On-Chip Planar Metasurfaces for Magnetic Sensors with Greatly Enhanced Sensitivity

Aleix Barrera, Emile Fourneau, Natanael Bort-Soldevila, Jaume Cunill-Subiranas, Nuria Del-Valle, Nicolas Lejeune, Michal Staňo, Alevtina Smekhova, Narcis Mestres, Lluis Balcells, Carles Navau, Vojtěch Uhlíř, Simon J. Bending, Sergio Valencia, Alejandro V. Silhanek, Anna Palau

ACS Nano 2025, 19, 10, 10461–10475
DOI: 10.1021/acsnano.5c00422

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High Pressure Oxygenation of EuBCO and GdBCO Coated Conductors

Tetiana Prikhna, Aiswarya Kethamkuzhi, Roxana Vlad, Myroslav Karpets, Robert Kluge, Semyon Ponomaryov, Viktor Moshchil, Xavier Obradors, Bernd Büchner, Joffre Gutierrez, Sabine Wurmehl & Teresa Puig

IEEE Transactions on Applied Superconductivity, vol. 35, no. 5, pp. 1-5, Aug. 2025, Art no. 6601505

DOI: 10.1109/TASC.2024.3511544

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Tuning the superconducting performance of YBa2Cu3O7-δ films through field-induced oxygen doping

Jordi Alcalà, Alejandro Fernández-Rodríguez, Thomas Günkel, Aleix Barrera, Mariona Cabero, Jaume Gazquez, Lluis Balcells, Narcís Mestres & Anna Palau

Scientific Reports volume 14, Article number: 1939 (2024)

DOI: 10.1038/s41598-024-52051-1

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Band Gap Tuning of Solution-Processed Ferroelectric Perovskite BiFe1–xCoxO3 Thin Films

Pamela MachadoMateusz ScigajJaume GazquezEstel RuedaAntonio Sánchez-DíazIgnasi FinaMartí Gibert-RocaTeresa PuigXavier ObradorsMariano Campoy-Quiles, and Mariona Coll*Chem. Mater.201931 (3), pp 947–954  DOI: 10.1021/acs.chemmater.8b04380

Ferroelectric perovskite oxides are emerging as a promising photoactive layer for photovoltaic applications because of their very high stability and their alternative ferroelectricity-related mechanism for solar energy conversion that could lead to extraordinarily high efficiencies. One of the biggest challenges so far is to reduce their band gap toward the visible region while simultaneously retaining ferroelectricity. To address these two issues, herein an elemental composition engineering of BiFeO3 is performed by substituting Fe by Co cations, as a means to tune the characteristics of the transition metal–oxygen bond. We demonstrate by solution processing the formation of epitaxial, pure phase, and stable BiFe1–xCoxO3 thin films for x ≤ 0.3 and film thickness up to 100 nm. Importantly, the band gap can be tuned from 2.7 to 2.3 eV upon cobalt substitution while simultaneously enhancing ferroelectricity. As a proof of concept, nonoptimized vertical devices have been fabricated and, reassuringly, the electrical photoresponse in the visible region of the Co-substituted phase is improved with respect to the unsubstituted oxide.

Direct and Converse Piezoelectric Responses at the Nanoscale from Epitaxial BiFeO3 Thin Films Grown by Polymer Assisted Deposition

DOI:10.1039/C8NR05737K

We use an original water-based chemical method, to grow pure epitaxial BiFeO3 (BFO) ultra-thin films with excellent piezoelectric properties. Particularly, we show that this novel chemical route produces a higher natural ferroelectric domain size distribution and coercive field compared to similar BFO films grown by physical methods. Moreover, we measured the d33 piezoelectric coefficient of 60 nm thick BFO films with a direct approach, using Direct Piezoelectric Force Microscopy (DPFM). As a result, first piezo-generated charge maps of a very thin BFO layer were obtained applying this novel technology. We also performed a comparative study of the d33 coefficients between standard PFM analysis and the DPFM microscopy showing similar values i.e. 17 pm/V and 22 pC/N respectively. Finally, we proved that the directionality of the piezoelectric effect in BFO ferroelectric thin films is preserved at low thickness dimensions demonstrating the potential of chemical processes for the development of low cost functional ferroelectric and piezoelectric devices.

Defect landscape and electrical properties in solution-derived LaNiO3 and NdNiO3 epitaxial thin films

B. Mundet, J. Jareño, J. Gazquez, M. Varela, X. Obradors, and T. Puig. Phys. Rev. Materials 2, 063607 

DOI:https://doi.org/10.1103/PhysRevMaterials.2.063607

In this work we evaluate the defects and the associated distortions present in tensile and compressive-strained chemical solution deposition–derived NdNiO3 (NNO) and LaNiO3 (LNO) thin films by means of aberration corrected scanning transmission electron microscopy. We elucidate a fundamental link between strain and the most common defect observed in nickelate films, the Ruddlesden-Popper fault (RPF), which will ultimately impinge on the electrical properties of the films. Overall, the concentration of RPF defects increases with the lattice mismatch. More specifically, LNO films are always metallic, although transitioning from compressive to tensile strain results in the appearance of RPFs and an increase of the resistivity. On the other hand, NNO films always behave as insulators under tensile strain, whereas under compressive strain the increase of the thickness makes the onset of the metal-to-insulator transition shift to higher temperatures.

Piezo-generated charge mapping revealed through direct piezoelectric force microscopy

Piezo-generated charge mapping revealed through direct piezoelectric force microscopy

A. GomezM. GichA. Carretero-GenevrierT. Puig & X. Obradors Nature Communications 8, Article number: 1113 (2017) doi:10.1038/s41467-017-01361-2 

While piezoelectric and ferroelectric materials play a key role in many everyday applications, there are still a number of open questions related to their physics. To enhance our understanding of piezoelectrics and ferroelectrics, nanoscale characterization is essential. Here, we develop an atomic force microscopy based mode that obtains a direct quantitative analysis of the piezoelectric coefficient d33. We report nanoscale images of piezogenerated charge in a thick single crystal of periodically poled lithium niobate (PPLN), a bismuth ferrite (BiFO3) thin film, and lead zirconate titanate (PZT) by applying a force and recording the current produced by these materials. The quantification of d33coefficients for PPLN (14 ± 3 pC per N) and BFO (43 ± 6 pC per N) is in agreement with the values reported in the literature. Even stronger evidence of the reliability of the method is provided by an equally accurate measurement of the significantly larger d33 of PZT.

Institut de Ciència de Materials de Barcelona ICMAB CSIC

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