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Optical echo-spectroscopy of highly doped Tm:YAG in the absence of an applied magnetic field and parameters describing the energy and phase relaxation
Tuning of physical properties of Fe7 (PO4 )6 by sodium intercalation magnetically ordered state through succession of phase transitions at TN1 = 45.5 K and TN2 = 16 K marked
Dynamics of plastic and liquid cyclohexane in bulk and in porous glasses studied by NMR methods of 4 nm, all applied methods corroborate DSC results of the virtual absence of a phase transition
Dynamics of plastic and liquid cyclohexane in bulk and in porous glasses studied by NMR methods of 4 nm, all applied methods corroborate DSC results of the virtual absence of a phase transition
ESR study in lightly doped La1-xSrxMnO3 ≤0.2). The temperature dependence of the ESR linewidth marks all significant transitions between both
Peculiarities of the dielectric properties of ternary 0.5(Y0.1Zr0.9O2) - 0.5(0.6SrTiO3 - 0.4BiScO3) ceramic system techniques. By XRD analysis, a coexistence of tetragonal P42/nmc phase related to the Y0.1Zr0.9O2 subsystem
The delay time of phase transition to the polar phase in relaxor ferroelectrics of the phase transition from the glasslike state to the field-induced ferroelectric state was determined from
Relaxor properties of ceramic solid solutions in SrTi0₃-BiSc0₃ system= Релаксорные свойства керамических твердых растворов системы SrTiO₃-BiScO₃ are specific for ferroelectrics with diffuse phase transition
Pressure-induced ferroelastic phase transition in LuLiF4 compound) has been found at 10.5 GPa. It has been determined that this is the second-order phase transition.
Phase transitions in the BIMEVOX solid solutions with Me = Ga, Zr order phase transitions at ∼ 308°C (BIGAVOX) and ∼ 270°C (BIZRVOX) have been revealed for solid
Страница 10 из 2548
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