Influence of alloying additions on magnetostriction and Young's modulus of nanoperm type amorphous alloys
In the present paper magnetostriction, Young's modulus and primary crystallization were examined for a group of amorphous alloys of nanoperm family i.e. Fe78B22, Fe76B22X2 (X=Cr, Zr, Nb). It was shown that the alloying additions cause a correlated decrease of Young’s modulus (over 2 times) and magnetostriction coefficients - parallel (about 40%) and spontaneous (about 30 %) in rel[...]
Ferroelectric and ferromagnetic properties of the (1-x)NiZnFeO4 -(x)Pb(Fe1/2Nb1/2)O3 composite
According to the thermodynamic terminology of the multiferroics,
they are some ferroics of II and III order which have
simultaneously at least two spontaneously ordered subsystems
among the states: ferromagnetic FM, ferroelectric FE, ferroelastic
FES and ferrotoroidal FT [1÷3]. Possible application of the
multiferroics depend, first of all, on a degree of mutual coupling of
particular subsystems (magnetic, electric and elastic) [4].
Materials showing simultaneous electric (FE - ferroelectric,
AFE - antiferroelectric or FIE - ferrielectric) and magnetic
ordering (FM - ferromagnetic, AFM - antiferromagnetic or FIM
ferrimagnetic) are called ferroelectromagnetics (FEM) [5]. In the
ferroelectromagnetics both magnetic and electric properties can be
controlled by external factors, such as: a magnetic field, an electric
field, stress or temperature [6]. If a mutliferroic material is the
ferromagnetic and the ferroelectric at the same time, then it will be
characterized by magnetic response to a variable electric field, or
inversely, a polarization change in the external magnetic field.
This effect can be strengthened by making composite based on the
ferrites and the ferroelectric materials (multiferroics, biferroics,
ferroics). According to the classification, made by D. Khomsky,
the mutliferroic materials can be divided into multiferroics of
type-I and type-II [5]. PbFe1/2Nb1/2O3 (PFN) is one of the wellknown
ferroelectromagnetic materials. It has a structure of the
perovskite type of the ABO3 general formula, where A positions of
the unit cell are filled with big ions of lead Pb, whereas B
positions are filled alternately with (in a random way) ions of iron
Fe and niobium Nb [7, 8]. According to the classification of D.
Khomsky [5] PFN belongs to mutiferroics of type-I, in which
ferroelectricity is connected with a displacement of ferroelectrically
active ions d0 (Nb) from the centre of regular
octahedrons - O6, whereas magnetism is[...]