n/a

MFe2O4 (M = Mn2+, Ni2+, Co2+ and Cu2+) ferrite powders were prepared by flash auto-combustion reaction. The structural identification of the samples was carried out using X-ray diffraction (XRD), transmission electron microscope (TEM), selected area electron diffraction (SAED) and IR spectra. The study established the formation of sub-nanosized particles especially for MFe2O4 (M = Ni, Co and Cu) ferrites. MFe2O4/PEG (polyethylene glycol) composites were prepared by cold uniaxial pressing. The magnetic properties were studied by carrying out the hysteresis of MFe2O4 and PEG/MFe2O4 composite at room temperature. The data showed that MnFe2O4 has the highest saturation magnetization while CoFe2O4 has the largest coercive field due to the high anisotropy of Co2+ ions. The ac electrical conductivity as well as the dielectric constant ε′ and loss tangent tan δ were measured at different frequencies at room temperature. The highest conductivity is achieved for PEG/Ni Fe2O4 and the lowest value of tan δ is obtained for PEG/MnFe2O4 amongst all PEG/MFe2O4 nanocomposites. © 2010 Elsevier B.V. All rights reserved.

MFe2O4 (M = Mn2+, Ni2+, Co2+ and Cu2+) ferrite powders were prepared by flash auto-combustion reaction. The structural identification of the samples was carried out using X-ray diffraction (XRD), transmission electron microscope (TEM), selected area electron diffraction (SAED) and IR spectra. The study established the formation of sub-nanosized particles especially for MFe2O4 (M = Ni, Co and Cu) ferrites. MFe2O4/PEG (polyethylene glycol) composites were prepared by cold uniaxial pressing. The magnetic properties were studied by carrying out the hysteresis of MFe2O4 and PEG/MFe2O4 composite at room temperature. The data showed that MnFe2O4 has the highest saturation magnetization while CoFe2O4 has the largest coercive field due to the high anisotropy of Co2+ ions. The ac electrical conductivity as well as the dielectric constant ε′ and loss tangent tan δ were measured at different frequencies at room temperature. The highest conductivity is achieved for PEG/Ni Fe2O4 and the lowest value of tan δ is obtained for PEG/MnFe2O4 amongst all PEG/MFe2O4 nanocomposites. © 2010 Elsevier B.V. All rights reserved.

MFe2O4 (M = Mn2+, Ni2+, Co2+ and Cu2+) ferrite powders were prepared by flash auto-combustion reaction. The structural identification of the samples was carried out using X-ray diffraction (XRD), transmission electron microscope (TEM), selected area electron diffraction (SAED) and IR spectra. The study established the formation of sub-nanosized particles especially for MFe2O4 (M = Ni, Co and Cu) ferrites. MFe2O4/PEG (polyethylene glycol) composites were prepared by cold uniaxial pressing. The magnetic properties were studied by carrying out the hysteresis of MFe2O4 and PEG/MFe2O4 composite at room temperature. The data showed that MnFe2O4 has the highest saturation magnetization while CoFe2O4 has the largest coercive field due to the high anisotropy of Co2+ ions. The ac electrical conductivity as well as the dielectric constant ε′ and loss tangent tan δ were measured at different frequencies at room temperature. The highest conductivity is achieved for PEG/Ni Fe2O4 and the lowest value of tan δ is obtained for PEG/MnFe2O4 amongst all PEG/MFe2O4 nanocomposites. © 2010 Elsevier B.V. All rights reserved.

\{MFe2O4\} (M = Mn2+, Ni2+, Co2+ and Cu2+) ferrite powders were prepared by flash auto-combustion reaction. The structural identification of the samples was carried out using X-ray diffraction (XRD), transmission electron microscope (TEM), selected area electron diffraction (SAED) and İR\} spectra. The study established the formation of sub-nanosized particles especially for \{MFe2O4\} (M = Ni, Co and Cu) ferrites. MFe2O4/PEG (polyethylene glycol) composites were prepared by cold uniaxial pressing. The magnetic properties were studied by carrying out the hysteresis of \{MFe2O4\} and PEG/MFe2O4 composite at room temperature. The data showed that MnFe2O4 has the highest saturation magnetization while CoFe2O4 has the largest coercive field due to the high anisotropy of Co2+ ions. The ac electrical conductivity as well as the dielectric constant ɛ′ and loss tangent tan δ were measured at different frequencies at room temperature. The highest conductivity is achieved for PEG/Ni Fe2O4 and the lowest value of tan δ is obtained for PEG/MnFe2O4 amongst all PEG/MFe2O4 nanocomposites.

The structure of some even-even superheavy nuclei with the proton number Z = 98-120 is studied using a semi-microscopic but not self-consistent model. The macroscopic energy part is obtained from the Skyrme nucleon-nucleon interaction in the semi-classical extended Thomas-Fermi approach. A simple but accurate method is derived for calculating the direct part of the Coulomb energy. The microscopic shell plus pairing energy corrections are calculated from the traditional Strutinsky method. Within this semi-microscopic approach, the total energy curves with the quadrupole deformation of the studied superheavy nuclei were calculated. The same approach features the well known 208Pb or 238U nuclei. For each nucleus the model predictions for the binding energy, the deformation parameters, the half-density radii and comparison with other theoretical models are made. The calculated binding energies are in good agreement with the available experimental data. © 2010 Pleiades Publishing, Ltd.

The structure of some even-even superheavy nuclei with the proton number Z = 98-120 is studied using a semi-microscopic but not self-consistent model. The macroscopic energy part is obtained from the Skyrme nucleon-nucleon interaction in the semi-classical extended Thomas-Fermi approach. A simple but accurate method is derived for calculating the direct part of the Coulomb energy. The microscopic shell plus pairing energy corrections are calculated from the traditional Strutinsky method. Within this semi-microscopic approach, the total energy curves with the quadrupole deformation of the studied superheavy nuclei were calculated. The same approach features the well known 208Pb or 238U nuclei. For each nucleus the model predictions for the binding energy, the deformation parameters, the half-density radii and comparison with other theoretical models are made. The calculated binding energies are in good agreement with the available experimental data. © 2010 Pleiades Publishing, Ltd.