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Pb-free ferroelectric thin films are gaining attention due to their applicability in memory, sensor, actuator, and microelectromechanical system. In this work, Na$_{0.4}$K$_{0.1}$Bi$_{0.5}$TiO$_3$ (NKBT0.1) ferroelectric thin films were deposited on Pt(111)/Ti/SiO$_2$/Si substrates using the pulsed laser deposition technique at various substrate temperatures (600-750 $^\circ$C). The comprehensive structural, microstructural, and ferroelectric properties characterizations depicted that the grain size, dielectric constant, and remnant polarization increased with higher deposition temperatures. The influence of higher substrate temperatures on the control of (100)-preferential orientations was observed, indicating the importance of deposition conditions. Significantly, films deposited at 700 deg C exhibited reduced dielectric loss of 0.08 (at 1kHz), high dielectric constant of 673, and remnant polarization of 17 microC/cm2 at room temperature. At this deposition temperature, a maximum effective piezoelectric coefficient of 76 pm/V was availed. Based on the structural analysis, dielectric properties, and ferroelectric behavior, the optimal deposition temperature for the NKBT0.1 thin films was 700 $^\circ$C. This study contributes to the understanding of the influence of substrate temperature on the structural and ferroelectric properties of Pb-free NKBT0.1 thin films, providing insights for the development of high-performance ferroelectric devices., Comment: 16 pages, 4 figures

The coexistence of multiple structural phases and field induced short-range to long-range order transition in ferroelectric materials, leads to a strong electrocaloric effect (ECE) and electrical energy storage density (Wrec) in the vicinity of ferroelectric to non-ergodic phase transition in NKBT ceramic. Structural analysis using X-ray diffraction, Raman spectroscopy and TEM studies ascertained the coexistence of tetragonal (P4mm) and rhombohedral (R3c) phases. Dielectric study has revealed a critical slowing down of polar domain dynamics below a diffuse phase transition. Present investigation reports ECE in lead-free (Na0.8K0.2)0.5Bi0.5TiO3 (NKBT) ceramic by direct and indirect methods, which confirm the multifunctional nature of NKBT and its usefulness for applications in refrigeration and energy storage. A direct method of EC measurement in NKBT ceramic exhibits significant adiabatic temperature change ({\Delta}T) ~ 1.10 K and electrocaloric strength ({\xi}) ~ 0.55 Kmm/kV near the ferroelectric to non-ergodic phase transition at an external applied field of 20 kV/cm. A highest recoverable energy (Wrec) ~ 0.78 J/cm3 and electrical storage efficiency ({\eta}) ~ 86% are achieved at 423 K and an applied field of 20 kV/cm. This behavior is ascribed to the delicate balance between the field induced order-disordered transition and the thermal energy needed to disrupt field induced co-operative interaction., Comment: Need to modify

This study investigates the temperature-dependent quasi-static magnetoelectric (ME) response of electrically poled lead-free Na$_{0.4}$K$_{0.1}$Bi$_{0.5}$TiO$_3$-NiFe$_2$O$_4$ (NKBT-NFO) laminated composites. The aim is to understand the temperature stability of ME-based sensors and devices. The relaxor ferroelectric nature of NKBT is confirmed through impedance and polarization-electric (PE) hysteresis loop studies, with a depolarization temperature (Td) of approximately 110$^\circ$C. Heating causes a decrease and disappearance of planar electromechanical coupling, charge coefficient, and remnant polarization above Td. The temperature rise also leads to a reduction in magnetostriction and magnetostriction coefficient of NFO by approximately 33% and 25%, respectively, up to approximately 125$^\circ$C. At room temperature, the bilayer and trilayer configurations exhibit maximum ME responses of approximately 33 mV/cm.Oe and 80 mV/cm.Oe, respectively, under low magnetic field conditions (300-450 Oe). The ME response of NKBT/NFO is highly sensitive to temperature, decreasing with heating in accordance with the individual temperature-dependent properties of NKBT and NFO. This study demonstrates a temperature window for the effective utilization of NKBT-NFO-based laminated composite ME devices., Comment: 14 pages, 4 figures

Nanocrystalline CuO-CuFe2O4 composite thin films were developed from CuFeO2 ceramic target using a radio frequency sputtering method followed by a thermal oxidation process. This fabrication process helps to develop porous sensing layers which are highly desirable for solid state resistive gas sensors. Their sensing properties towards ethanol and hydrogen gas in dry air were examined at the operating temperatures ranging from 250 deg C to 500 deg C. The electrical transients during adsorption and desorption of the test gases were fitted with the Langmuir single site gas adsorption model. A composite thin film with a total thickness of 25 nm showed highest response (79%) towards hydrogen (500 ppm) at the operating temperature of 400 deg C. The shortest response time (tres) was found to be ~60 and ~90 seconds for hydrogen and ethanol respectively. The dependence of the response of the sensor on gas concentration (10-500 ppm) was also studied., Comment: 7 pages, 6 figures, This paper has been submitted in a reputed journal on Jan 06, 2018, This work has been submitted to the IEEE for possible publication

Lead based relaxor ferroelectric thin films have been of technological importance due to excellent properties for several commercial applications. However subtleness and high cost of fabrication have plagued of these materials. In this work a systematic study of PMN-PT thin films grown on LCMO buffered platinized glass substrates has been undertaken. The films were grown at room temperature using RF magnetron sputtering. Single phase PMN-PT films could be obtained by exsitu thermal annealing in air for 2h at temperatures 550 and 650 degree C. The films annealed at temperatures lower than 550 degree C and films without buffer layer showed presence of pyrochlore. Effect of annealing temperature on the microstructure, dielectric and ferroelectric properties of the PMN-PT films has been investigated. Scanning electron micrographs of single phase PMN-PT films show a bimodal grain size distribution for films annealed at 550 and 650 degree C. A high dielectric constant of 1300 and a remnant polarization (2Pr) of 17micro C/cm2 were observed for film annealed at 650 degree C.

By using the stripline Microwave Vector Network Analyzer Ferromagnetic Resonance and Pulsed Inductive Microwave Magnetometry spectroscopy techniques, we study a strong coupling regime of magnons to microwave photons in the planar geometry of a lithographically formed split-ring resonator (SRR) loaded by a single-crystal epitaxial yttrium-iron garnet (YIG) film. Strong anti-crossing of the photon modes of SRR and of the magnon modes of the YIG film is observed in the applied-magnetic-field resolved measurements. The coupling strength extracted from the experimental data reaches 9 percent at 3 GHz. Theoretically, we propose an equivalent circuit model of an SRR loaded by a magnetic film. This model follows from the results of our numerical simulations of the microwave field structure of the SRR and of the magnetization dynamics in the YIG film driven by the microwave currents in the SRR. The equivalent circuit model is in good agreement with the experiment. It provides a simple physical explanation of the process of mode anti-crossing. Our findings are important for future applications in microwave quantum photonic devices as well as in magnetically tunable metamaterials exploiting the strong coupling of magnons to microwave photons.

Copper ferrite thin films were rf sputtered at a power of 50W. The as deposited films were annealed in air at 800{\deg}C and slow cooled. The transmission electron microscope (TEM) studies were carried out on as deposited as well as on slow cooled film. Significantly larger defect concentration, including stacking faults, was observed in 50W as deposited films than the films deposited at a higher rf power of 200W. The film annealed at 800{\deg}C and then slow cooled showed an unusual grain growth upto 180nm for a film thickness of ~240nm. These grains showed Kikuchi pattern., Comment: 5 pages and 3 figures

Copper ferrite thin films were deposited on amorphous quartz substrates. The as deposited films were annealed in air and either quenched or slow cooled. Magnetization studies were carried out on the as deposited as well as annealed films using a SQUID magnetometer. The M-H curves were measured up to a field of 7T, at temperatures varying from 5K to 300K. The magnetization in the films did not saturate, even at the highest field. The expression, M(H)= Q(1- a/H^n) fitted the approach to saturation best with n=1/2, for all films and at all temperatures. The coefficient a was the highest for the as deposited film and was the smallest for the quenched film. In the case of as deposited film, the value of coefficient a increased with increasing temperature, while for the annealed films, the value of a showed a decrease as temperature increases., Comment: 5 pages, 3 figures

The copper ferrite thin films have been deposited by RF sputtering at a 50W rf power. The As-deposited films are annealed in air at $800^{\circ}$C and then slow cooled. The As-deposited (AD) as well as slow cooled (SC) films are studied using a SQUID Magnetometer. The M Vs H curves have been recorded at various temperatures between 5K to 300K. The coercivities obtained from the MH curves are then plotted against temperature (T). The magnetization in the films does not saturate, even at the highest field of 7T. The high field part of the M Vs H curves is fitted using the H1/2 term of Chikazumi expression M(H)= Q*(1- a /Hn), with n=1/2. The variation of coefficient 'a' of H1/2 term has been observed with temperature (T). An attempt has been made to correlate this with the coercivity (Hc) in the case of annealed films., Comment: 2 pages, 2 figures

The rf sputtered copper ferrite films contain nanocrystalline grains. In these films, the magnetization does not saturate even in high magnetic fields. This phenomenon of high field susceptibility is attributed to the defects and/or superparamagnetic grains in the films. A simple model is developed to describe the observed high field magnetization behavior of these films. The model is found to fit well to the high field part for all the studied films. An attempt is also made to explain the temperature variation of the ferrimagnetic contribution on the basis of reported exchange constants., Comment: 5 pages + 4 figures