“…Furthermore, a strong c-axis orientation texture generally indicates an intimate connection between the {0001} planes (perpendicular to the c-axes) of the PrCo 5 crystals. In particular, PrCo 5 has a c/a value of 0.798 and the [0001] hexagonal c-axis of the unit cell is the desirable texture axis, 11 presenting a favorable condition for the occurrence of the coincidence site lattice (CSL) boundary, Σ13a. 12 Here, the Σ value represents the reciprocal density of coinciding sites and the symmetrical configuration of the boundary planes.…”
We report a magnetically-anisotropic PrCo 5 permanent bulk magnet, prepared by a hot deformation method, with crystallographic orientation-dependent magnetic properties. Although the PrCo 5 crystals strongly favor the {0001} orientation texture, the crystallographic orientation textures of PrCo 5 crystallites differ at various radial locations. From the bulk center to the edge, the c-axis orientation texture decreases from 5.4 MRD to 4.1 MRD, whereas the remanence decreases from 8.93 kGs to 7.58 kGs and the coercivity increases from 4.34 kOe to 6.56 kOe. This paper also reports the alteration of boundary plane orientation textures, resulting from the corresponding energy anisotropy at different locations, and suggests that the development of grain boundaries with lower boundary energies has a significant impact on the magnetic properties with regard to remanence and energy density. The current work therefore proposes an elegant approach to attain desired magnetic properties in PrCo 5 magnets by fine-tuning the crystallographic orientation.
“…Furthermore, a strong c-axis orientation texture generally indicates an intimate connection between the {0001} planes (perpendicular to the c-axes) of the PrCo 5 crystals. In particular, PrCo 5 has a c/a value of 0.798 and the [0001] hexagonal c-axis of the unit cell is the desirable texture axis, 11 presenting a favorable condition for the occurrence of the coincidence site lattice (CSL) boundary, Σ13a. 12 Here, the Σ value represents the reciprocal density of coinciding sites and the symmetrical configuration of the boundary planes.…”
We report a magnetically-anisotropic PrCo 5 permanent bulk magnet, prepared by a hot deformation method, with crystallographic orientation-dependent magnetic properties. Although the PrCo 5 crystals strongly favor the {0001} orientation texture, the crystallographic orientation textures of PrCo 5 crystallites differ at various radial locations. From the bulk center to the edge, the c-axis orientation texture decreases from 5.4 MRD to 4.1 MRD, whereas the remanence decreases from 8.93 kGs to 7.58 kGs and the coercivity increases from 4.34 kOe to 6.56 kOe. This paper also reports the alteration of boundary plane orientation textures, resulting from the corresponding energy anisotropy at different locations, and suggests that the development of grain boundaries with lower boundary energies has a significant impact on the magnetic properties with regard to remanence and energy density. The current work therefore proposes an elegant approach to attain desired magnetic properties in PrCo 5 magnets by fine-tuning the crystallographic orientation.
“…Since its discovery in 1967, 1 the permanent magnet intermetallic compound SmCo 5 has been widely studied both experimentally 2 and theoretically. 3 As a promising candidate for thin film recording media, 4,5 the performances of the SmCo 5 magnet are determined by its crystallographic features to a large extent, which can be summarized as the following aspects: (1) in permanent magnets with uniaxial magnetic anisotropy, the saturation magnetization and the remanence are determined by the grain orientation texture, 6 which provides the information about grain alignment and helps to measure the efficiency in acquiring remanent magnetization; 7 (2) the SmCo 5 magnet has a high magnetocrystalline anisotropy constant of 1.1 × 10 8 erg cm −3 , 4 and the magnetocrystalline anisotropy parameter has a close relation to both magnetic hysteresis characteristics 2 and thermal fluctuation of the magnetic moment, 8 and particularly, locations with low magnetocrystalline anisotropy are often concentrated near grain boundaries; 9 (3) improving the corrosion resistance of the SmCo 5 magnet is an important issue, 5 and corrosion resistance has been demonstrated to be closely correlated to the distribution features of grain boundaries on a statistical basis, namely the "grain boundary character distribution (GBCD)". 10 In brief, characterizing the crystallographic textures of the SmCo 5 magnet has major significance.…”
Section: Introductionmentioning
confidence: 99%
“…3) and the [0001] hexagonal axis of the unit cell is the desirable texture axis, 6 which leads to the high frequency occurrence of a coincidence site lattice (CSL) boundary namely the Σ13a grain boundary; 11 here, the Σ value represents the reciprocal density of coinciding sites and the symmetrical configuration of boundary planes, and the basic crystallographic feature of the Σ13a boundary can be described as a 27.796°rotation about the [0001] axis (abbreviated as 27.796°/[0001]). Therefore, the crystallographic textures of the SmCo 5 magnet should include the orientation textures of both SmCo 5 grains and SmCo 5 /SmCo 5 grain boundary planes.…”
“…Until now, only transmission electron microscopy (TEM) had been used. 4. Permanent magnets based on the Sm 2 Co 17 phase present high intrinsic coercivities at high temperatures (up to 1 T at 500 C) which make them suitable for high technology applications.…”
mentioning
confidence: 99%
“…4 EBSD-orientation imaging microscopy (OIM) scans and EDS measurements were performed in a FEI Quanta 200 TSL/ SEM with a tungsten filament. 4 EBSD-orientation imaging microscopy (OIM) scans and EDS measurements were performed in a FEI Quanta 200 TSL/ SEM with a tungsten filament.…”
In permanent magnets based on the Sm2Co17 phase, the high coercivity depends on the presence of a complex microstructure, consisting of a Sm2(Co,Fe)17 cell phase, a cell boundary phase Sm(Co,Cu)5, and a Zr-rich platelet or lamellae phase. The aim of this work is to use electron back scatter diffraction (EBSD) in order to identify the different phases present in the isotropic magnets produced from cast alloys with the composition of Sm(CobalFe0.2Cu0.1Zrx)8, where x = 0, 0.02, or 0.06, and correlate them with the different phases observed in scanning electron microscopy (SEM) images. Due to the combination of careful surface preparation and high resolution microscopy, it was possible to observe the cellular structure characteristic of the 2:17 magnets in the SEM images. Until now, only transmission electron microscopy (TEM) had been used. Composition maps, energy dispersive spectroscopy (EDS), and EBSD measurements were used for doing the phase identification.
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