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Título

Electrocaloric effect near room temperature in lead-free Aurivillius phase Sr2Bi4Ti5O18 upon La and Nb codoping [Dataset]

AutorLafuerza, Sara CSIC ORCID ; Gracia, David CSIC ORCID; Blasco, Javier CSIC ORCID; Evangelisti, Marco CSIC ORCID
Palabras claveElectrocaloric effect
Direct and indirect electrocaloric measurements
Aurivillius phase
Lead-free ferroelectrics
Fecha de publicación10-oct-2023
EditorDIGITAL.CSIC
CitaciónLafuerza, Sara; Gracia, David; Blasco, Javier; Evangelisti, Marco; 2023; Electrocaloric effect near room temperature in lead-free Aurivillius phase Sr2Bi4Ti5O18 upon La and Nb codoping [Dataset]; DIGITAL.CSIC; https://doi.org/10.20350/digitalCSIC/15626
ResumenLa and Nb codoping of the five-layer Aurivillius phase Sr2Bi4Ti5O18 induces compositional disorder and diffuse relaxor transitions at much lower temperatures than the undoped ferroelectric compound (560 K), while preserving the orthorhombic structure. For moderate La and Nb concentrations, the ferroelectric properties are enhanced in the vicinity of room temperature, and so is their electrocaloric effect measured directly with a homemade quasi-adiabatic calorimeter. The adiabatic temperature change reaches, e.g., ΔT ⁓ 0.3 K at 355 K with a temperature span ⁓ 15 K, under ΔE = 37 kV/cm. The large field dispersion of the effect is ascribed to field-induced transitions from short-range-ordered relaxor to long-range-ordered ferroelectric states. Indirect estimations of the electrocaloric effect from electric polarization data are not able to quantitatively predict the direct results and emphasize the need of applying direct measurement methods, especially for relaxor ferroelectrics.
Descripción[Description of methods used for collection/generation of data] Crystal structures were characterized by powder X-ray diffraction (XRD) at room temperature in a Rigaku D-Max system using Cu Kα1,2 wavelengths. Rietveld analysis of the X-ray patterns was performed using the Fullprof package program. Electrical and electrocaloric properties measurements were conducted on sintered disc-shaped samples, with typical dimensions of 8 mm diameter and thickness between 0.5 and 1 mm. Electrodes were made with silver paste in sandwich geometry. The dielectric constant was derived from measurements with an impedance analyzer (Wayne Kerr Electronics 6500B), applying sinusoidal excitations of 1 V amplitude at several frequencies between 100 Hz and 4 MHz. The polarization versus electric field P(E) curves were recorded using a commercial polarization analyzer (aixACCT Easy Check 300) jointly with a high voltage amplifier (Trek 610E), applying sinusoidal excitations with typical frequency of 10 Hz and E field amplitudes up to 70 kV/cm. Direct measurements of the electrocaloric effect (ECE) were performed using a dedicated in-house-developed quasi-adiabatic calorimeter. The adiabatic temperature change was measured as a function of temperature every 1 K and at different applied E field variations. Samples were measured in the “contactless” mode to minimize heat losses, held only by the high voltage coaxial cable and K-type thermocouple for the direct measurement of the temperature variation. Voltages up to either 2 kV or 5 kV were applied using two different homemade high-voltage converters. Heat capacity measurements were also performed, using a commercial adiabatic calorimeter (from Termis Ltd.).
[Methods for processing the data] For the indirect estimation of the electrocaloric effect, well-known thermodynamic formulations based on Maxwell relations have been applied to the polarization data recorded at several temperatures, to derive entropy variations as a function of temperature.
URIhttp://hdl.handle.net/10261/336892
DOIhttps://doi.org/10.20350/digitalCSIC/15626
ReferenciasGracia, David; Lafuerza, Sara; Blasco, Javier; Evangelisti, Marco; 2023; The electrocaloric effect of lead-free Ba1−yCayTi1−xHfxO3 from direct and indirect measurements [Preprint]; arXiv; https://doi.org/10.48550/arXiv.2308.11341
Gracia, David; Lafuerza, Sara; Blasco, Javier; Evangelisti, Marco; 2024; The electrocaloric effect of lead-free Ba1−yCayTi1−xHfxO3 from direct and indirect measurements; Elsevier; https://doi.org/10.1016/j.jallcom.2024.173923
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