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1

IEEE Power Electronics Society. Electronics Transformers Technical Committee. and IEEE Standards Board, eds. IEEE standard for ferroresonant voltage regulators. Institute of Electrical and Electronics Engineers, 1990.

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2

IEEE Power Electronics Society. Electronics Transformers Technical Committee. and IEEE Standards Board, eds. IEEE standard for ferroresonant voltage regulators. Institute of Electrical and Electronics Engineers, 1998.

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3

Geck, Jochen. Spins, charges, and orbitals in perovskite manganites: Resonant and hard X-ray scattering studies. Mensch & Buch, 2004.

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4

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. Ferromagnetic Resonance. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0008.

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In the previous chapters we covered theoretical aspects of magnetism and magnetization dynamics, as well as practical aspects of implementation of the SLL equation in efficient softwares. In this chapter we focus on the most natural and frequently used experimental method to study magnetization dynamics, namely ferromagnetic resonance (FMR). This experimental technique has evolved into a powerful experimental technique for studies of magnetization dynamics of materials. It is, by far, the most common method for extracting damping parameters in materials, and is also a reliable technique for es
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5

Yaln, Orhan, ed. Ferromagnetic Resonance - Theory and Applications. InTech, 2013. http://dx.doi.org/10.5772/50583.

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6

Shavrov, V. G., and V. I. Shcheglov. Ferromagnetic Resonance in Orientational Transition Conditions. Taylor & Francis Group, 2021.

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7

Ferromagnetic Resonance in Orientational Transition Conditions. Taylor & Francis Group, 2021.

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8

Shavrov, V. G., and V. I. Shcheglov. Ferromagnetic Resonance in Orientational Transition Conditions. Taylor & Francis Group, 2021.

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9

Shavrov, V. G., and V. I. Shcheglov. Ferromagnetic Resonance in Orientational Transition Conditions. Taylor & Francis Group, 2021.

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10

Spin-pumping effects in ferromagnetic thin film heterostructures measured through ferromagnetic resonance. [publisher not identified], 2022.

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11

Vonsovskii, S. V. Ferromagnetic Resonance: The Phenomenon of Resonant Absorption of a High-Frequency Magnetic Field in Ferromagnetic Substances. Elsevier Science & Technology Books, 2013.

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12

Sovskii, S. V. Von. Ferromagnetic Resonance: The Phenomenon of Resonant Absorption of a High-Frequency Magnetic Field in Ferromagnetic Substances. Elsevier Science & Technology Books, 2016.

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13

Novel torques on magnetization measured through ferromagnetic resonance. [publisher not identified], 2015.

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14

Compton, Robert L. Ferromagnetic resonance study of the magnetic anisotropy of a bilayer of Fe on FePtp3s. 2001.

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15

Zhang, Fengling. Ferromagnetic resonance study of anisotropies of Co/Re multilayers. 1998.

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16

Lui, Weixiao. Ferromagnetic resonance analysis of epitaxial Fe/Cr & Co/Mo multilayers. 1995.

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17

Teng, Nienchtze. Exchange bias anisotropy: Probing the FM/AF spin interaction with variable-temperature ferromagnetic resonance. 1999.

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18

Nelineĭnye spinovye volny. "Nauka," Glav. red. fiziko-matematicheskoĭ lit-ry, 1987.

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19

O'Brien, Alexandra V. A ferromagnetic resonance study of the magnetic anisotropies and interlayer coupling of Co/Cr trilayers. 1997.

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20

Saitoh, E., and K. Ando. Experimental observation of the spin Hall effect using spin dynamics. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0015.

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This chapter describes an experiment on the inverse spin Hall effect (ISHE) induced by spin pumping. Spin pumping is the generation of spin currents as a result of magnetization M(t) precession; in a ferromagnetic/paramagnetic bilayer system, a conduction-electron spin current is pumped out of the ferromagnetic layer into the paramagnetic conduction layer in a ferromagnetic resonance condition. The sample used in the experiment is a Ni81Fe19/Pt bilayer film comprising a 10-nm-thick ferromagnetic Ni81Fe19layer and a 10-nm-thick paramagnetic Pt layer. For the measurement, the sample system is pl
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21

Institute Of Electrical and Electronics Engineers. IEEE Standard for Ferroresonant Voltage Regulators(ansi). Institute of Electrical & Electronics Enginee, 1997.

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22

449-1998 IEEE Standard for Ferroresonant Voltage Regulators. Inst of Elect & Electronic, 1999.

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23

Pirota, Kleber Roberto, Angela Knobel, Manuel Hernandez-Velez, Kornelius Nielsch, and Manuel Vázquez. Magnetic nanowires: Fabrication and characterization. Edited by A. V. Narlikar and Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533053.013.22.

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This article describes the fabrication and characterization of magnetic nanowires, focusing on the magnetic properties of patterned arrays of metallic magnetic nanowires electrodeposited into the pores of anodized-alumina membranes. It also discusses the complex magnetization processes, both in isolated nanowires and in collectively patterned arrays. After providing an overview of the state-of-the-art on fabrication techniques of nanowires, the article considers the microstructure of magnetic nanowires and the magnetic properties of single nanowires. It then examines the collective behavior of
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24

Solymar, L., D. Walsh, and R. R. A. Syms. Magnetic materials. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198829942.003.0011.

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Macroscopic and microscopic theories of magnetic polarization are discussed. The origin of domains, domain walls, and of the hysteresis curve and the contrast between soft and hard magnetic materials are explained. The more important elements of the quantum theory of magnetism are discussed. The principles of the alignments in antiferromagnetic and ferromagnetic materials are explained. Magnetic resonance phenomena are discussed. Magnetoresistance and spintronics and their device prospects are also discussed at some length.
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25

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. The Damping Term, from First Principles. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0006.

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In the previous chapters we described the basic principles of density functional theory, gave examples of how accurate it is to describe static magnetic properties in general, and derived from this basis the master equation for atomistic spin-dynamics; the SLL (or SLLG) equation. However, one term was not described in these chapters, namely the damping parameter. This parameter is a crucial one in the SLL (or SLLG) equation, since it allows for energy and angular momentum to dissipate from the simulation cell. The damping parameter can be evaluated from density functional theory, and the Kohn-
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