Advances in Nanoscale Magnetism: Proceedings of the by I. Galanakis, K. Özdog̃an, E. Şaşiog̃lu (auth.), Professor Dr.

By I. Galanakis, K. Özdog̃an, E. Şaşiog̃lu (auth.), Professor Dr. Bekir Aktas, Dr. Faik Mikailov (eds.)

The ebook goals to supply an outline of modern development within the figuring out of magnetic homes in nanoscale via contemporary result of a number of theoretical and experimental investigations. The papers describe a variety of actual points, including theoretical and experimental tools. it really is of relevant curiosity to researchers and experts in magnetism and magnetic fabrics technology, either in educational and business learn, in addition to complex students.

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Extra info for Advances in Nanoscale Magnetism: Proceedings of the International Conference on Nanoscale Magnetism ICNM-2007 June 25–29, Istanbul, Turkey

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Miura, J. Appl. Phys. 95, 6518 (2004) 37. K. Ono, J. Okabayashi, M. Mizuguchi, M. Oshima, A. Fujimori, H. Akinaga, J. Appl. Phys. 91, 8088 (2002) 38. M. Shirai, Physica E 10, 143 (2001) 39. M. Shirai, J. Appl. Phys. 93, 6844 (2003) 40. H. Zhao, F. Matsukura, K. Takamura, E. Abe, D. Chiba, H. Ohno, Appl. Phys. Lett. 79, 2776 (2001) 41. H. Zhao, F. Matsukura, K. Takamura, E. Abe, D. Chiba, Y. Ohno, K. Ohtani, H. Ohno, Mat. Sci. Semicond. Proc. 6, 507 (2003) 42. M. Horne, P. M. Temmerman, Z. Szotek, A.

The equation proposed by Bloch–Bloembergen is frequently used in the study of the microscopic processes; and the approximated Lorentzian formula is used in experimental studies [23]. The line-width of the FMR spectra is directly related to the damping of spin dynamics and in-homogeneity including the defects, impurity, variant, porosity, vacant, etc. in the films. The intrinsic damping constant is generally calculated by analyzing the line-width of the FMR spectra. Even though the a-damping constant is extremely important for achieving high-speed magnetization switching, there are very few studies on a-Gilbert damping constant of Heusler alloy films [29, 30].

X-ray diffraction pattern will show three types of reflections with structure amplitudes F as follows [22] 1. , F(1,1,1) = 4|{(fA − fC )2 + (fB − fD )2}1/2| 2. , F(220) = 4|fA + fC + fB + fD | In the above expressions, fA , fC , fB , and fD are the average scattering factors of atoms at the corresponding lattice sites. Reflections for which (h + k + l)/2 = 2n are the principal reflections. As seen from the above expression, all the average scattering factors simply add up and so any interchange in positions will not affect the structure amplitude F in this case.

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