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1

Babu, Md Majibul Haque, and Maxim Tsoi. "Contact and bulk rectification effects in ferromagnetic resonance experiments." Low Temperature Physics 50, no. 8 (2024): 683–87. http://dx.doi.org/10.1063/10.0027925.

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We present an experimental study of the spin rectification effects produced by ferromagnetic resonance in a NiFe wire. A system of four independent nonmagnetic contact probes was used to supply both rf and dc currents to the wire and to measure dc voltages at different locations in the wire. The rf current drives the ferromagnet’s magnetization into resonance and produces a dc photovoltage which results from the rectification of rf current in the ferromagnet with oscillating magnetization. Our 4-probe system provided a means to detect the photovoltage and separate contributions from the ferrom
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2

Barandiarán, J. M., and D. S. Schmool. "Ferromagnetic resonance studies of multiphase ferromagnets." Journal of Magnetism and Magnetic Materials 221, no. 1-2 (2000): 178–86. http://dx.doi.org/10.1016/s0304-8853(00)00382-6.

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3

Kharisov, A. T., L. A. Kalyakin, and M. A. Shamsutdinov. "Autoresonance Excitation of Nonlinear Oscillations of Magnetization and Domain Walls in Ferromagnets." Solid State Phenomena 168-169 (December 2010): 77–80. http://dx.doi.org/10.4028/www.scientific.net/ssp.168-169.77.

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We investigate the conditions of capturing into resonance and exciting nonlinear ferromagnetic resonance in a ferromagnetic film with the anisotropic easy plane, as well as autoresonance excitation of nonlinear oscillations of the domain wall in uniaxial ferromagnets. The investigations demonstrate that in easy-plane ferromagnets with a narrow resonance line nonlinear oscillations of magnetization in the autoresonance mode can be generated. This autoresonance takes place if the resonance field grows slowly and pumping frequency is the constant which is equal to the frequency of linear resonanc
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4

Lee, Yong Heng, and Ramanathan Mahendiran. "Transport and electron spin resonance studies in Mo-doped LaMnO3." AIP Advances 13, no. 2 (2023): 025115. http://dx.doi.org/10.1063/9.0000442.

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We report the magnetic, electrical, thermoelectric, and magnetic resonance properties of the Mn-site doped manganite LaMn0.94Mo0.06O3. This sample undergoes an insulator-metal transition around 235 K, near the ferromagnetic Curie temperature (TC = 237 K) in zero external magnetic field. On the other hand, thermopower exhibits a maximum at TS = 258 K, which is 23 K higher than TC. This discrepancy is attributed to nucleation of ferromagnetic clusters (Griffiths phase) above TC, which is supported by the deviation of inverse susceptibility from Curie-Weiss from linear behavior below 270 K and no
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5

Dantas, Ana L., L. L. Oliveira, M. L. Silva, and A. S. Carriço. "Ferromagnetic resonance of compensated ferromagnetic/antiferromagnetic bilayers." Journal of Applied Physics 112, no. 7 (2012): 073907. http://dx.doi.org/10.1063/1.4757032.

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6

Layadi, A., and J. O. Artman. "A ferromagnetic resonance investigation of ferromagnetic coupling." Journal of Physics D: Applied Physics 30, no. 24 (1997): 3312–16. http://dx.doi.org/10.1088/0022-3727/30/24/008.

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7

Dowling, Reyne, Ryszard Narkowicz, Kilian Lenz, Antje Oelschlägel, Jürgen Lindner, and Mikhail Kostylev. "Resonance-Based Sensing of Magnetic Nanoparticles Using Microfluidic Devices with Ferromagnetic Antidot Nanostructures." Nanomaterials 14, no. 1 (2023): 19. http://dx.doi.org/10.3390/nano14010019.

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We demonstrated resonance-based detection of magnetic nanoparticles employing novel designs based upon planar (on-chip) microresonators that may serve as alternatives to conventional magnetoresistive magnetic nanoparticle detectors. We detected 130 nm sized magnetic nanoparticle clusters immobilized on sensor surfaces after flowing through PDMS microfluidic channels molded using a 3D printed mold. Two detection schemes were investigated: (i) indirect detection incorporating ferromagnetic antidot nanostructures within microresonators, and (ii) direct detection of nanoparticles without an antido
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8

Jin, Wei, Kuang Shi, and Jun Hao Li. "The Study of Ferromagnetic Resonance Overvoltage and its Suppression Methods in 35kv Power System." Advanced Materials Research 748 (August 2013): 449–52. http://dx.doi.org/10.4028/www.scientific.net/amr.748.449.

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Ferromagnetic resonance overvoltage is an internal overvoltage and it often occurred in the power distribution system which neutral point ungrounded. A 35kV power system is used as the prototype to establish the 35 kV substation's simulation model which is based on the ATP - EMTP and ferromagnetic resonance overvoltage is researched and analyzed In this paper. The ferromagnetic resonance overvoltage which is stimulated by single-phase ground fault is studied in this paper studied and ferromagnetic resonance suppression methods were also studied. The results show that the nonlinear resistor is
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9

Shigeno, Nozomu, Shin Negishi, Kazushi Hoshi, Takayuki Fukunaga, Shinichi Furusawa, and Hiroshi Sakurai. "Ferromagnetic Resonance Frequency of Single-Layer Magnetic Metal Films with Lattice Distortion." Key Engineering Materials 459 (December 2010): 15–18. http://dx.doi.org/10.4028/www.scientific.net/kem.459.15.

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The ferromagnetic resonance frequency of single-layer magnetic films has been investigated in relation to lattice distortion. It is found that the ferromagnetic resonance frequency depends on a lattice distortion. This result raises the possibility of tuning the ferromagnetic resonance frequency by controlling the lattice distortion.
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10

Su, Ri-Jian, Ya-Bin Wang, Li-Hong Yu, Hao Tang, Zhong-Zhou Du, and Qiu-Wen Zhang. "A Ferromagnetic Resonance Temperature Measurement Method Based on Sweep Frequency Technique." Journal of Nanoelectronics and Optoelectronics 16, no. 10 (2021): 1537–43. http://dx.doi.org/10.1166/jno.2021.3108.

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The ferromagnetic resonance frequency of the ferromagnetic nanoparticles has a strong temperature dependency. The frequency sweep method is a standard method to measure frequency accurately in the available technology. Based on the free energy of the spin system of single-domain ferromagnetic nanoparticles with uniaxial anisotropy, we establish a relationship model between ferromagnetic resonance frequency and temperature under the ferromagnetic resonance condition. And this model is simulated by the frequency sweep method in the temperature range of 0–60 °C, which proves that it is practicabl
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11

Xiang, Ying, Jun-Sheng Feng, Xin Luo, and Yuan Chen. "Transverse Ferromagnetic Resonance of Heisenberg Ferromagnets With Exchange Anisotropy." IEEE Transactions on Magnetics 47, no. 6 (2011): 1653–57. http://dx.doi.org/10.1109/tmag.2011.2116160.

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12

Patel, Rajen, and Frank J. Owens. "Evidence for Stable High-Temperature Ferromagnetism in Fluorine-Treated C60." Journal of Materials 2013 (February 2, 2013): 1–5. http://dx.doi.org/10.1155/2013/261304.

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It is shown by magnetic field dependent ac susceptibility, magnetic force microscopy, and ferromagnetic resonance that exposure of C60 to fluorine at 160°C produces a stable ferromagnetic material with a Curie temperature well above room temperature. The exposure to fluorine is accomplished by decomposing a fluorine-rich polymer, trifluorochloroethylene [F2C–CFCl]n, which has C60 imbedded in it. Based on previous experimental observations and molecular orbital calculations, it is suggested that the ferromagnetism is arising from crystals of C60–F.
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13

Zhou, Ziyao, Bin Peng, Mingmin Zhu, and Ming Liu. "Voltage control of ferromagnetic resonance." Journal of Advanced Dielectrics 06, no. 02 (2016): 1630005. http://dx.doi.org/10.1142/s2010135x1630005x.

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Voltage control of magnetism in multiferroics, where the ferromagnetism and ferroelectricity are simultaneously exhibiting, is of great importance to achieve compact, fast and energy efficient voltage controllable magnetic/microwave devices. Particularly, these devices are widely used in radar, aircraft, cell phones and satellites, where volume, response time and energy consumption is critical. Researchers realized electric field tuning of magnetic properties like magnetization, magnetic anisotropy and permeability in varied multiferroic heterostructures such as bulk, thin films and nanostruct
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14

Öner, Y., B. Aktaş, F. Apaydin, and E. A. Harris. "Ferromagnetic resonance study ofNi79Mn21alloy." Physical Review B 37, no. 10 (1988): 5866–69. http://dx.doi.org/10.1103/physrevb.37.5866.

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15

Sasaki, Y., X. Liu, J. K. Furdyna, M. Palczewska, J. Szczytko, and A. Twardowski. "Ferromagnetic resonance in GaMnAs." Journal of Applied Physics 91, no. 10 (2002): 7484. http://dx.doi.org/10.1063/1.1447214.

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16

Kohmoto, Osamu. "Ferromagnetic Resonance in Ca0.995La0.005B6." Japanese Journal of Applied Physics 41, Part 1, No. 11A (2002): 6358–59. http://dx.doi.org/10.1143/jjap.41.6358.

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17

Guan, Y., and W. E. Bailey. "Dual-frequency ferromagnetic resonance." Review of Scientific Instruments 77, no. 5 (2006): 053905. http://dx.doi.org/10.1063/1.2204907.

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18

Goennenwein, S. T. B., S. W. Schink, A. Brandlmaier, et al. "Electrically detected ferromagnetic resonance." Applied Physics Letters 90, no. 16 (2007): 162507. http://dx.doi.org/10.1063/1.2722027.

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19

Denysenkov, V. P., and A. M. Grishin. "Broadband ferromagnetic resonance spectrometer." Review of Scientific Instruments 74, no. 7 (2003): 3400–3405. http://dx.doi.org/10.1063/1.1581395.

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20

Lasley-Hunter, B., D. Hunter, Maxim Noginov, et al. "Ferromagnetic resonance studies in ZnMnO dilute ferromagnetic semiconductors." Journal of Applied Physics 99, no. 8 (2006): 08M116. http://dx.doi.org/10.1063/1.2172218.

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21

Xu, Wentao, D. B. Watkins, L. E. DeLong, K. Rivkin, J. B. Ketterson, and V. V. Metlushko. "Ferromagnetic resonance study of nanoscale ferromagnetic ring lattices." Journal of Applied Physics 95, no. 11 (2004): 6645–47. http://dx.doi.org/10.1063/1.1667452.

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22

Bhat, V. S., J. Sklenar, B. Farmer, et al. "Ferromagnetic resonance study of eightfold artificial ferromagnetic quasicrystals." Journal of Applied Physics 115, no. 17 (2014): 17C502. http://dx.doi.org/10.1063/1.4859035.

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23

Pashaev, Kh M., and D. L. Mills. "Ferromagnetic-resonance spectrum of exchange-coupled ferromagnetic bilayers." Physical Review B 43, no. 1 (1991): 1187–89. http://dx.doi.org/10.1103/physrevb.43.1187.

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24

Puzic, Aleksandar, Bartel Van Waeyenberge, Kang Wei Chou, et al. "Spatially resolved ferromagnetic resonance: Imaging of ferromagnetic eigenmodes." Journal of Applied Physics 97, no. 10 (2005): 10E704. http://dx.doi.org/10.1063/1.1860971.

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25

Miyadai, Tomonao, Tadashi Sekiguchi, Akira Shinogi, and Keizo Endo. "Ferromagnetic Resonance in a Ferromagnetic Heusler Alloy Co2TiAl." Journal of the Physical Society of Japan 54, no. 4 (1985): 1650–51. http://dx.doi.org/10.1143/jpsj.54.1650.

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26

Sakata, M., T. Kawasaki, T. Shibue, S. Tsuruta, H. Yoshimura, and H. Namiki. "3P135 Magnetic tests and ferromagnetic resonance on Daphnia resting eggs." Seibutsu Butsuri 45, supplement (2005): S237. http://dx.doi.org/10.2142/biophys.45.s237_3.

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27

Wang, Xin, Li Zhang, Meng Ran Guan, Jian Liang Xie, and Long Jiang Deng. "A Ferromagnetic Resonance Numerical Computation Method of Ferromagnetic Nano-Sphere." Advanced Materials Research 643 (January 2013): 157–61. http://dx.doi.org/10.4028/www.scientific.net/amr.643.157.

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We have studied the approach for dynamic micromagnetic equilibrium conditions (Brown’s equations) in terms of nucleation theory provide micromagnetic solutions for linearized forms of the equilibrium equations. We focus on the case of ferromagnetic resonance here described for a ferromagnetic sphere with uniform magnetization and with no losses. With the linear approximation we have derived uniform and symmetric resonance mode to the micromagnetic equations describing the dynamic properties of the near single-domain states by ignoring the magnetostatic potential gradient in symmetric case. Mor
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28

Ohta, H., S. Okubo, H. Kikuchi, and S. Ono. "Millimetre-wave ESR (electron-spin resonance) measurements of frustrated system ZnCr2xGa2–2xO4." Canadian Journal of Physics 79, no. 11-12 (2001): 1387–91. http://dx.doi.org/10.1139/p01-089.

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The magnetic properties of a three-dimensional topological frustrated system ZnCr2xGa2-2xO4, which is an anti-ferromagnet with a spinel structure, have been investigated by our millimetre-wave ESR (electron-spin resonance) measurements using the pulsed magnetic field up to 16 T in the temperature region from 1.8 to 265 K. In the high-temperature region, typical Cr3+ EPR (electron-paramagnetic resonance) with the g-value of 1.95 was observed. For the x = 1 sample, AFMR (anti-ferromagnetic resonance) with the easy-plane-type magnetic anisotropy was observed below TN. It turned out that the anti-
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29

García-Miquel, H., J. M. García, J. M. García-Beneytez, M. Vázquez, and G. Kurlyandskaya. "Resonancia ferromagnética en vidrios metálicos." Boletín de la Sociedad Española de Cerámica y Vidrio 39, no. 3 (2000): 367–70. http://dx.doi.org/10.3989/cyv.2000.v39.i3.860.

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30

Sobolev, Nikolai A., Marcio A. Oliveira, Vitor S. Amaral, et al. "Ferromagnetism and Ferromagnetic Resonance in Mn Implanted Si and GaAs." Materials Science Forum 514-516 (May 2006): 280–83. http://dx.doi.org/10.4028/www.scientific.net/msf.514-516.280.

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Ferromagnetism persisting above 375 K and anisotropic ferromagnetic resonance (FMR) spectra have been detected for the first time in Si co-implanted with Mn and As and annealed under appropriate conditions. For comparison, semi-insulating GaAs samples have been implanted with the same ions and subsequently annealed. They also exhibit ferromagnetism with a Curie temperature well in excess of 375 K. High-resolution transmission electron microscopy (TEM) performed on the samples with the best magnetic characteristics has shown the presence of nanoclusters due to the segregation of the implanted s
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31

Adar, Eliezer, Serghei A. Baranov, Nikolai A. Sobolev, and Anatolii M. Yosher. "Ferromagnetic resonance in cast microwires and its application for the non-contact diagnostics." Moldavian Journal of the Physical Sciences 1-2, no. 19 (2020): 89–97. https://doi.org/10.5281/zenodo.4118691.

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Ferromagnetic resonance in glass-coated Fe-based cast amorphous microwires reveals large residual stresses appearing in the microwire core during casting. These stresses, together with magnetostriction, determine the magnetoelastic anisotropy. Ferromagnetic resonance frequency is affected, in addition to residual and internal stresses, by external stresses applied to the microwire or a composite containing it (so-called stress effect). The dependence of ferromagnetic resonance frequency on the deformation of microwires is proposed to be used in the distant diagnostics of dangerous deformations
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32

Vetoshko, P. M., V. S. Vlasov, V. G. Shavrov, and V. I. Shcheglov. "Effect of Elastic Resonances of Substrate on Ferromagnetic Resonance in Yttrium Iron Garnet Films." Радиотехника и электроника 68, no. 2 (2023): 157–64. http://dx.doi.org/10.31857/s0033849423020146.

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The problem of excitation of ferromagnetic resonance in a thin ferrite film with magnetoelastic properties located on a thick elastic substrate is considered. A model is proposed for the excitation of elastic modes in the substrate due to the propagation of a periodic boundary regime created by magnetic oscillations in the film. The conditions for stationary oscillations are used to obtain the frequency response characteristics of ferromagnetic resonance, which exhibit strong oscillations due to the excitation of high-order elastic modes over the thickness of the substrate.
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33

Rinkevich, Anatoly B., Dmitry V. Perov, Elena A. Tolmacheva, Evgeny A. Kuznetsov, Olga V. Nemytova, and Mikhail A. Uimin. "Magnetic and Microwave Properties of Nanocomposites Containing Iron Particles Encapsulated in Carbon." Materials 15, no. 15 (2022): 5124. http://dx.doi.org/10.3390/ma15155124.

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The magnetic and microwave properties of nanocomposites containing iron particles encapsulated in a carbon shell (Fe@C), as well as carbon nanotubes (CNT), have been experimentally studied. The examination of magnetic properties of composites shows that the materials under study contain a ferromagnetic component. The availability of ferromagnetic ordering for the dielectric matrix-based nanocomposite sample with Fe@C particles has been confirmed by the measurement results of the transmission and the reflection coefficients of the microwaves, since the ferromagnetic resonance has been observed.
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34

Bhide, M. K., R. M. Kadam, A. K. Tyagi, et al. "Unusual magnetic properties of Mn-doped ThO2 nanoparticles." Journal of Materials Research 23, no. 2 (2008): 463–72. http://dx.doi.org/10.1557/jmr.2008.0064.

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We report the synthesis of Th1–xMnxO2 (x = 0, 0.001, 0.002, 0.004, and 0.01 wt%) nanoparticles by the urea combustion method using thorium nitrate gel followed by heat treatment at a higher temperature (T). The obtained Th1–xMnxO2 nanocrystals were characterized by x-ray diffraction (XRD), direct-current magnetization (M) measurements and electron paramagnetic resonance (EPR). XRD analysis revealed that Th1–xMnxO2 crystallizes in the cubic structure (Fm3m). M measurements showed ferromagnetic ordering at room temperature for Th0.99Mn0.01O2 samples annealed at 775 K. An intense and broad ferrom
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35

Bar'yakhtar, V. G., and V. A. Popov. "Ferromagnetic resonance in the nonhomogeneous intermediate state of a ferromagnet." Physica B: Condensed Matter 269, no. 2 (1999): 123–38. http://dx.doi.org/10.1016/s0921-4526(99)00103-9.

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36

Hu, Jing-guo, Guo-jun Jin, and Yu-qiang Ma. "Ferromagnetic resonance and exchange anisotropy in ferromagnetic/antiferromagnetic bilayers." Journal of Applied Physics 91, no. 4 (2002): 2180–85. http://dx.doi.org/10.1063/1.1433927.

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37

Usov, N. A. "Ferromagnetic resonance in thin ferromagnetic film with surface anisotropy." Journal of Magnetism and Magnetic Materials 474 (March 2019): 118–21. http://dx.doi.org/10.1016/j.jmmm.2018.10.134.

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38

Takahashi, S., S. Hikino, M. Mori, J. Martinek, and S. Maekawa. "Supercurrent pumping by ferromagnetic resonance in ferromagnetic Josephson junctions." Physica C: Superconductivity and its Applications 463-465 (October 2007): 989–92. http://dx.doi.org/10.1016/j.physc.2007.02.045.

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39

S, Aksoy, Posth O, Acet M, et al. "Ferromagnetic resonance in Ni-Mn based ferromagnetic Heusler alloys." Journal of Physics: Conference Series 200, no. 9 (2010): 092001. http://dx.doi.org/10.1088/1742-6596/200/9/092001.

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40

Yu, Chengtao, Michael J. Pechan, Swedesh Srivastava, et al. "Ferromagnetic resonance in ferromagnetic/ferroelectric Fe∕BaTiO3∕SrTiO3(001)." Journal of Applied Physics 103, no. 7 (2008): 07B108. http://dx.doi.org/10.1063/1.2834243.

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41

Liu, Xinyu, Xiang Li, Seul-Ki Bac, et al. "Ferromagnetic resonance and spin-wave resonances in GaMnAsP films." AIP Advances 8, no. 5 (2018): 056402. http://dx.doi.org/10.1063/1.5006090.

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42

Genkin, G. M., M. V. Sapozhnikov, and I. D. Tokman. "Frequencies of ferromagnetic resonance of ferromagnet-antiferromagnet-ferromagnet (FM/AFM/FM) trilayers." Journal of Magnetism and Magnetic Materials 131, no. 3 (1994): 369–84. http://dx.doi.org/10.1016/0304-8853(94)90282-8.

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43

Gorbachev, Evgeny A., Lev A. Trusov, Liudmila N. Alyabyeva, et al. "High-coercivity hexaferrite ceramics featuring sub-terahertz ferromagnetic resonance." Materials Horizons 9, no. 4 (2022): 1264–72. http://dx.doi.org/10.1039/d1mh01797g.

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Dense ceramics were obtained by annealing single-domain Al-doped hexaferrite particles. The materials possess giant coercivities and natural ferromagnetic resonance at 160–280 GHz. A large blueshift of the ferromagnetic resonance frequency was found.
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44

Gorelik, L. Yu, and S. I. Kulinich. "Collisionless microwave energy absorption by a breather gas in a one-dimensional magnet." Soviet Journal of Low Temperature Physics 12, no. 8 (1986): 494–95. https://doi.org/10.1063/10.0031563.

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The collisionless absorption of energy from a microwave field polarized along the ground state of a ferromagnet by a breather gas is studied. It is established that the energy absorbed by the breather subsystem as a function of the external frequency has a sharp peak, lying below the doubled frequency of the homogeneous ferromagnetic resonance.
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45

Скороходов, Е. В., М. В. Сапожников та В. Л. Миронов. "Магнитно-резонансная силовая спектроскопия массива микрополосок пермаллоя". Письма в журнал технической физики 44, № 5 (2018): 49. http://dx.doi.org/10.21883/pjtf.2018.05.45707.17101.

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AbstractThe ferromagnetic resonance in an array of permalloy microstrips 3000 × 500 × 30 nm in size ordered on a rectangular grid 3.5 × 6 μm in size has been investigated by magnetic resonance force microscopy. The dependences of magnetic resonance force microscopy spectra of a sample on the probe–sample distance are analyzed. The possibility of detection of a ferromagnetic resonance spectrum of a single microstrip is demonstrated.
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46

Lv, Ming Jun, Xin Zhao, Xiang Dong Zhao, Jian Guo Liu, Feng Zhen Liu, and Yan Hui Sun. "Analysis and Prevention of Grid Over-Voltage Ferromagnetic Resonance." Advanced Materials Research 960-961 (June 2014): 929–34. http://dx.doi.org/10.4028/www.scientific.net/amr.960-961.929.

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Over-voltage in the power system can be caused by a lot of reasons , including higher frequency ferromagnetic resonance overvoltage which occurs in normal operation and causes great harm. Overvoltage events often result in damages to electrical equipment or even power outages . In this paper,ferromagnetic resonance is analyzed to study harm , causes, conditions , and phenomena and to handle resonance and develop practical preventive measures. The related analysis is important to work for the future operation of the power grid to prevent and limit the ferromagnetic resonance over voltage which
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47

Noginova, N., V. Gubanov, M. Shahabuddin, et al. "Ferromagnetic Resonance in Permalloy Metasurfaces." Applied Magnetic Resonance 52, no. 7 (2021): 749–58. http://dx.doi.org/10.1007/s00723-021-01347-w.

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48

Fang, D., H. Kurebayashi, J. Wunderlich, et al. "Spin–orbit-driven ferromagnetic resonance." Nature Nanotechnology 6, no. 7 (2011): 413–17. http://dx.doi.org/10.1038/nnano.2011.68.

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