Abstract:We report on the discovery of Griffiths-like phase in several compounds of the R 5 ͑Si x Ge 1−x ͒ 4 ͑R = Gd, Tb, Dy, and Ho͒ system, through the existence of an anomalous behavior on the reciprocal magnetic susceptibility ͑ −1 ͒. We found that this anomaly is restricted to the samples which present the Gd 5 Si 2 Ge 2 -type ͑monoclinic͒ or the Sm 5 Ge 4 -type ͕orthorhombic-II ͓O͑II͔͖͒ structural phases at room temperature. This peculiar effect originates from local disorder within the crystallographic structure… Show more
“…Note that these abnormal reciprocal susceptibility features have also been observed in other compounds that present strong interplay between the lattice and spin degrees of freedom (R 5 [Si,Ge] 4 and La[Sr,Ca]MO); 19,[31][32][33] thus, a similar analysis may explain these observations.…”
The cubic spinel CdCr2S4 gained recently a vivid interest, given the relevance of relaxor-like dielectric behavior in its paramagnetic phase. By a singular combination of local probe techniques namely Pair Distribution Function and Perturbed Angular Correlation we firmly establish that the Cr ion plays the central key role on this exotic phenomenon, namely through a dynamic off-centering displacement of its coordination sphere. We further show that this off centering of the magnetic Cr-ion gives rise to a peculiar entanglement between the polar and magnetic degrees of freedom, stabilizing, in the paramagnetic phase, short range magnetic clusters, clearly seen in ultra-low field susceptibility measurements. Moreover, the Landau theory is here used to demonstrate that a linear coupling between the magnetic and polar order parameters is sufficient to justify the appearance of magnetic cluster in paramagnetic phase of this compound. These results open insights on the hotly debated magnetic and polar interaction, setting a step forward in the reinterpretation of the coupling of different physical degrees of freedom.
“…Note that these abnormal reciprocal susceptibility features have also been observed in other compounds that present strong interplay between the lattice and spin degrees of freedom (R 5 [Si,Ge] 4 and La[Sr,Ca]MO); 19,[31][32][33] thus, a similar analysis may explain these observations.…”
The cubic spinel CdCr2S4 gained recently a vivid interest, given the relevance of relaxor-like dielectric behavior in its paramagnetic phase. By a singular combination of local probe techniques namely Pair Distribution Function and Perturbed Angular Correlation we firmly establish that the Cr ion plays the central key role on this exotic phenomenon, namely through a dynamic off-centering displacement of its coordination sphere. We further show that this off centering of the magnetic Cr-ion gives rise to a peculiar entanglement between the polar and magnetic degrees of freedom, stabilizing, in the paramagnetic phase, short range magnetic clusters, clearly seen in ultra-low field susceptibility measurements. Moreover, the Landau theory is here used to demonstrate that a linear coupling between the magnetic and polar order parameters is sufficient to justify the appearance of magnetic cluster in paramagnetic phase of this compound. These results open insights on the hotly debated magnetic and polar interaction, setting a step forward in the reinterpretation of the coupling of different physical degrees of freedom.
“…Such phenomenon was firstly reported in the Tb 5 Si 2 Ge 2 compound, when it was associated with the experimentally observed deviation from the expected linearity (from Curie-Weiss law) of the 1 (T) curve in the paramagnetic region, T > T C [33]. Later, different works, reported by Ouyang, Tian, Pereira and co-workers identified the Griffiths-like phase in other compounds of the R 5 T 4 family [23,[48][49][50]. All these compounds presented anomalies featuring their reciprocal susceptibility curve: a "stair-like" behavior occurring in an intermediate temperature region, T C < T < T G .…”
Section: Is the Griffiths-like Phase A Requisite For A Giant Magnetocmentioning
confidence: 73%
“…In the past few years several R 5 T 4 compounds (R = rare earth: Gd, Tb, Dy, and Ho; T = group 14 elements) have shown a Griffiths-like behavior [33,[48][49][50]. Such phenomenon was firstly reported in the Tb 5 Si 2 Ge 2 compound, when it was associated with the experimentally observed deviation from the expected linearity (from Curie-Weiss law) of the 1 (T) curve in the paramagnetic region, T > T C [33].…”
Section: Is the Griffiths-like Phase A Requisite For A Giant Magnetocmentioning
confidence: 99%
“…All these compounds presented anomalies featuring their reciprocal susceptibility curve: a "stair-like" behavior occurring in an intermediate temperature region, T C < T < T G . Later on, our group has completed the phase diagrams of the R 5 (Si x Ge 1-x ) (R = Gd, Tb, Dy and Ho) compounds with their corresponding Griffiths-like phase [50]. It was observed that despite the different main temperatures along their composition for each R compound (T G , T C and T N ), the phase diagrams were very similar in shape and two main conclusions could immediately be drawn: (1) the Griffiths singularity behavior appears only in the M and O(II) phases for compositions below a characteristic Si concentration that was defined as x p and (2) the O(II) structure is stabilized when the ratio…”
Section: Is the Griffiths-like Phase A Requisite For A Giant Magnetocmentioning
Magnetic materials with strong spin-lattice coupling are a powerful set of candidates for multifunctional applications because of their multiferroic, magnetocaloric (MCE), magnetostrictive and magnetoresistive effects. In these materials there is a strong competition between two states (where a state comprises an atomic and an associated magnetic structure) that leads to the occurrence of phase transitions under subtle variations of external parameters, such as temperature, magnetic field and hydrostatic pressure. In this review a general method combining detailed magnetic measurements/analysis and first
OPEN ACCESSEntropy 2014, 16 3814 principles calculations with the purpose of estimating the phase transition temperature is presented with the help of two examples (Gd 5 Si 2 Ge 2 and Tb 5 Si 2 Ge 2 ). It is demonstrated that such method is an important tool for a deeper understanding of the (de)coupled nature of each phase transition in the materials belonging to the R 5 (Si,Ge) 4 family and most possibly can be applied to other systems. The exotic Griffiths-like phase in the framework of the R 5 (Si x Ge 1-x ) 4 compounds is reviewed and its generalization as a requisite for strong phase competitions systems that present large magneto-responsive properties is proposed.
In the present work, spontaneous magnetization is observed in the inverse magnetic susceptibility of La 0.7 Ca 0.3 MnO 3 and La 0.7 Ba 0.3 MnO 3 compounds above T C up to a temperature T * . From information gathered from neutron diffraction, dilatometry, and high-field magnetization data, we suggest that T * is related to the transition temperature of the low-temperature (high magnetic field) magnetic phase. In the temperature region between T * and T C , the application of a magnetic field drives the system from the high-temperature to low-temperature magnetic phases, the latter possessing a higher magnetization.
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