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Journal articles on the topic 'Ferromagnetic resonance'

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Author: Grafiati
Published: 4 June 2021
Last updated: 7 September 2023

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1

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

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2

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 resonance. It has been established that effectively exciting nonlinear oscillations of the domain wall in uniaxial ferromagnets and controlling the wall dynamics by low-amplitude alternating fields with the slow variation of the planar field in the autophasing mode are possible in the case of weak dissipation.
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3

Lee, Yong Heng, and Ramanathan Mahendiran. "Transport and electron spin resonance studies in Mo-doped LaMnO3." AIP Advances 13, no. 2 (February 1, 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 non-linear field dependence of magnetization. The magnetic resonance spectra shows both paramagnetic and ferromagnetic resonance signals between 240 and 260 K. It is suggested that the ferromagnetic clusters enlarge in size with lowering temperature and percolate leading to long-range ferromagnetism and metallicity.
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4

Tatarsky D. A., Skorokhodov E. V., Mironov V. L., and Gusev S. A. "Ferromagnetic resonance in exchange-coupled magnetic vortices." Physics of the Solid State 64, no. 9 (2022): 1319. http://dx.doi.org/10.21883/pss.2022.09.54174.40hh.

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The results of a study of low-frequency ferromagnetic resonance in a system of two overlapping permalloy disks by magnetic resonance force spectroscopy are presented. It is shown that the resonant frequency of the gyrotropic mode of oscillations of magnetic vortices in this system significantly depends on the vorticity of their shells. The experimental dependences of the resonant frequencies of various states on the external magnetic field are qualitatively consistent with the results of micromagnetic modeling. Keywords: ferromagnetic resonance, magnetic resonance force spectroscopy, magnetic vortices.
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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 (October 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 (December 21, 1997): 3312–16. http://dx.doi.org/10.1088/0022-3727/30/24/008.

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7

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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8

Zhou, Ziyao, Bin Peng, Mingmin Zhu, and Ming Liu. "Voltage control of ferromagnetic resonance." Journal of Advanced Dielectrics 06, no. 02 (June 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 nanostructure by different magnetoelectric (ME) coupling mechanism: strain/stress, interfacial charge, spin–electromagnetic (EM) coupling and exchange coupling, etc. In this review, we focus on voltage control of ferromagnetic resonance (FMR) in multiferroics. ME coupling-induced FMR change is critical in microwave devices, where the electric field tuning of magnetic effective anisotropic field determines the tunability of the performance of microwave devices. Experimentally, FMR measurement technique is also an important method to determine the small effective magnetic field change in small amount of magnetic material precisely due to its high sensitivity and to reveal the deep science of multiferroics, especially, voltage control of magnetism in novel mechanisms like interfacial charge, spin–EM coupling and exchange coupling.
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9

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 (June 2011): 1653–57. http://dx.doi.org/10.1109/tmag.2011.2116160.

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10

Öner, Y., B. Aktaş, F. Apaydin, and E. A. Harris. "Ferromagnetic resonance study ofNi79Mn21alloy." Physical Review B 37, no. 10 (April 1, 1988): 5866–69. http://dx.doi.org/10.1103/physrevb.37.5866.

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11

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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12

Kohmoto, Osamu. "Ferromagnetic Resonance in Ca0.995La0.005B6." Japanese Journal of Applied Physics 41, Part 1, No. 11A (November 15, 2002): 6358–59. http://dx.doi.org/10.1143/jjap.41.6358.

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13

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

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14

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

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15

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

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16

Lasley-Hunter, B., D. Hunter, Maxim Noginov, J. B. Dadson, K. Zhang, R. R. Rakhimov, A. K. Pradhan, Jun Zhang, and D. J. Sellmyer. "Ferromagnetic resonance studies in ZnMnO dilute ferromagnetic semiconductors." Journal of Applied Physics 99, no. 8 (April 15, 2006): 08M116. http://dx.doi.org/10.1063/1.2172218.

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17

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 (June 2004): 6645–47. http://dx.doi.org/10.1063/1.1667452.

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18

Bhat, V. S., J. Sklenar, B. Farmer, J. Woods, J. B. Ketterson, J. T. Hastings, and L. E. De Long. "Ferromagnetic resonance study of eightfold artificial ferromagnetic quasicrystals." Journal of Applied Physics 115, no. 17 (May 7, 2014): 17C502. http://dx.doi.org/10.1063/1.4859035.

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19

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

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20

Puzic, Aleksandar, Bartel Van Waeyenberge, Kang Wei Chou, Peter Fischer, Hermann Stoll, Gisela Schütz, Tolek Tyliszczak, et al. "Spatially resolved ferromagnetic resonance: Imaging of ferromagnetic eigenmodes." Journal of Applied Physics 97, no. 10 (May 15, 2005): 10E704. http://dx.doi.org/10.1063/1.1860971.

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21

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 (April 15, 1985): 1650–51. http://dx.doi.org/10.1143/jpsj.54.1650.

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22

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 connected in the PT primary neutral side and small resistance is connected in the PT open delta are effectively methods which can restrain ferromagnetic resonance overvoltage.
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23

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 (June 30, 2000): 367–70. http://dx.doi.org/10.3989/cyv.2000.v39.i3.860.

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24

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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25

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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26

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 (October 1, 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 practicable.
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27

Vazhenina I.G., Stolyar S.V., Tyumentseva A.V., Volochaev M.N., Iskhakov R.S., Komogortsev S.V., Pyankov V. F., and Nikolaeva E.D. "Study of magnetic iron oxide nanoparticles coated with silicon oxide by ferromagnetic method." Physics of the Solid State 65, no. 6 (2023): 884. http://dx.doi.org/10.21883/pss.2023.06.56095.01h.

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Magnetic nanoparticles of magnetite with a size of ~8 nm synthesized with a different type of coating were studied by ferromagnetic resonance in the temperature range from 7 to 300 K. The features of the experimental temperature dependences of the parameters of the ferromagnetic resonance curve (the magnitude of the resonant field, line width and intensity) and their approximation allowed us to estimate the values of characteristic temperatures. Firstly, the value of the Vervey temperature and the dependence of its value on the type of coating were determined. Secondly, the temperature of transition of nanoparticles to the superparamagnetic state (blocking temperature) and the temperature range within which the magnetic structure of the outer shell of the magnetic nanoparticle is in the spin glass state are established Keywords: iron oxide nanoparticles, ferromagnetic resonance, superparamagnetism, blocking temperature.
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28

Couture, P., S. Goldman, R. E. Camley, E. Iacocca, K. L. Livesey, T. Robinson, D. Meyers, S. Maat, H. T. Nembach, and Z. Celinski. "Ferromagnetic resonance of hollow micron-sized magnetic cylinders." Applied Physics Letters 121, no. 20 (November 14, 2022): 202403. http://dx.doi.org/10.1063/5.0124550.

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We have explored dynamic magnetic properties of micron-sized Ni-coated carbon fibers embedded in a polymer matrix for electromagnetic interference shielding applications. These hollow magnetic cylinders exhibit unusual dynamic magnetic properties, which were measured with a broad-band ferromagnetic resonance system (FMR). We observe three families of FMR modes, which are connected to different physical locations within the cylinder. We develop a simple analytic model to explain these results and corroborate resonant mode profiles with micromagnetic simulations. We find excellent agreement between experimental results and theoretical models. Our work indicates that global demagnetizing factors are not appropriate for understanding the spin motions in these hollow cylinders. The FMR absorption observed in these hallow cylinders is very different from those observed in nanowires or solid cylinders. The field-swept envelope of all the observed FMR resonances is very broad, approximately [Formula: see text] = 1 T, with a linewidth of individual modes around [Formula: see text] = 250 mT. This can be important for electromagnetic shielding applications.
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29

Shi, Yun Bo, Hui Xue, Zong Min Ma, Huan Zhang, Jun Tang, Chen Yang Xue, Jun Liu, and Yan Jun Li. "Observation of Ferromagnetic Resonance in Magnetic Exchange Force Microscopy (MExFM)." Key Engineering Materials 609-610 (April 2014): 1392–97. http://dx.doi.org/10.4028/www.scientific.net/kem.609-610.1392.

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The atomic spin interaction is very important for understanding the superficially magnetic feature of nanostructure at atomic level. Magnetic exchange force microscopy (MExFM) is an innovative means of measuring surface spin force. But it is difficult to separate the surface topography and spin information. We develop the magnetic exchange force microscopy using ferromagnetic resonance (FMR-MExFM). The theoretical and experimental results demonstrate that this method can separate the two kinds of information effectively. Here, in order to obtain the high sensitivity in detecting the ferromagnetic resonance, we fabricate the microwave irradiation device to optimize the position between the device and the cantilever. We have succeeded in observing the ferromagnetic resonance effect and determining its resonant frequency using the homemade microwave irradiation device and the network analyzer. This research is very important for developing FMR-MExFM and novel magnetic sensor, detecting the magnetic information, etc.
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30

Sobolev, Nikolai A., Marcio A. Oliveira, Vitor S. Amaral, Armando Neves, M. Celeste Carmo, Werner Wesch, Oliver Picht, Elke Wendler, Ute Kaiser, and J. Heinrich. "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 species in both Si and GaAs. The angular dependence of the FMR spectra also reveals the existence of magnetic clusters with the hard magnetization axis aligned along the four equivalent <111> crystal axes. The spectra are very similar in Si and GaAs, indicating that the clusters in both materials probably consist of hexagonal MnAs.
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31

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. Moreover, using numerical integration solution to calculate exchange and magnetic energy, both resonance modes are proved to be effective approximate solution of Brown’s equations in the nanometer range.
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32

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 (February 15, 2002): 2180–85. http://dx.doi.org/10.1063/1.1433927.

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33

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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34

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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35

S, Aksoy, Posth O, Acet M, Meckenstock R, Lindner J, Farle M, and Wassermann E. F. "Ferromagnetic resonance in Ni-Mn based ferromagnetic Heusler alloys." Journal of Physics: Conference Series 200, no. 9 (January 1, 2010): 092001. http://dx.doi.org/10.1088/1742-6596/200/9/092001.

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36

Yu, Chengtao, Michael J. Pechan, Swedesh Srivastava, Chris J. Palmstrøm, Michael Biegaslski, Charles Brooks, and Darrell Schlom. "Ferromagnetic resonance in ferromagnetic/ferroelectric Fe∕BaTiO3∕SrTiO3(001)." Journal of Applied Physics 103, no. 7 (April 2008): 07B108. http://dx.doi.org/10.1063/1.2834243.

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37

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 (August 1999): 123–38. http://dx.doi.org/10.1016/s0921-4526(99)00103-9.

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38

Liu, Xinyu, Xiang Li, Seul-Ki Bac, Xucheng Zhang, Sining Dong, Sanghoon Lee, Margaret Dobrowolska, and Jacek K. Furdyna. "Ferromagnetic resonance and spin-wave resonances in GaMnAsP films." AIP Advances 8, no. 5 (May 2018): 056402. http://dx.doi.org/10.1063/1.5006090.

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39

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 (March 1994): 369–84. http://dx.doi.org/10.1016/0304-8853(94)90282-8.

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40

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 (December 1, 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-ferromagnetic gap opens up just below TN suggesting that the transition is of the first order. The x dependences of ESR were also observed and their temperature dependences of the g-value and the linewidth will be discussed in connection with those of other frustrated systems such as Kagome lattice substance. PACS Nos.: 75.50, 76.30-v, 75.40-s
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41

Noginova, N., V. Gubanov, M. Shahabuddin, Yu Gubanova, S. Nesbit, V. V. Demidov, V. A. Atsarkin, E. N. Beginin, and A. V. Sadovnikov. "Ferromagnetic Resonance in Permalloy Metasurfaces." Applied Magnetic Resonance 52, no. 7 (June 18, 2021): 749–58. http://dx.doi.org/10.1007/s00723-021-01347-w.

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42

Fang, D., H. Kurebayashi, J. Wunderlich, K. Výborný, L. P. Zârbo, R. P. Campion, A. Casiraghi, B. L. Gallagher, T. Jungwirth, and A. J. Ferguson. "Spin–orbit-driven ferromagnetic resonance." Nature Nanotechnology 6, no. 7 (May 22, 2011): 413–17. http://dx.doi.org/10.1038/nnano.2011.68.

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43

Jalalian, A., M. S. Kavrik, S. I. Khartsev, and A. M. Grishin. "Ferromagnetic resonance in Y3Fe5O12 nanofibers." Applied Physics Letters 99, no. 10 (September 5, 2011): 102501. http://dx.doi.org/10.1063/1.3633351.

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44

Qiu, Rong-ke, An-dong Huang, Da Li, and Zhi-dong Zhang. "Resonance frequency in ferromagnetic superlattices." Journal of Physics D: Applied Physics 44, no. 41 (September 26, 2011): 415002. http://dx.doi.org/10.1088/0022-3727/44/41/415002.

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45

Kohmoto, Osamu. "Erratum: “Ferromagnetic Resonance in Ca0.995La0.005B6”." Japanese Journal of Applied Physics 42, Part 1, No. 4A (April 15, 2003): 1834B. http://dx.doi.org/10.1143/jjap.42.1834b.

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46

De Biasi, E., C. A. Ramos, R. D. Zysler, and H. Romero. "Ferromagnetic resonance in amorphous nanoparticles." Physica B: Condensed Matter 354, no. 1-4 (December 2004): 286–89. http://dx.doi.org/10.1016/j.physb.2004.09.103.

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47

Wigen, P. E., M. Ye, and D. W. Peterman. "Controlling chaos in ferromagnetic resonance." Journal of Magnetism and Magnetic Materials 140-144 (February 1995): 2074–76. http://dx.doi.org/10.1016/0304-8853(94)00594-x.

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48

Boero, G., S. Rusponi, P. Bencok, R. S. Popovic, H. Brune, and P. Gambardella. "X-ray ferromagnetic resonance spectroscopy." Applied Physics Letters 87, no. 15 (October 10, 2005): 152503. http://dx.doi.org/10.1063/1.2089180.

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49

Zhuravlev, V. A., and E. P. Naiden. "Ferromagnetic resonance in hexaferrite nanopowders." Russian Physics Journal 51, no. 1 (January 2008): 38–44. http://dx.doi.org/10.1007/s11182-008-9026-1.

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50

Vidil, A. Yu, I. V. Zavislyak, and M. O. Popov. "Relaxation at Nonlinear Ferromagnetic Resonance." Ukrainian Journal of Physics 59, no. 2 (February 2014): 141–47. http://dx.doi.org/10.15407/ujpe59.02.0141.

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