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"But we feel it is on the cusp, at an inflection point.
ρ versus T curve shows a cusp at T ρ. ρ decreases rapidly below T ρ.
ρ versus T curve shows a cusp at T ρ. c.
Conditions for G3 continuous contact with circles are then studied and it turns out that an ordinary cusp at each end of the evolute solution is required.
Thus, geometric properties of a family of PH polynomial quartics, allowing to generate such an ordinary cusp at one end, are studied.
All ZFC curves in Figs. 2 and 3 demonstrate cusp at low temperatures: very sharp for the Sp1 and smoother for the Sp2 ribbons.
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Shallow energy cusps at coincidence site lattice (CSL) misorientations were found.
As can be seen from the figure, the longitudinal magnetoresistance dependencies demonstrate the expressed cusps at fields up to 1.0 T.
Since the maximum Y current densities occur in the cusps at latitudes near −52° and −62°, the maximum generated magnetic field also occurs in this region between latitudes −50° and −65°.
For hyperbolic spaces obtained as quotients Γ⧹Hn + 1, where Γ is a discrete group of fractional linear transformations having a geometrically finite fundamental domain without cusps at infinity, s is constant.
In both the simulations and experiments, the activation energies and the logarithm of the pre-exponential factor in the mobility exhibited very similar variations with misorientation, including the presence of distinct cusps at low Σ misorientations.
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