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Reorientation transition

In addition to the hexagonal-square transition, a reorientation transition of the hexagonal vortex lattice from a state with the diagonal of the rhombic unit cell along [110] direction to [100] direction has been observed for YNi2B2C (Paul et al. 1998). Figure 51b shows that for H applied perpendicular to c the transition to a (nearly) square lattice occurs at a field of about 1 Tesla and at 0.8 Tesla a reorientation transition of the diagonal of the rhombic cell takes place (Sakata et al. 2000). [Pg.274]

The symmetry changes of the vortex lattice in borocarbide superconductors affect their pinning properties as was shown for YNi2B2C (Silhanek et al. 2001). For the field orientation // c, the reorientation transition of the vortex lattice mentioned above was found to be associated with a significant kink in the volume pinning force Fp, whereas in the basal plane (for H c) the signature of nonlocal effects is a fourfold periodicity of Fp. [Pg.275]

Ivanova, T.I., Pastushenkov, Yu.G., Skokov, K.P., Telegina, I.V., Tskhadadze, I.A. (1998) Spin-reorientation transitions and magnetic anisotropy in TbFen-xCoxTi compounds, J.Alloys Comp. 280 20-25. [Pg.491]

The intrinsic magnetic properties of the Er2Fei4B intermetallic compound have been previously investigated [1], According to the literature data [1,2] the magnetic ordering temperature of this compound is Tc = 554 K. Er2Fei4B exhibits one successive spin reorientation transition (SRT) at about 325 - 327 K. [Pg.605]

The aim of this work is to study the effect of hydrogenation on the magnetic phase transitions (Curie and spin-reorientation transition temperatures) in the Er2Fei4B compound using the magnetization measurements with continuous control of the hydrogen content in the examined sample. [Pg.605]

Figure 3. The dependence of spin-reorientation transition temperature on the hydrogen pressure for Er2Fei4BHx. Figure 3. The dependence of spin-reorientation transition temperature on the hydrogen pressure for Er2Fei4BHx.
The spin-reorientation transition in Er2Fei4B compound can be attributed to the competing of the uniaxial Fe sub lattice and the planar rare-earth sublattice anisotropy, with the former being dominant at higher temperatures and the latter being dominant at lower ones. [Pg.609]

A. Alavi, R. Lynden-Bell, and R. Brown (1999) Displacement and distortion of the ammonium ion in reorientational transition states of ammonium chloride and ammonium fluoride. J. Chem. Phys. 110, p. 5861... [Pg.275]


See other pages where Reorientation transition is mentioned: [Pg.100]    [Pg.253]    [Pg.254]    [Pg.334]    [Pg.253]    [Pg.255]    [Pg.287]    [Pg.173]    [Pg.486]    [Pg.599]    [Pg.605]    [Pg.607]    [Pg.610]    [Pg.612]    [Pg.24]    [Pg.486]    [Pg.599]    [Pg.605]    [Pg.607]    [Pg.610]    [Pg.612]    [Pg.256]    [Pg.349]    [Pg.74]    [Pg.202]    [Pg.244]    [Pg.244]    [Pg.249]    [Pg.258]    [Pg.362]    [Pg.362]    [Pg.321]    [Pg.324]    [Pg.326]   
See also in sourсe #XX -- [ Pg.253 , Pg.255 , Pg.256 , Pg.266 , Pg.283 , Pg.287 , Pg.304 ]




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Glass transition temperature molecular reorientation mechanism

Reorientation

Reorientational

Spin-reorientation transition

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