Olga Caballero-Calero

Dr. Olga Caballero-Calero

IMN-Instituto de Micro y Nanotecnología (CNM-CSIC), Madrid, Spain

Research Focus & Metrics

Academic Career Length

24Years (2003-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 August 2013 in Renewable and Sustainable Energy Reviews
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Journal Article
Closed access
MMMarisol Martin-Gonzalez
Marisol Martin-Gonzalez
OCOlga Caballero-Calero
Olga Caballero-Calero
PDP. Díaz-Chao
P. Díaz-Chao

7 January 2021 in Nanoscale
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Journal Article
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ARAlejandra Ruiz-Clavijo
Alejandra Ruiz-Clavijo
OCOlga Caballero-Calero
Olga Caballero-Calero
MMMarisol Martin-Gonzalez
Marisol Martin-Gonzalez
Anodic porous alumina, –AAO– (also known as nanoporous alumina, nanohole alumina arrays, –NAA– or nanoporous anodized alumina platforms, –NAAP–) has opened new opportunities in a wide range of fields, and is used as an advanced photonic structure for applications in structural coloration and advanced optical biosensing based on the ordered nanoporous structure obtained and as a template to grow nanowires or nanotubes of different materials giving rise to metamaterials with tailored properties. Therefore, understanding the structure of nanoporous anodic alumina templates and knowing how they are fabricated provide a tool for the further design of structures based on them, such as 3D nanoporous structures developed recently. In this work, we review the latest developments related to nanoporous alumina, which is currently a very active field, to provide a solid and thorough reference for all interested experts, both in academia and industry, on these nanostructured and highly useful structures. We present an overview of theories on the formation of pores and self-ordering in alumina, paying special attention to those presented in recent years, and different nanostructures that have been developed recently. Therefore, a wide variety of architectures, ranging from ordered nanoporous structures to diameter changing pores, branched pores, and 3D nanostructures will be discussed. Next, some of the most relevant results using different nanostructured morphologies as templates for the growth of different materials with novel properties and reduced dimensionality in magnetism, thermoelectricity, etc. will be summarised, showing how these structures have influenced the state of the art in a wide variety of fields. Finally, a review on how these anodic aluminium membranes are used as platforms for different applications combined with optical techniques, together with principles behind these applications will be presented, in addition to a hint on the future applications of these versatile nanomaterials. In summary, this review is focused on the most recent developments, without neglecting the basis and older studies that have led the way to these findings. Thus, it gives an updated state-of-the-art review that should be useful not only for experts in the field, but also for non-specialists, helping them to gain a broad understanding of the importance of anodic porous alumina, and most probably, endow them with new ideas for its use in fields of interest or even developing the anodization technique.

16 June 2021 in Advanced Sustainable Systems
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Journal Article
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OCOlga Caballero-Calero
Olga Caballero-Calero
JAJosé R. Ares
José R. Ares
MMMarisol Martin-Gonzalez
Marisol Martin-Gonzalez
This review article gives an overview of the recent research directions in eco‐friendly, non‐toxic, and earth‐abundant thermoelectric materials. It covers materials such as sulfides, tetrahedrites, earth‐abundant oxides, silicides, copper iodine, Half‐Heusler intermetallic compounds, nitrides, and other environmentally friendly thermoelectrics. In all cases, their history, structure, general characteristics, thermoelectric properties, synthesis methods, and related thermoelectric applications are compiled. It is also shown that they are starting to be an excellent alternative for producing cost‐effective, sustainable, and non‐toxic thermoelectric generators. This review does not try to include all possible materials, but to show that there are high zT thermoelectric materials that are starting to be an excellent alternative for producing cost‐effective, sustainable, and non‐toxic thermoelectric generators.

24 October 2014 in Nature Communications
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JMJaime Martín
Jaime Martín
MMMarisol Martin-Gonzalez
Marisol Martin-Gonzalez
JFJose Francisco Fernández
Jose Francisco Fernández
OCOlga Caballero-Calero
Olga Caballero-Calero
Three-dimensional (3D) nanostructures combine properties of nanoscale materials with the advantages of being macro-sized pieces when the time comes to manipulate, measure their properties or make a device. However, the amount of compounds with the ability to self-organize in ordered 3D nanostructures is limited. Therefore, template-based fabrication strategies become the key approach towards 3D nanostructures. Here we report the simple fabrication of a template based on anodic aluminium oxide, having a well-defined, ordered, tunable, homogeneous 3D nanotubular network in the sub 100-nm range. The 3D templates are then employed to achieve 3D, ordered nanowire networks in Bi2Te3 and polystyrene. Finally, we demonstrate the photonic crystal behaviour of both the template and the polystyrene 3D nanostructure. Our approach may establish the foundations for future high-throughput, cheap, photonic materials and devices made of simple commodity plastics, metals and semiconductors.

26 April 2005 in Applied Physics Letters
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Journal Article
Closed access
JOJ. Olivares
J. Olivares
GGG. García
G. García
AGA. García-Navarro
A. García-Navarro
FAF. Agulló-López
F. Agulló-López
OCOlga Caballero-Calero
Olga Caballero-Calero
AGA. García-Cabañes
A. García-Cabañes
We demonstrate a swift ion-beam irradiation procedure based on electronic (not nuclear) excitation to generate a large index jump step-like optical waveguide (Δn0≈0.2,Δne≈0.1) in LiNbO3. The method uses medium-mass ions with a kinetic energy high enough to assure that their electronic stopping power Se(z) reaches a maximum value close to the amorphous (latent) track threshold inside the crystal. Fluorine ions of 20 and 22MeV and fluences in the range (1–30)×1014 are used for this work. A buried amorphous layer having a low refractive index (2.10 at a wavelength of 633nm) is then generated at a controlled depth in LiNbO3, whose thickness is also tuned by irradiation fluence. The layer left at the surface remains crystalline and constitutes the core of the optical waveguide which, moreover, is several microns far from the end of the ion range. The waveguides show, after annealing at 300°C, low propagation losses (≈1dB∕cm) and a high second-harmonic generation coefficient (50%–80% of that for bulk unirradiated LiNbO3, depending on the fluence). The formation and structure of the amorphous layer has been monitored by additional Rutherford backscattering/channeling experiments.

6 December 2012 in ACS Applied Materials & Interfaces
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Journal Article
Closed access
JMJaime Martín
Jaime Martín
CMCristina Vicente Manzano
Cristina Vicente Manzano
OCOlga Caballero-Calero
Olga Caballero-Calero
MMMarisol Martin-Gonzalez
Marisol Martin-Gonzalez