Cooling magnetic field dependence of magnetic phase transition has been observed in Y0.9Pr0.1CrO3. GzFx order (spin structure of PrCrO3) is dominant after zero field cooling (ZFC), whereas G(x)F(z) order (spin structure of YCrO3) is dominant after cooling under a field higher than 100 Oe. Positive/negative exchange bias-like effect, with large vertical shift and small horizontal shift, has been observed after FC/ZFC process. The vertical shift can be attributed to the frozen ordered Pr3+ and Cr3+ spins in magnetic domains, because of the strong coupling between Pr3+ and Cr3+ sublattices; while the horizontal shift is a result of the pinning of spins at the interfaces. The frozen structure is generated by the field used for the measurement o...
The exchange-bias (EB) effect with sign reversalwas found in LuFe0.5Cr0.5O3 ferrite-chromite, which ...
In this work, we have carried out a detailed study of the magnetic and structural properties of YFe1...
The first-order character of the transition from the low-to-intermediate spin state in the system (P...
In this paper, we demonstrate an interesting feature in YbCrO<sub>3</sub> (YCO) nanocrystals, in whi...
Using magnetic domain observations, we investigated the reversal process of the perpendicular exchan...
Exchange bias (EB) effects in YFe0.5Cr0.5O3, which exhibits magnetization reversal, were systemicall...
In exchange-biased systems, antiferromagnetic Cr2O3 has drawn intensive attention because of its hig...
CrCl3 has been known for a long time to be a quasi 2D ferromagnet FM with a specific heat peak at ...
The temperature and cooling-eld dependences of an exchange bias eld in a 4-nm Fe/16.2-nm Cr(100) bil...
We report on exchange bias effects in 10 nm particles of Pr0.5Ca0.5MnO3 which appear as a result of ...
Moderate dc magnetic fields of less than 1 T allow tuning the exchange bias in an epitaxially grown ...
CrCl3 has been known for a long time to be a quasi-2D ferromagnet (FM) with a specific-heat peak at ...
We report field-induced switchable polarization (P similar to 0.2-0.8 mu C/cm(2)) below the Neel tem...
RFe1−xCrxO3 with R = Y and Lu, comparing the numerical simulations with experiments and mean field...
The family of hole-doped Pr-based perovskite cobaltites, Pr0.5Ca0.5CoO3 and (Pr1−yREy)0.3Ca0.7CoO3 (...
The exchange-bias (EB) effect with sign reversalwas found in LuFe0.5Cr0.5O3 ferrite-chromite, which ...
In this work, we have carried out a detailed study of the magnetic and structural properties of YFe1...
The first-order character of the transition from the low-to-intermediate spin state in the system (P...
In this paper, we demonstrate an interesting feature in YbCrO<sub>3</sub> (YCO) nanocrystals, in whi...
Using magnetic domain observations, we investigated the reversal process of the perpendicular exchan...
Exchange bias (EB) effects in YFe0.5Cr0.5O3, which exhibits magnetization reversal, were systemicall...
In exchange-biased systems, antiferromagnetic Cr2O3 has drawn intensive attention because of its hig...
CrCl3 has been known for a long time to be a quasi 2D ferromagnet FM with a specific heat peak at ...
The temperature and cooling-eld dependences of an exchange bias eld in a 4-nm Fe/16.2-nm Cr(100) bil...
We report on exchange bias effects in 10 nm particles of Pr0.5Ca0.5MnO3 which appear as a result of ...
Moderate dc magnetic fields of less than 1 T allow tuning the exchange bias in an epitaxially grown ...
CrCl3 has been known for a long time to be a quasi-2D ferromagnet (FM) with a specific-heat peak at ...
We report field-induced switchable polarization (P similar to 0.2-0.8 mu C/cm(2)) below the Neel tem...
RFe1−xCrxO3 with R = Y and Lu, comparing the numerical simulations with experiments and mean field...
The family of hole-doped Pr-based perovskite cobaltites, Pr0.5Ca0.5CoO3 and (Pr1−yREy)0.3Ca0.7CoO3 (...
The exchange-bias (EB) effect with sign reversalwas found in LuFe0.5Cr0.5O3 ferrite-chromite, which ...
In this work, we have carried out a detailed study of the magnetic and structural properties of YFe1...
The first-order character of the transition from the low-to-intermediate spin state in the system (P...