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Dive into the research topics where K. R. S. Preethi Meher is active.

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Featured researches published by K. R. S. Preethi Meher.


Journal of Applied Physics | 2009

Colossal dielectric behavior of semiconducting Sr2TiMnO6 ceramics

K. R. S. Preethi Meher; K. B. R. Varma

Manganitelike double perovskite Sr2TiMnO6 (STMO) ceramics fabricated from the powders synthesized via the solid-state reaction route, exhibited dielectric constants as high as similar to 10(5) in the low frequency range (100 Hz-10 kHz) at room temperature. The Maxwell-Wagner type of relaxation mechanism was found to be more appropriate to rationalize such high dielectric constant values akin to that observed in materials such as KxTiyNi(1-x-y)O and CaCu3Ti4O12. The dielectric measurements carried out on the samples with different thicknesses and electrode materials reflected the influence of extrinsic effects. The impedance studies (100 Hz-10 MHz) in the 180-300 K temperature range revealed the presence of two dielectric relaxations corresponding to the grain boundary and the electrode. The dielectric response of the grain boundary was found to be weakly dependent on the dc bias field (up to 11 V/cm). However, owing to the electrode polarization, the applied ac/dc field had significant effect on the low frequency dielectric response. At low temperatures (100-180 K), the dc conductivity of STMO followed a variable range hopping behavior. Above 180 K, it followed the Arrhenius behavior because of the thermally activated conduction process. The bulk conductivity relaxation owing to the localized hopping of charge carriers obeyed the typical universal dielectric response.


Journal of Applied Physics | 2010

Structure, dielectric, and magnetic properties of Sr2TiMnO6 ceramics

K. R. S. Preethi Meher; M. Savinov; S. Kamba; V. Goian; K. B. R. Varma

Sr2TiMnO6, a double perovskite associated with high degree of B-site cation disorder was investigated in detail for its structural, magnetic, and dielectric properties. Though x-ray powder diffraction analysis confirms its cubic structure, first order Raman scattering and infrared reflectivity spectra indicate a breaking of the local cubic symmetry. The magnetization study reveals an anomaly at 14 K owing to a ferrimagnetic/canted antiferromagneticlike ordering arising from local Mn-O-Mn clusters. Saturated M-H hysteresis loops obtained at 5 K also reflect the weak ferromagnetic exchange interactions present in the system and an approximate estimation of Mn3+/Mn4+ was done using the magnetization data for the samples sintered at different temperatures. The conductivity and dielectric behavior of this system has been investigated in a broad temperature range of 10 to 300 K. Intrinsic permittivity was obtained only below 100 K whereas giant permittivity due to conductivity and Maxwell-Wagner polarization was observed at higher temperatures. X-ray photoemission studies further confirmed the presence of mixed oxidation states of Mn and the valence band spectra analysis was carried out in detail


Journal of Applied Physics | 2009

Bi4Ti3O12–5BiFeO3 Aurivillius intergrowth: Structural and ferroelectric properties

K. R. S. Preethi Meher; K. B. R. Varma

Aurivillus intergrowth Bi4Ti3O12-5BiFeO(3) was demonstrated to be ferroelectric that evoked the possibility of achieving high temperature magnetoelectric property in this family of compounds. X-ray diffraction studies confirmed its structure to be orthorhombic [Fmm2; a=5.5061(11) A degrees, b=5.4857(7) A degrees, c=65.742(12) A degrees]. However, transmission electron microscopy established the random incidence of intergrowth at nanoscale corresponding to n=6 and n=7 members of the Aurivillius family. Diffuse ferroelectric orthorhombic to paraelectric tetragonal phase transition around 857 K was confirmed by dielectric and high temperature x-ray diffraction studies. Polarization versus electric field hysteresis loops associated with 2P(r) of 5.2 mu C/cm(2) and coercive field of 42 kV/cm were obtained at 300 K.


Journal of Applied Physics | 2014

Closely related magnetic and dielectric transitions in the “114” magnetoelectric Zn-doped CaBaCo4O7

Md. Motin Seikh; V. Caignaert; E. Suard; K. R. S. Preethi Meher; A. Maignan; B. Raveau

We report on the impact of zinc doping upon the magneto-electric properties of CaBaCo4O7.We show that the presence of less than 1% Zn at the Co sites decreases TC from 64 K to 48 K and generates two magnetic transitions, concomitant with changes of slope of dielectric permittivity, at 54 K and 77 K, respectively. Powder neutron diffraction and magnetic data show the existence of an incommensurate magnetic phase and a spin-flop transition in this temperature range. The crossover of the magnetodielectric effect of this oxide, from positive below 50 K to negative above this temperature emphasizes the primordial role of the incommensurate magnetic phase in the evolution of these properties.


Integrated Ferroelectrics | 2010

Dielectric and Impedance Studies on 0.5Li(2)O-0.5K(2)O-2B(2)O(3) Glasses

Gadige Paramesh; K. R. S. Preethi Meher; M. Niyaz Ahmed; K. B. R. Varma

Transparent glasses in the system 0.5Li2O-0.5K2O-2B2O3 (LKBO) were fabricated via the conventional melt quenching technique. Amorphous and glassy nature of the samples was confirmed by X-ray diffraction and differential scanning calorimetry (DSC) respectively. Complex dielectric and impedance studies were conducted on the samples at different temperatures in the100 Hz-10 MHz frequency range. ac conductivity was calculated from the dielectric data and the conductivity relaxation was found to obey the Jonschers law. The Nyquists plots (Z ″(ω) vs. Z′(ω)) showed single suppressed semicircles at all the temperatures under study indicating the non ideal Debye type relaxation process to be active. Activation energies for conduction and relaxation process were calculated using the Arrhenius relation. The UV-visible optical transmission spectra was shown a wide transmission window and calculated optical band gap was found to be 5.67 eV.


International Journal of Materials Research | 2013

Structural and relaxor characteristics of Ca0.18Sr0.226Ba0.594Nb2O6

K. R. S. Preethi Meher; Rahul Vaish; Jungang Hou; Dalibor Krsmanovic; Rajeev Kumar; K. B. R. Varma

Abstract Polycrystalline Ca0.18Sr0.226Ba0.594Nb2O6 (CSBN18) was synthesized via the solid-state reaction route. X-ray structural studies confirmed it belonged to the tetragonal tungsten bronze family. Rietveld refinement of the X-ray data has been carried out for CSBN18 where the atomic positions and site occupancy factors for A-sites have been determined. The dielectric properties of CSBN18 ceramic were studied as a function of temperature in the 100 Hz–1 MHz frequency range. The dielectric relaxation followed the Vogel–Fulcher relation wherein Ea = 37.4 meV; Tf = 131.5 °C and ω0 = 4.31 × 109 rad s−1. A high pyroelectric coefficient of ∼ 250 μC m−2.K was obtained around the transition temperature (∼150 °C). This is significantly higher than that reported for polycrystalline SrxBa1-xNb2O6 (SBN). However, the piezoelectric coefficient (d33) of the title composition was as low as 6 pC N−1.


SOLID STATE PHYSICS: Proceedings of the 56th DAE Solid State Physics Symposium 2011 | 2012

High temperature phase transition studies and dielectric properties of Sr2SbMnO6

K. R. S. Preethi Meher; Pierre-Eymeric Janolin; Nicolas Guiblin; Gadige Paramesh; K. B. R. Varma

Sr2SbMnO6 (SSMO) ceramics were, fabricated using the nanocrystalline powders obtained via molten salt synthesis (MSS) method. High temperature X-ray diffraction studies confirmed the structural phase transition (room temperature tetragonal (I4/mcm) to the cubic phase (Pm-3m)) temperature to be around 736K. The discontinuity in the phase transition indicated its first order nature reflecting the presence of ferroelectric-like distortions in SSMO prepared from MSS which seemed to be unique as it was not observed so far in the case of SSMO prepared using solid-state reaction method. The dielectric behavior of SSMO was studied in the 300-950 K temperature range at high frequencies (MHz range) in order to suppress the of space charge and related effects that dominate at such higher temperatures and mask the real phase transition.


Journal of Solid State Chemistry | 2012

Synthesis dependent characteristics of Sr{sub 1-x}Mn{sub x}TiO{sub 3} (x=0.03, 0.05, 0.07 and 0.09)

K. R. S. Preethi Meher; Christine Bogicevic; Pierre-Eymeric Janolin

Sr1-xMnxTiO3 (where x=0.03, 0.05, 0.07 and 0.09) was synthesized via different routes that include solid-state, oxalate precipitation and freeze drying. In oxalate precipitation technique, compositions corresponding to 3 and 5 mol% doping of Mn were monophasic whereas the higher compositions revealed the presence of the secondary phases such as MnO, Mn3O4 etc., as confirmed by high resolution X-ray diffraction (XRD) studies. The decomposition behavior of the precursors prepared using oxalate precipitation method corresponding to the above mentioned compositions was studied. Nanopowders of compositions pertaining to 5 to 9 mol% of Mn doping were obtained using freeze-drying technique. The average crystallite size of these nanopowders was found to be in the 35 to 65 nm range. The microstructural studies carried out on the sintered ceramics, fabricated using powders synthesized by different routes established the fine grained nature ( < 1 mu m) of the one obtained by freeze drying method. Raman scattering studies were carried out in order to complement the observations made from XRD regarding the phase purity. The dielectric properties of the ceramics obtained by different synthesis routes were studied in the 80-300 K temperature range at 100 kHz and the effect of grain size has been discussed


Materials Research Bulletin | 2016

Origin of giant dielectric constant and conductivity behavior in Zn1-xMgxO (0 <= x <= 0.1) ceramics

C. Justin Raj; Gadige Paramesh; B. Shri Prakash; K. R. S. Preethi Meher; K. B. R. Varma


Journal of Solid State Chemistry | 2012

Synthesis dependent characteristics of Sr1−xMnxTiO3 (x=0.03, 0.05, 0.07 and 0.09)

K. R. S. Preethi Meher; Christine Bogicevic; Pierre-Eymeric Janolin; K. B. R. Varma

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K. B. R. Varma

Indian Institute of Science

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Gadige Paramesh

Indian Institute of Science

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A. Maignan

Centre national de la recherche scientifique

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Antara Baral

Indian Institute of Science

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B. Shri Prakash

Council of Scientific and Industrial Research

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M. Niyaz Ahmed

Indian Institute of Science

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M. Savinov

Indian Institute of Science

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