2020
DOI: 10.1103/physreve.102.022804
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Experimental exploration of dynamic phase transitions and associated metamagnetic fluctuations for materials with different Curie temperatures

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Cited by 23 publications
(12 citation statements)
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“…Overall, presence of sidebands in the kinetic Ising model has been theoretically confirmed by a variety of methods including the MFT [94], EFT [98] and MC simulations based on Metropolis and Glauber dynamics [37] thereby supporting the experimental observations [94]. DPT and metamagnetic anomalies have also been experimentally realized at room temperature for epitaxial Co 1−x Ru x films with uniaxial in-plane anisotropy for Ru content ranging between 0.0 ⩽ x ⩽ 0.26 [99] for which T c decreases as the Ru concentration increases. As shown in figure 7, although the qualitative evolution of the sidebands are not sensitive to varying x values, quantitative behavior of metamagnetic anomalies of Co 1−x Ru x films are found to be strongly dependent on the T/T c ratio, since the side band peaks become enhanced with increasing x.…”
Section: Metamagnetic Anomaliessupporting
confidence: 61%
“…Overall, presence of sidebands in the kinetic Ising model has been theoretically confirmed by a variety of methods including the MFT [94], EFT [98] and MC simulations based on Metropolis and Glauber dynamics [37] thereby supporting the experimental observations [94]. DPT and metamagnetic anomalies have also been experimentally realized at room temperature for epitaxial Co 1−x Ru x films with uniaxial in-plane anisotropy for Ru content ranging between 0.0 ⩽ x ⩽ 0.26 [99] for which T c decreases as the Ru concentration increases. As shown in figure 7, although the qualitative evolution of the sidebands are not sensitive to varying x values, quantitative behavior of metamagnetic anomalies of Co 1−x Ru x films are found to be strongly dependent on the T/T c ratio, since the side band peaks become enhanced with increasing x.…”
Section: Metamagnetic Anomaliessupporting
confidence: 61%
“…To achieve good epitaxial quality and the particular crystal orientation that contains the c-axis within the surface plane and thus induces an in-plane easy magnetization axis, a specific growth sequence has been used, that is described in detail in prior work [44,45]. Specifically, the sequence of sample S1 includes a hydrofluoric acid etched Si (110) substrate, 35 nm of Ag (110), 10 nm of Cr (211), 20 nm of Co 74 Ru 26 (1010), and a 10 nm SiO 2 overcoat, which was deposited to avoid surface oxidation and contaminations of the magnetic CoRu layer [46]. The second sample (S2) consists of a 50 nm thick yttrium iron garnet (YIG) layer deposited on a thermally oxidized Si substrate via radiofrequency magnetron sputtering and post-annealed in atmosphere at 750 • C for 1 h. On top of this layer, a 0.3 nm Ni 80 Fe 20 layer and a 1 nm Pt overcoat have also been sputtered deposited in succession to protect the sample [47].…”
Section: Samplesmentioning
confidence: 99%
“…Recently, the experimental observations of Refs. 16,36 have been supported by some theoretical studies [37][38][39][40] . In the following, we present our simulation results for the present model.…”
Section: Metamagnetic Anomaliesmentioning
confidence: 77%