059.

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6

Asada, Seiichi, and Masahiro Kitada. "FexN thin films with perpendicular magnetic anisotropy." Applied Physics Letters 46, no. 8 (April 15, 1985): 792–93. http://dx.doi.org/10.1063/1.95885.

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7

Nahid, M. A. I., and Takao Suzuki. "Magnetic anisotropy of Fe3Pt alloy thin films." Applied Physics Letters 85, no. 18 (November 2004): 4100–4102. http://dx.doi.org/10.1063/1.1815070.

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8

Piramanayagam, S. N., M. Matsumoto, and A. Morisako. "Perpendicular magnetic anisotropy in NdFeB thin films." Journal of Applied Physics 85, no. 8 (April 15, 1999): 5898–900. http://dx.doi.org/10.1063/1.369907.

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9

Sun, Jia Li, and Jing Guo Hu. "Magnetization Reversal in Ferromagnetic Thin Films." Advanced Materials Research 399-401 (November 2011): 890–95. http://dx.doi.org/10.4028/www.scientific.net/amr.399-401.890.

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The magnetization reversal mechanism of the magnetic films system with the different magnetic anisotropy, exchange coupling, interface coupling, etc. has been simulated by Monte-Carlo method. The results show that the decrease of magnetic anisotropy is in favor of motion of domain walls, but is not conducive to consistent rotation. The interface coupling of both the ferromagnetic film and the antiferromagnetic film are helpful to the motion of domain walls while the antiferromagnetic film coupling is the more effective. Meantime, the evolution of the microscopic magnetic domain structures has been inspected intuitively while the system is in the process of magnetization.
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10

Kouchiyama, A., I. Sumita, Y. Nakayama, and M. Asanuma. "Magnetic anisotropy of sputtered Co-Cr thin films." Journal of the Magnetics Society of Japan 12, no. 2 (1988): 81–84. http://dx.doi.org/10.3379/jmsjmag.12.81.

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11

Katada, H., T. Shimatsu, I. Watanabe, H. Muraoka, Y. Nakamura, and Y. Sugita. "Induced Uniaxial Magnetic Anisotropy in Thin Permalloy Films." Journal of the Magnetics Society of Japan 24, no. 4−2 (2000): 539–42. http://dx.doi.org/10.3379/jmsjmag.24.539.

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12

Suzuki, Y., G. Hu, R. B. van Dover, and R. J. Cava. "Magnetic anisotropy of epitaxial cobalt ferrite thin films." Journal of Magnetism and Magnetic Materials 191, no. 1-2 (January 1999): 1–8. http://dx.doi.org/10.1016/s0304-8853(98)00364-3.

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13

Cheng, Ruihua, Z. Y. Liu, Xu Bo, S. Adenwalla, L. Yuan, S. H. Liou, and P. A. Dowben. "Magnetic anisotropy in epitaxial CrO2 (100) thin films." Materials Letters 56, no. 3 (October 2002): 295–99. http://dx.doi.org/10.1016/s0167-577x(02)00458-5.

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14

Liu, Xiaoxi, Sagar Shirasath, and Kensuke Shindoh. "Co-Ferrite Thin Films With Perpendicular Magnetic Anisotropy." IEEE Transactions on Magnetics 51, no. 11 (November 2015): 1–4. http://dx.doi.org/10.1109/tmag.2015.2436394.

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15

Kouchiyama, A., M. Asanuma, I. Sumita, and Y. Nakayama. "Magnetic Anisotropy of Suppttered Co-Cr Thin Films." IEEE Translation Journal on Magnetics in Japan 4, no. 1 (January 1989): 46–51. http://dx.doi.org/10.1109/tjmj.1989.4563954.

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16

Chang, H. W., M. H. Wu, C. C. Hsieh, W. C. Chang, and D. S. Xue. "High Magnetic Anisotropy Field in CoZr Thin Films." IEEE Transactions on Magnetics 47, no. 10 (October 2011): 3924–27. http://dx.doi.org/10.1109/tmag.2011.2157469.

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17

Luo, C. P., S. H. Liou, L. Gao, Y. Liu, and D. J. Sellmyer. "Nanostructured FePt:B2O3 thin films with perpendicular magnetic anisotropy." Applied Physics Letters 77, no. 14 (October 2, 2000): 2225–27. http://dx.doi.org/10.1063/1.1314289.

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18

Myagkov, V. G., L. E. Bykova, V. Yu Yakovchuk, A. A. Matsynin, D. A. Velikanov, G. S. Patrin, G. Yu Yurkin, and G. N. Bondarenko. "High rotatable magnetic anisotropy in MnBi thin films." JETP Letters 105, no. 10 (May 2017): 651–56. http://dx.doi.org/10.1134/s0021364017100095.

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19

Košuth, M., V. Popescu, H. Ebert, and G. Bayreuther. "Magnetic anisotropy of thin Fe films on GaAs." Europhysics Letters (EPL) 72, no. 5 (December 2005): 816–22. http://dx.doi.org/10.1209/epl/i2005-10309-6.

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20

Resnick, Damon A., A. McClure, C. M. Kuster, P. Rugheimer, and Y. U. Idzerda. "Field dependent magnetic anisotropy of Ga0.2Fe0.8 thin films." Journal of Applied Physics 109, no. 7 (April 2011): 07A938. http://dx.doi.org/10.1063/1.3563122.

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21

Kistenmacher, T. J., W. A. Bryden, and K. Moorjani. "Random magnetic anisotropy in thin films of amorphousMn48B52." Physical Review B 40, no. 14 (November 15, 1989): 9895–99. http://dx.doi.org/10.1103/physrevb.40.9895.

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22

Su, Q., J. P. Teter, Y. Wen, J. R. Cullen, and M. Wuttig. "Magnetic anisotropy in Terfenol-D thin films (abstract)." Journal of Applied Physics 81, no. 8 (April 15, 1997): 5424. http://dx.doi.org/10.1063/1.364559.

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23

Dunaevskii, S. M., E. Yu Lobanova, E. K. Mikhailenko, and I. I. Pronin. "Magnetic Anisotropy of Graphene-Coated Thin Iron Films." Physics of the Solid State 61, no. 7 (July 2019): 1310–15. http://dx.doi.org/10.1134/s1063783419070072.

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24

Yamkane, Z., M. Hannachi, R. Moubah, S. Derkaoui, H. Lassri, L. Bessais, and N. Mliki. "Random Magnetic Anisotropy Studies in SmCo5 Thin Films." Journal of Superconductivity and Novel Magnetism 31, no. 7 (November 24, 2017): 2055–58. http://dx.doi.org/10.1007/s10948-017-4446-1.

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25

JIAO, DONGMAO, JIANGONG LI, XIA NI, and XUDONG ZHANG. "MICROSTRUCTURES AND MAGNETIC PROPERTIES OF COBALT THIN FILMS." Modern Physics Letters B 22, no. 31 (December 20, 2008): 3079–86. http://dx.doi.org/10.1142/s021798490801759x.

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Cobalt thin films deposited by radio frequency sputtering were investigated. Microstructures of the Co films were analyzed by XRD and TEM. The results show that films microstructure varies with the variation of the sputter gas pressure P Ar . Magnetic properties measured by VSM show that all the films possess relatively high saturation magnetization 4πMs, and strong in-plane uniaxial magnetic anisotropy field Hk. Co films deposited below 0.3 Pa show soft magnetic properties and its microwave permeability was measured by vector network analyzer in the 0.1–5 GHz range.
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26

Lai, Heng, Zhi Gao Huang, Rongquan Gai, Shui Yuan Chen, and You Wei Du. "Dynamics of Magnetization Reversal in Thin Polycrystalline Co Films." Materials Science Forum 475-479 (January 2005): 2263–66. http://dx.doi.org/10.4028/www.scientific.net/msf.475-479.2263.

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The thin polycrystalline Co films with different annealed time were prepared by magnetron sputtering method. XRD and hysteresis loops of the samples were measured. A mean field equation with Heisenberg model for calculating dynamic scaling was derived. The experimental and simulated results indicate that, the scaling law, A=A0+H0 a ω b, describes well dynamic magnetization along easy and hard axes for the anisotropy magnetic films; the anisotropy scaling exponents exist clearly in the anisotropy films; the simulated results are consistent with the experimental those.
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27

Li, Jianjun. "Angular Response of Magnetostrictive Thin Films." Journal of Nanomaterials 2012 (2012): 1–7. http://dx.doi.org/10.1155/2012/940272.

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The magnetostrictions of the single TbFe layer and coupled Py/TbFe2bilayers were measured by using laser deflectometry. The dependences of the magntostriction performance on the driving magnetic field direction have been investigated. The relationship studies between the saturation bending angle and torsion angle of the single layer with perpendicular anisotropy and coupled bilayers with in-plane uniaxial anisotropy have been conducted. Interesting “jump” reflecting the spin dynamics is observed in the magnetostriction loops of the coupled bilayers.
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28

Yu, Ying, Shu Hong Xie, and Qing Feng Zhan. "Effect of Thickness on Mechanically Tunable Magnetic Anisotropy of FeGa Thin Films Deposited on Flexible Substrates." Materials Science Forum 815 (March 2015): 227–32. http://dx.doi.org/10.4028/www.scientific.net/msf.815.227.

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A practical way to manipulate the magnetic anisotropy of magnetostrictive FeGa thin films grown on flexible polyethylene terephthalate (PET) substrates is introduced in this study. The effect of film thickness on magnetic properties and magnetostriction constant of polycrystalline FeGa thin films was investigated. The anisotropy field Hk of flexible FeGa films, i.e., the saturation field determined by fitting the hysteresis curves measured along the hard axis, was enhanced with increasing the tensile strain applied along the easy axis of the thin films, but this enhancement via strain became unconspicuous with increasing the thickness of FeGa films. In order to study the magnetic sensitivity of thin films responding to the external stress, we applied different strains on these films and measure the corresponding anisotropy field. Moreover, the effective magnetostriction constant of FeGa films was calculated from the changes of both anisotropy field and external strain based on the Villari effect. A Neel’s phenomenological model was developed to illustrate that the effective anisotropy field of FeGa thin films was contributed from both the constant volume term and the inverse thickness dependent surface term. Therefore, the magnetic properties for the volume and surface of FeGa thin films were different, which has been verified in this work by using vibrating sample magnetometer (VSM) and magneto-optic Kerr effect (MOKE) system. The anisotropy field contributed by the surface of FeGa film and obtained by MOKE is smaller than that contributed by the film volume and measured by VSM. We ascribed the difference in Hk to the relaxation of the effective strain applied on the films with increasing the thickness of films.
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29

Suezawa, K., M. Yamaguchi, K. I. Arai, Y. Shimada, S. Tanabe, and K. Ito. "Control of Magnetic Anisotropy by Micro-patterning Magnetic Thin Films." Journal of the Magnetics Society of Japan 24, no. 4−2 (2000): 731–34. http://dx.doi.org/10.3379/jmsjmag.24.731.

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30

Katada, H., T. Shimatsu, I. Watanabe, H. Muraoka, Y. Nakamura, and Y. Sugita. "Induced Uniaxial Magnetic Anisotropy in Very Thin Soft Magnetic Films." Journal of the Magnetics Society of Japan 25, no. 4−2 (2001): 867–70. http://dx.doi.org/10.3379/jmsjmag.25.867.

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31

Kawada, Y., M. Onose, R. Tojo, T. Komine, and R. Sugita. "Magnetic domain structure in thin CoPt perpendicular magnetic anisotropy films." EPJ Web of Conferences 40 (2013): 07002. http://dx.doi.org/10.1051/epjconf/20134007002.

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32

Jakučionis, L., and V. Kleiza. "Electrical Anisotropy of Thin Metal Films Growing on Dielectric Substrates." Nonlinear Analysis: Modelling and Control 7, no. 2 (December 5, 2002): 45–52. http://dx.doi.org/10.15388/na.2002.7.2.15193.

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Electrical properties of conductive thin films, that are produced by vacuum evaporation on the dielectric substrates, and which properties depend on their thickness, usually are anisotropic i.e. they have uniaxial anisotropy. If the condensate grow on dielectric substrates on which plane electrical field E is created the transverse voltage U⊥ appears on the boundary of the film in the direction perpendicular to E. Transverse voltage U⊥ depends on the angle γ between the applied magnetic field H and axis of light magnetisation. When electric field E is applied to continuous or grid layers, U⊥ and resistance R of layers are changed by changing γ. It means that value of U⊥ is the measure of anisotropy magnitude. Increasing voltage U0 , which is created by E, U⊥ increases to certain magnitude and later decreases. The anisotropy of continuous thin layers is excited by inequality of conductivity tensor components σ0 ≠ σ⊥. The reason of anisotropy is explained by the model which shows that properties of grain boundaries are defined by unequal probability of transient of charge carrier.
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33

Mao, Xing Yu, Zhi Jian Ke, Wei Dong Zou, Qiu Bao Lin, and Yan Wu. "The Magnetic Properties of FeCoNbB Nanocrystalline Films." Advanced Materials Research 787 (September 2013): 388–91. http://dx.doi.org/10.4028/www.scientific.net/amr.787.388.

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The nanocrystalline FeCoNbB films are made by magnetron sputtering. The magnetization saturation of the filmes increase with the film thickness. The complex permeability spectra of the samples vary with the thickness of the film as well. The relaxation frequency is much higher than that of FeCoNbB ribbons because of magnetocrystalline anisotropy. The amplitude of the real part of the permeability decreases with the rising thickness of the film. This phenomenon suggest that the random anisotropy theory is to somewhat applicable for thin films. The X-ray diffraction pattern and the shape of the hysteresis loop show the crystal grains grow with the increase of the film thickness and also result a deterioration in magnetic softness.
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34

Stebliy, Maxim E., Alexey V. Ognev, Alexander Samardak, Gleb Tregubov, Evgeniy Mikoluk, and Ludmila A. Chebotkevich. "The Improved Magneto-Optical Kerr Effect Method of Magnetic Anisotropy Measurements in Thin Films and Nanostructures." Solid State Phenomena 215 (April 2014): 445–47. http://dx.doi.org/10.4028/www.scientific.net/ssp.215.445.

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Magnetic anisotropy of thin films and nanodisk arrays made of cobalt has been studied by the magneto-optical anisometry with modulated field. The improved method of magnetic anisotropy field measurements in thin films has been proposed. This method has been used for cobalt nanodisk arrays in order to investigate anisotropy of magnetization reversal processes due to dipole-dipole interaction between nanodisks.
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35

Wu, Han-Chun, Xiao Liu, Cormac Ó. Coileáin, Hongjun Xu, Mourad Abid, Mohamed Abid, Askar Syrlybekov, et al. "Competition Between Anti-Phase Boundaries and Charge-Orbital Ordering in Epitaxial Stepped Fe3O4(100) Thin Films." SPIN 07, no. 02 (November 22, 2016): 1750001. http://dx.doi.org/10.1142/s2010324717500011.

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Magnetite is a highly utilized transition metal oxide with many interesting magnetic and transport properties. The presence of anti-phase boundaries (APBs) and charge-orbital ordering (COO) are two of the most exciting properties of epitaxial magnetite thin films. Here, epitaxial stepped Fe3O4 films were prepared to investigate the competition between APBs and COO via measurements of in-plane anisotropy. The anisotropy was probed for two orthogonal configurations, with magnetic field applied or electrical-contacts aligned either along or perpendicular to the steps. We reveal that the APBs dominate the magnetic and transport properties of the films above the Verwey transition temperature ([Formula: see text]. However, below [Formula: see text] film thickness becomes a decisive factor in determining the magnetic nature of stepped magnetite films, due to its correlation with domain size. When the film is thinner than a critical thickness, the anisotropy is dominated by the APBs, and a higher anisotropy constant and MR ratio are observed when the magnetic field or contacts are oriented along the steps. Conversely, for sufficiently thick films, below [Formula: see text], the magnetic and electrical transport properties are dominated by COO. Thus a higher anisotropy constant and MR ratio are observed when the magnetic field or contacts are oriented perpendicular to the steps.
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36

Kandpal, Lalit M., Sandeep Singh, Pawan Kumar, P. K. Siwach, Anurag Gupta, V. P. S. Awana, and H. K. Singh. "Magnetic anisotropy and anisotropic magnetoresistance in strongly phase separated manganite thin films." Journal of Magnetism and Magnetic Materials 408 (June 2016): 60–66. http://dx.doi.org/10.1016/j.jmmm.2016.02.022.

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37

Rappoport, Tatiana G., F. S. de Menezes, L. C. Sampaio, M. P. Albuquerque, and F. Mello. "Domain Analysis and Magnetic Relaxation in Thin Films." International Journal of Modern Physics C 09, no. 06 (September 1998): 821–25. http://dx.doi.org/10.1142/s0129183198000753.

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We have simulated the magnetic relaxation (M(t)) and the nucleation of magnetic domains in the presence of magnetic field in thin films with anisotropy perpendicular to the film plane. We have used Monte Carlo simulations based on the two-dimensional classical Ising model including the long-range dipole–dipole and Zeeman interactions. Domains nucleated during the magnetic relaxation exhibit very rough interfaces. We analyze the roughness and the M(t) as a function of the relative strength of dipole–dipole and Zeeman terms.
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38

DEMIREL, ALI IHSAN. "PINNING MECHANISM AND FLUX MOTION IN YBa2Cu3O7 THIN FILMS." International Journal of Modern Physics B 18, no. 07 (March 20, 2004): 999–1006. http://dx.doi.org/10.1142/s0217979204024434.

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The flux creep phenomena and the J c characteristics have been investigated in the YBa 2 Cu 3 O 7 (YBCO) thin films grown by metal organics chemical vapor deposition (MOCVD) technique. The anisotropy of the current density (J c ) is discussed on the basis of the intrinsic pinning model and the anisotropic critical magnetic field (H c2 ). The properties of the high J c and the pinning energy are related with the fine precipitates observed by tunneling electron microscopy (TEM). The strong pinning mechanism affects the amount of the flux motion.
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39

Mangin, S., C. Bellouard, G. Marchal, and B. Barbara. "Control of the magnetic anisotropy of GdFe thin films." Journal of Magnetism and Magnetic Materials 165, no. 1-3 (January 1997): 161–64. http://dx.doi.org/10.1016/s0304-8853(96)00495-7.

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40

Li, Yi, C. Polaczyk, and D. Riegel. "Magnetic anisotropy of thin Fe films grown on Ni." Journal of Magnetism and Magnetic Materials 165, no. 1-3 (January 1997): 227–29. http://dx.doi.org/10.1016/s0304-8853(96)00516-1.

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41

Fu, Y., Z. Yang, T. Miyao, M. Matsumoto, X. X. Liu, and A. Morisako. "Induced anisotropy in soft magnetic Fe65Co35/Co thin films." Materials Science and Engineering: B 133, no. 1-3 (August 2006): 61–65. http://dx.doi.org/10.1016/j.mseb.2006.05.002.

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42

Magnus, F., R. Moubah, A. H. Roos, A. Kruk, V. Kapaklis, T. Hase, B. Hjörvarsson, and G. Andersson. "Tunable giant magnetic anisotropy in amorphous SmCo thin films." Applied Physics Letters 102, no. 16 (April 22, 2013): 162402. http://dx.doi.org/10.1063/1.4802908.

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43

Barsukov, I., Yu Fu, A. M. Gonçalves, M. Spasova, M. Farle, L. C. Sampaio, R. E. Arias, and I. N. Krivorotov. "Field-dependent perpendicular magnetic anisotropy in CoFeB thin films." Applied Physics Letters 105, no. 15 (October 13, 2014): 152403. http://dx.doi.org/10.1063/1.4897939.

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44

Kang, S. S., X. Y. Liu, X. H. Xiang, G. J. Jin, J. H. Du, M. Lu, Mu Wang, et al. "Growth-induced magnetic anisotropy behavior in Ni thin films." Journal of Magnetism and Magnetic Materials 187, no. 2 (August 1998): 154–59. http://dx.doi.org/10.1016/s0304-8853(98)00119-x.

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45

Zhou, Y. Z., J. S. Chen, G. M. Chow, and J. P. Wang. "FePt-Ag Nanocomposite Thin Films with Longitudinal Magnetic Anisotropy." Journal of Nanoscience and Nanotechnology 4, no. 7 (September 1, 2004): 704–7. http://dx.doi.org/10.1166/jnn.2004.089.

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46

Chen, Y. J., T. Suzuki, S. P. Wong, and H. Sang. "Perpendicular magnetic anisotropy of Co–Ag granular thin films." Journal of Applied Physics 85, no. 8 (April 15, 1999): 5048–50. http://dx.doi.org/10.1063/1.370087.

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47

Pick, Štěpán, J. Dorantes-Dávila, G. M. Pastor, and Hugues Dreyssé. "Magnetic anisotropy of transition-metal thin films: Convergence properties." Physical Review B 50, no. 2 (July 1, 1994): 993–97. http://dx.doi.org/10.1103/physrevb.50.993.

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48

Resnick, Damon A., A. McClure, C. M. Kuster, P. Rugheimer, and Y. U. Idzerda. "Field dependent magnetic anisotropy of Fe1−xZnx thin films." Journal of Applied Physics 113, no. 17 (May 7, 2013): 17A920. http://dx.doi.org/10.1063/1.4796048.

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49

Sugimoto, Naoto, Takashi Inukai, Morito Matsuoka, and Ken'ichi Ono. "Stress-Induced Perpendicular Magnetic Anisotropy in PtMnSb Thin Films." Japanese Journal of Applied Physics 28, Part 1, No. 6 (June 20, 1989): 1139–40. http://dx.doi.org/10.1143/jjap.28.1139.

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50

Zdyb, R., A. Pavlovska, and E. Bauer. "Strain engineering of magnetic anisotropy in thin ferromagnetic films." Journal of Physics: Condensed Matter 21, no. 31 (July 7, 2009): 314012. http://dx.doi.org/10.1088/0953-8984/21/31/314012.

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