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A. Perevertov

Publications and source records attributed to A. Perevertov.

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Shape of temperature dependence of spontaneous magnetization of various ferromagnets

The shape of the temperature dependence of spontaneous magnetization was analyzed for about forty ferromagnetic materials. The squareness of the shape was determined by fitting the magnetization curves with the superellipse equation (Lame curve). The agreement between the Lame curve fits and the experimental data was good for most materials. The squareness parameter (the power coefficient in the superellipse equation was found to range from 1.4 to 3.0. The largest squareness was observed for iron, whereas the smallest was found for antiferromagnetic materials and the Ni55Cu45 alloy. The squareness parameter was studied as a function of the Curie temperature, TC. For metallic alloys, a general tendency was observed: the squareness increased with increasing Curie temperature. The only exception was cobalt, which exhibited the same magnetization curve in reduced coordinates as nickel despite having a Curie temperature twice as high. The addition of either ferromagnetic or nonferromagnetic metals to iron or nickel led to a decrease in squareness. No influence of the thermal expansion coefficient on the magnetization curve was observed: zero-expansion Invar exhibited a standard shape following the Lame curve.

cond-mat.mtrl-sci

Temperature dependence of the spontaneous magnetization of Ni2MnGa and other ferromagnets. The superellipse equation

The temperature dependence of the spontaneous magnetization of Ni2MnGa and other ferromagnets can be described in reduced coordinates by the superellipse equation using a single dimensionless parameter. This critical exponent parameter equals 2.4 for Ni2MnGa, 2.7 for nickel and cobalt, 3 for iron and 2.05 for gadolinium. Because reduced magnetization and reduced temperature enter the equation symmetrically, the MS(T) dependence can be measured only in the low-temperature range, from 0 to 0.5TC. The magnetization curve from 0.5TC to TC can then be obtained by interchanging reduced magnetization and temperature in the superellipse equation. In this way, the experimentally challenging task of measuring spontaneous magnetization near TC is avoided, as the behavior near TC is effectively determined from measurements performed near T = 0. The MS(T) dependence in a whole temperature range is fully determined by two parameters - the Curie temperature, TC and the critical exponent, n .

cond-mat.mtrl-sci

Kerr microscopy study of magnetic domains and their dynamics in bulk Ni-Mn-Ga austenite

The observation of magnetic domains on austenite Ni-Mn-Ga bulk samples has been a big challenge for many years. Using advanced Kerr microscopy, with automatic compensation of the sample motion and monochromatic LED light we were able to observe magnetic domains and follow their evolution with magnetic field on the _100_ faces of an austenite bulk single crystal. After mechanical polishing variable fine stress-induced domains patterns were observed at different locations. The surface coercivity visualized by the Kerr loop was two orders higher than the bulk coercivity from magnetometry measurement. After additional electropolishing, wide 180 domains were observed with a width of about 50 micrometers and the Kerr loop coercivity decreased to the level determined from the magnetometry. Surprisingly, the magnetic domains were observed only along one of two _100_ cubic axes lying in the surface plane.

cond-mat.mtrl-sci