68 research outputs found
The Influence of Yb Substitution on the Magnetic, Electric Properties and Electronic Structure of YbxGd1-xNi5 System
The crystal and electronic structure, magnetic and electric properties of intermetallic compounds
YbxGd1¡xNi5 (x = 0:0, 0.2, 0.4, 0.5) are presented. The whole series crystallize in the hexagonal CaCu5
type of crystal structure. The ordering temperatures TC and the e®ective magnetic moments decrease with
increase in ytterbium concentration. The electronic structure studied by X-ray photelectron spectroscopy method
shows the domination of Ni 3d states nearby the Fermi level. The multiplet structure visible in valence bands is
typical of Yb3+ ions
Influence of transition metal substitution on the low-field magnetic properties in the Gd(Ni1-xTx)3 (T = Fe, Co) intermetallic compounds
The low-field magnetic properties of polycrystalline Gd(Ni1 xTxq3 (T = Fe, Co) intermetallic compounds are
presented. The whole system crystallizes in the rhombohedral PuNi3 type of crystal structure. The composition
dependence of the Curie temperature TCpxq is associated with the change in the number of 3d electrons. Moreover,
the field cooled and zero field cooled (FC-ZFC) curves at low applied magnetic field are related to the anisotropy of T
element. The saturation magnetic moment MSpxq upon doping was estimated based on the hysteresis loops MpHq[…
Hyperfine interactions in RxGd1- xFe3 intermetallics R = Tb, Y
The structural and magnetic properties of rare earth iron intermetallic compounds TbxGd1-xFe3 and YxGd1-xFe3 (x = 0. 0, 0. 1, 0. 2, 0. 4, 0. 5, 0. 6, 0. 8, 1. 0) was studied by X-ray diffraction, the 57Fe Mössbauer effect and SQUID measurements. All investigated compounds crystallize in the rhombohedral PuNi3-type of crystal structure. The investigation of magnetic properties of RxGd1-xFe3 proved their ferrimagnetic behavior. The Curie temperature of the investigated compounds decreases with the increase of R concentration from 721K (GdFe3) to 655K (TbFe3) and 533K (YFe3). The saturation magnetic moment MS in the RxGd1-xFe3 system increase with x parameter. The Mössbauer spectra are analyzed using four sextets, corresponding to three crystallographically (b, c, h) and four magnetically (b, c, h1, h2) inequivalent sites for iron. The mean hyperfine magnetic field increases with increase of the Gd concentration
Influence of cr-atoms on the magnetic and electrical properties in Ho(Co1-xCrx)2 compounds
AC magnetic susceptibility, electrical resistivity and X-ray Photoelectron
Spectroscopy (XPS) measurements have been performed on the
Ho(Coi_a,Cra,)2 compounds with x=0.0, 0.03, 0.05, 0.10, 0.15 and 0.20.
A strengthening of the HoCo2 ferrimagnetism shows up through a rapid
increase at small Cr concentration x of the Curie temperature Tq which
reaches a maximum around x= 0.15. The lattice parameters also go through
a maximum for the same concentration of Cr. A remarkable decrease of
the density of states near the Fermi level is observed for the sample with
x= 0.20. We correlate the changes of the Curie temperature with the decrease
of d-electron concentration when Cr substitutes for Co[…
Effect of Tb/Gd substitution on crystal structure and exchange interactions of Gd1- xTb xNi 3 intermetallic compounds
In the paper an in uence of Tb/Gd substitution on crystal structure and exchange interactions of
Gd1xTbxNi3 (x = 0:0, 0.5, 0.8, 1.0) polycrystalline compounds have been studied. The crystal structure of all
samples was checked at the room temperature by means of X-ray di raction. Exchange integrals of R R (JRR),
T T (JTT) and R T (JRT) atoms were evaluated from M(T) magnetization curves (2 300 K, 2 T) based on
the mean eld theory calculation. As it was shown the samples examined are single phase and crystallize in
the PuNi3 (space group R-3m) type of crystal structure. The Tb/Gd substitution causes the decrease of lattice
parameters as well as the volume of the unit cell. With increase of the x parameter the magnetic moment of Tb
atoms increases from 6.94 B (x = 0:5) to 8.12 B (x = 1). The M(T) dependence of the examined compounds
depends almost 8 times stronger on exchange interactions within the R R site than the interactions between the
two antiferromagnetically coupled magnetic sublattices R T
Effect of alloying on magnetism and electronic structure of Gd(In1-xSnx)3 system - Ab initio study
We present the results of ab initio study of electronic and magnetic properties of Gd(In1xSnx)3 alloys carried
out with the use of FP-LAPW method. Our precise ab initio calculations for the rst time uniquelly con rmed
experimentally based predictions that the ground state magnetic structure of the alloys is antiferromagnetic and
that upon the In/Sn substitution the magnetic structure undergo transition, changing the antiferromagnetic ordering from the ( 00)-type for the GdSn3 compound to the ( 0)-type for the GdIn3 one. Moreover, calculations
gave an explanation of the oscillatory variation of density of states at Fermi level indicated by XPS measurements
Corrosion study of resorbable Ca60Mg15Zn25 bulk metallic glasses in physiological fluids
The corrosion activity of amorphous plates of Ca60Mg15Zn25 alloy was investigated. The biocompatible elements
were selected for the alloy composition. The electrochemical corrosion and immersion tests were carried out in a
multi-electrolyte fluid and Ringer's solution. Better corrosion behavior was observed for the samples tested in a
multi-electrolyte fluid despite the active dissolution of Ca and Mg in Ringer's solution. The experimental results
indicated that reducing concentration of NaCl from 8.6 g/dm3 for Ringer's solution to 5.75 g/dm3 caused the
decrease of the corrosion rate. The volume of the hydrogen evolved after 480 min in Ringer's solution (40.1 ml/
cm2) was higher in comparison with that obtained in a multi-electrolyte fluid (24.4 ml/cm2). The values of opencircuit
potential (EOCP) for the Ca60Mg15Zn25 glass after 1 h incubation in Ringer's solution and a multielectrolyte
fluid were determined to be −1553 and −1536 mV vs. a saturated calomel electrode (SCE). The
electrochemical measurements indicated a shift of the corrosion current density (jcorr) from 1062 μA/cm2 for
the sample tested in Ringer's solution to 788 μA/cm2 for the specimen immersed in a multi-electrolyte fluid. The
corrosion products analysis was conducted by using the X-ray photoelectron spectroscopy (XPS). The corrosion
products were identified to be CaCO3, Mg(OH)2, CaO, MgO and ZnO. The mechanism of corrosion process was
proposed and described based on the microscopic observations. The X-ray diffraction and Fourier transform
infrared spectroscopy (FTIR) also indicated that Ca(OH)2, CaCO3, Zn(OH)2 and Ca(Zn(OH)3)2·2H2O mainly
formed on the surface of the studied alloy.The work was supported by National Science Centre under research project no.: 2013/09/B/ST8/02129
Electrical resistivity and electronic structure of the Tb xGd 1-xNi 3 system
In the paper the electric properties and electronic structure of the intermetallic TbxGd1xNi3 compounds are
presented. The partial replacement of Gd by Tb atoms causes the decrease of the Curie temperature (TC) and
the increase of the residual resistivity. According to the Matthiessen rule the scattering mechanisms in (T) have
been analyzed. Moreover, the reduced form of the electrical resistivity Z(T T0) indicates a deviation from the
linearity for x > 0:2. This kind of behaviour can be attributed to density of d states near by the Fermi level (EF)
which are dominated by Ni 3d states. The valence band spectra as well as the core level lines have been analyzed as the in uence of Tb/Gd substitution on the electronic structure
Magneto-history effect in the Tb xGd 1-xNi 3 Compounds
The compounds TbxGd1xNi3 with a PuNi3-type structure have been obtained. The magnetic properties
have been investigated by using SQUID magnetometer (Quantum Design MPMS, temperature from 1.9 K to
300 K and magnetic eld up to 7 T). The partial replacement of Gd by Tb atoms is re ected in a decrease of the
ordering temperature from 115 K (x = 0:0) to 81 K (x = 1:0) as well as the increase of the saturation magnetic
moment MS from 6.93 B/f.u. (x = 0:0) to 7.14 B/f.u. (x = 1:0). A large di erence of M(T) curves has been
noticed between the so-called eld cooling zero eld cooling magnetization. The thermomagnetic curves are
sensitive to the applied magnetic eld and their origin can be understood as the domain-wall pinning e ect and
as the temperature dependence of coercivity
The Electronic and Magnetic Properties of YbxGd1-xNi5 Systems
The intermetallic compounds YbxGd1¡xNi5 crystallize in the hexagonal CaCu5-type structure. Based on
wide ranging SQUID-type magnetometer, it was shown that the saturation magnetization decreases with growing
concentration of ytterbium. The opposite tendency was observed for the Sommerfeld coefficient obtained in the
heat capacity measurements. These results are confirmed using ab initio band structure calculations
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