{"id":222,"date":"2019-03-19T17:50:47","date_gmt":"2019-03-19T16:50:47","guid":{"rendered":"https:\/\/grupos.unican.es\/apye\/2019\/?page_id=222"},"modified":"2025-12-04T13:18:13","modified_gmt":"2025-12-04T12:18:13","slug":"proyectos","status":"publish","type":"page","link":"https:\/\/grupos.unican.es\/apye\/proyectos\/","title":{"rendered":"Proyectos"},"content":{"rendered":"\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><tbody><tr><td><\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>PLATAFORMA TECNOL\u00d3GICA MULTIUSO PARA EL ESTUDIO DE PINTURAS, RESTOS \u00d3SEOS Y \u00daTILES PREHIST\u00d3RICOS POR MEDIO DE MICRO-ESPECTROSCOPIA RAMAN PORT\u00c1TIL.<br>PROYECTOS<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PROYECTOS DE I+D CONVOCATORIA 2021<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">SODERCAN Gobierno de Cantabria<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Budget: 20000 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI1: F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2023\/03\/INFORME_FINAL.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">MEMORIA FINAL DE PROYECTO (ver memoria)<\/a><\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"935\" height=\"137\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22.png\" alt=\"\" class=\"wp-image-245\" style=\"width:532px;height:76px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22.png 935w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22-600x88.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22-300x44.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22-768x113.png 768w\" sizes=\"auto, (max-width: 935px) 100vw, 935px\" \/><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>FOTOLUMINISCENCIA AMPLIFICADA POR PLASMONES SUPERFICALES EN NANOMATERIALES DOPADOS CON LANTANIDOS SINTONIZADA MEDIANTE ALTA PRESION<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong> <\/strong>MINISTERIO DE CIENCIA E INNOVACI\u00d3N\/ FEDER UE<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/09\/2022 \u2013 31\/08\/2025 Budget: 113.740 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI1: F. Rodr\u00edguez, PI2: R. Valiente<\/p>\n\n\n\n<div data-wp-context=\"{ &quot;autoclose&quot;: false, &quot;accordionItems&quot;: [] }\" data-wp-interactive=\"core\/accordion\" role=\"group\" class=\"wp-block-accordion is-layout-flow wp-block-accordion-is-layout-flow\">\n<div data-wp-class--is-open=\"state.isOpen\" data-wp-context=\"{ &quot;id&quot;: &quot;accordion-item-2&quot;, &quot;openByDefault&quot;: false }\" data-wp-init=\"callbacks.initAccordionItems\" data-wp-on-window--hashchange=\"callbacks.hashChange\" class=\"wp-block-accordion-item is-layout-flow wp-block-accordion-item-is-layout-flow\">\n<h3 class=\"wp-block-accordion-heading\"><button aria-expanded=\"false\" aria-controls=\"accordion-item-2-panel\" data-wp-bind--aria-expanded=\"state.isOpen\" data-wp-on--click=\"actions.toggle\" data-wp-on--keydown=\"actions.handleKeyDown\" id=\"accordion-item-2\" class=\"wp-block-accordion-heading__toggle\"><span class=\"wp-block-accordion-heading__toggle-title\">Resumen<\/span><span class=\"wp-block-accordion-heading__toggle-icon\" aria-hidden=\"true\">+<\/span><\/button><\/h3>\n\n\n\n<div inert aria-labelledby=\"accordion-item-2\" data-wp-bind--inert=\"!state.isOpen\" id=\"accordion-item-2-panel\" role=\"region\" class=\"wp-block-accordion-panel is-layout-flow wp-block-accordion-panel-is-layout-flow\">\n<p class=\"wp-block-paragraph\">El proyecto ha logrado acometer la mayor\u00eda de los hitos inicialmente propuestos cuyos resultados originales se reflejan en 12 publicaciones en revistas internacionales de prestigio, en la modalidad de <em>open access.<\/em> Los logros mas destacados son los siguientes:<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">En el \u00e1mbito de la <strong>plasm\u00f3nica<\/strong> bajo presi\u00f3n, hemos demostrado que las nanopart\u00edculas de oro son mas sensibles y mec\u00e1nicamente mas estables, cuando tienen forma alargada (bastones y bipir\u00e1mides) y estructura pentamaclada. Adem\u00e1s, las nanopart\u00edculas de oro, tanto monocristalinas como pentamacladas, son ligeramente mas densas (~0.2%) y mas duras (mayor m\u00f3dulo de compresi\u00f3n: ~3%) que el oro macrosc\u00f3pico. Asimismo, hemos demostrado que las nanopart\u00edculas pentamacladas de oro, no tienen estructura fcc, sino que muestran polimorfismo. Hemos desarrollado un modelo basado en la teor\u00eda de la elasticidad que explica la diferente estructura de dichas nanopart\u00edculas en funci\u00f3n de su geometria. Como aplicaci\u00f3n destacable del estudio se ha sugerido el uso como sensores plasm\u00f3nicos para la medida del \u00edndice de refracci\u00f3n del agua y de diversas mezclas de alcoholes, normalmente utilizados como medios transmisores de presi\u00f3n, a altas presiones (hasta 600.000 atm.) en fases policristalinas o v\u00edtreas, hecho que no ha sido posible hasta ahora mediante t\u00e9cnicas convencionales (dispersi\u00f3n Brillouin, interferometr\u00eda, etc.) de medida del \u00edndice de refracci\u00f3n.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">En el \u00e1mbito de los <strong>nano \u00f3xidos luminiscentes<\/strong>, el proyecto ha conseguido diferentes logros en la s\u00edntesis y caracterizaci\u00f3n estructural (estructura y h\u00e1bito cristalinos) de nano\u00f3xidos dopados con iones de tierras raras e iones de transici\u00f3n, correlacionando su eficiencia cu\u00e1ntica luminiscente con la forma, tama\u00f1o y estructura de la nanopart\u00edcula controlado en el proceso de s\u00edntesis o bien debido a transiciones de fase inducidas por presi\u00f3n. Asimismo, se consigui\u00f3 establecer los criterios para integrar dichas nanopart\u00edculas en matrices v\u00edtreas de \u00edndice de refracci\u00f3n similar, con el fin de ser utilizadas en aplicaciones de medios activos l\u00e1ser y en sens\u00f3rica. Otro logro del proyecto fue clarificar supuestos comportamientos luminiscentes de nanopart\u00edculas atribuidos al Cu<sup>2+<\/sup>, demostrando la necesaria aplicaci\u00f3n del m\u00e9todo cient\u00edfico en trabajos de caracterizaci\u00f3n de materiales luminiscentes, demostrando la utilidad de las t\u00e9cnicas de alta presi\u00f3n para constatar la ausencia de luminiscencia en sistemas de Cu<sup>2+<\/sup> as\u00ed como evaluar la eficiencia cu\u00e1ntica luminiscente de Mn<sup>2+<\/sup> en aleaciones con estructuras unidimensionales. Un aspecto destacado del trabajo es la influencia de la presencia de nanopart\u00edculas met\u00e1licas en la amplificaci\u00f3n de la intensidad luminiscente de nanopart\u00edculas activadas \u00f3pticamente. Hemos demostrado que la mera mezcla de nanopart\u00edculas met\u00e1licas de oro con otras luminiscentes, no da lugar a fen\u00f3menos de amplificaci\u00f3n, sino a otros fen\u00f3menos \u00f3pticos de inter\u00e9s relacionados con la captaci\u00f3n e inyecci\u00f3n de luz en part\u00edculas. Su estudio no obstante se alejaba de los objetivos del proyecto.<\/p>\n\n\n\n<div data-wp-context=\"{ &quot;autoclose&quot;: false, &quot;accordionItems&quot;: [] }\" data-wp-interactive=\"core\/accordion\" role=\"group\" class=\"wp-block-accordion is-layout-flow wp-block-accordion-is-layout-flow\">\n<div data-wp-class--is-open=\"state.isOpen\" data-wp-context=\"{ &quot;id&quot;: &quot;accordion-item-1&quot;, &quot;openByDefault&quot;: false }\" data-wp-init=\"callbacks.initAccordionItems\" data-wp-on-window--hashchange=\"callbacks.hashChange\" class=\"wp-block-accordion-item is-layout-flow wp-block-accordion-item-is-layout-flow\">\n<h3 class=\"wp-block-accordion-heading\"><button aria-expanded=\"false\" aria-controls=\"accordion-item-1-panel\" data-wp-bind--aria-expanded=\"state.isOpen\" data-wp-on--click=\"actions.toggle\" data-wp-on--keydown=\"actions.handleKeyDown\" id=\"accordion-item-1\" class=\"wp-block-accordion-heading__toggle\"><span class=\"wp-block-accordion-heading__toggle-title\"><\/span><span class=\"wp-block-accordion-heading__toggle-icon\" aria-hidden=\"true\">+<\/span><\/button><\/h3>\n\n\n\n<div inert aria-labelledby=\"accordion-item-1\" data-wp-bind--inert=\"!state.isOpen\" id=\"accordion-item-1-panel\" role=\"region\" class=\"wp-block-accordion-panel is-layout-flow wp-block-accordion-panel-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<div data-wp-context=\"{ &quot;autoclose&quot;: false, &quot;accordionItems&quot;: [] }\" data-wp-interactive=\"core\/accordion\" role=\"group\" class=\"wp-block-accordion is-layout-flow wp-block-accordion-is-layout-flow\">\n<div data-wp-class--is-open=\"state.isOpen\" data-wp-context=\"{ &quot;id&quot;: &quot;accordion-item-3&quot;, &quot;openByDefault&quot;: false }\" data-wp-init=\"callbacks.initAccordionItems\" data-wp-on-window--hashchange=\"callbacks.hashChange\" class=\"wp-block-accordion-item is-layout-flow wp-block-accordion-item-is-layout-flow\">\n<h3 class=\"wp-block-accordion-heading\"><button aria-expanded=\"false\" aria-controls=\"accordion-item-3-panel\" data-wp-bind--aria-expanded=\"state.isOpen\" data-wp-on--click=\"actions.toggle\" data-wp-on--keydown=\"actions.handleKeyDown\" id=\"accordion-item-3\" class=\"wp-block-accordion-heading__toggle\"><span class=\"wp-block-accordion-heading__toggle-title\">Resultados<\/span><span class=\"wp-block-accordion-heading__toggle-icon\" aria-hidden=\"true\">+<\/span><\/button><\/h3>\n\n\n\n<div inert aria-labelledby=\"accordion-item-3\" data-wp-bind--inert=\"!state.isOpen\" id=\"accordion-item-3-panel\" role=\"region\" class=\"wp-block-accordion-panel is-layout-flow wp-block-accordion-panel-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-accent-color\">Publicaciones en revistas<\/mark><\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Behavior of Au Nanoparticles under Pressure Observed by In Situ Small-Angle X\u2010ray Scattering<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">C. Mart\u00edn-S\u00e1nchez, A. S\u00e1nchez-Iglesias, J.A. Barreda-Arg\u00fceso, A Polian, L. M. Liz-Marz\u00e1n, <strong>F. Rodr\u00edguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>ACS Nano<\/em> <strong>17<\/strong>(1), 743\u2013751 (2023)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acsnano.2c10643\">https:\/\/doi.org\/10.1021\/acsnano.2c10643<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Unveiling the structural and electronic interplay in 3d and 4f\/5d compounds at high-pressure<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">V. Monteseguro, J.A. Sans, V. Cuartero, J. Ruiz-Fuertes, C Popescu, <strong>F. Rodriguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Acta Crystallographica Section A: Foundations and Advance<\/em>, <strong>77<\/strong>, C451 (2021)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/journals.iucr.org\/a\/issues\/2021\/a2\/00\/a60040\/a60040.pdf\">https:\/\/journals.iucr.org\/a\/issues\/2021\/a2\/00\/a60040\/a60040.pdf<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Band-Gap Energy and Electronic d\u2013d Transitions of NiWO<sub>4<\/sub> Studied under High-Pressure Conditions<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Daniel Errandonea, <strong>Fernando Rodriguez<\/strong>, Rosario Vilaplana, David Vie, Siddhi Garg, Bishnupriya Nayak, Nandini Garg, Jaspreet Singh, Venkatakrishnan Kanchana, Ganapathy Vaitheeswaran<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>The Journal of Physical Chemistry C, <\/em><strong>127<\/strong>, 15630-15640 (2023)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acs.jpcc.3c03512\">https:\/\/doi.org\/10.1021\/acs.jpcc.3c03512<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Photoluminescence and Raman study of the high-pressure behavior of monoclinic (Eu<sub>1-x<\/sub>Yb<sub>x<\/sub>)<sub>2<\/sub>O<sub>3&nbsp;<\/sub>solid solutions<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">M.T Candela, <strong>F. Aguado<\/strong>, J.A. Gonz\u00e1lez, <strong>R. Valiente<\/strong> <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>J. Alloys Compd<\/em>. <strong>967<\/strong>, 171621 (1-11) (2023)<br><a href=\"https:\/\/doi.org\/10.1016\/j.jallcom.2023.171621\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/doi.org\/10.1016\/j.jallcom.2023.171621<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>The influence of PEGylated gold nanoparticles on the solidification of alcohols.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">C. Mart\u00edn-S\u00e1nchez, A. S\u00e1nchez-Iglesias, J.A. Barreda-Arg\u00fceso, J.A. Gonz\u00e1lez, <strong>F. Rodr\u00edguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>J. Mat. Chem. C,<\/em><strong>12,<\/strong> 6469-6478 (2024)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1039\/D4TC00358F\">https:\/\/doi.org\/10.1039\/D4TC00358F<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Spectroscopic, vibrational and structural insights into LaYbO<sub>3<\/sub>: Pr<sup>3+<\/sup> and LaLuO<sub>3<\/sub>: Pr<sup>3+<\/sup>, Tb<sup>3+<\/sup> perovskites at ambient and high-pressure conditions.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">M.T. Candela, <strong>F. Aguado<\/strong>, V. Monteseguro, J.A. Gonz\u00e1lez, <strong>R. Valiente<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Ceramics International, <\/em><strong>51<\/strong>, 16539-16550 (2024).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1016\/j.ceramint.2024.09.151\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/doi.org\/10.1016\/j.ceramint.2024.09.151<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Optical spectroscopy of exchange-coupled ions: Insights into homonuclear, heteronuclear and mixed transition-metal\/rare-earth systems.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">D. P\u00e9rez-Franc\u00e9s, <strong>F. Rodr\u00edguez<\/strong>, <strong>R. Valiente<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Optical Materials<\/em>, 116965 (2025).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1016\/j.optmat.2025.116965\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/doi.org\/10.1016\/j.optmat.2025.116965<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Pressure-induced modifications of magnetic and optical properties in Yb<sup>3+<\/sup>-doped CrBr<sub>3<\/sub>.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">T. J. Snoeren, M.T. Candela, <strong>R. Valiente<\/strong>, D.R. Gamelin<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Optical Materials<\/em>, 117102 (2025).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1016\/j.optmat.2025.117102\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/doi.org\/10.1016\/j.optmat.2025.117102<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Highly sensitive optical nanothermometry using Er<sup>3+<\/sup>-doped GdOF nanoparticles: synthesis, characterization, and temperature sensing applications.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">F. Scardaci, J.I. Espeso, D. P\u00e9rez-Franc\u00e9s, G. Malandrino, <strong>R. Valiente<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Journal of Luminescence<\/em>, 121290 (2025).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1016\/j.jlumin.2025.121290\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/doi.org\/10.1016\/j.jlumin.2025.121290<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Correspondence on \u201cSuppressing Energy Migration via Antiparallel Spin Alignment in One\u2010Dimensional Mn<sup>2+<\/sup> Halide Magnets with High Luminescence Efficiency\u201d<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Angewandte Chemie International Edition<\/em>, <strong>64<\/strong>(33), e202509184 (2025).<a href=\"https:\/\/doi.org\/10.1002\/anie.202509184\">https:\/\/doi.org\/10.1002\/anie.202509184<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Origin of the rich polymorphism of gold in penta-twinned nanoparticles.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">C. Mart\u00edn-S\u00e1nchez, A. S\u00e1nchez-Iglesias, J.A. Barreda-Argueso, J.P. Iti\u00e9, P. Chauvigne, L.M. Liz-Marz\u00e1n, <strong>F. Rodr\u00edguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Nano Letters<\/em>, <strong>25<\/strong>(9), 3588-3596 (2025)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acs.nanolett.4c06473\">https:\/\/doi.org\/10.1021\/acs.nanolett.4c06473<\/a><em>\u201copen access\u201d<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Optical and Vibrational properties of Rb<sub>2<\/sub>CuCl<sub>4<\/sub>(H<sub>2<\/sub>O)<sub>2<\/sub>. Pseudo Jahn-Teller distortion.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">L. G\u00f3mez, <strong>F. Rodriguez<\/strong>, <strong>F. Aguado<\/strong>, <strong>R. Valiente<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Physical Review B<\/em> <strong>00<\/strong>, 004100 (2025) Aceptado<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1103\/hqd1-wl7f\">https:\/\/doi.org\/10.1103\/hqd1-wl7f<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>YPO<sub>4<\/sub>: Pr<sup>3+<\/sup> nanocrystal embedded into an optical fiber<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">D. Dorosz, M. Kochanowicz, <strong>R. Valiente<\/strong>, A. Diego-Rucabado, <strong>F. Rodr\u00edguez<\/strong>, N. Si\u00f1eriz-Niembro, J. I Espeso, M. Lesniak, P. Miluski, S. Conzendorf, J. Posseckardt, Z. Liao, G. L. Jimenez, R. M\u00fcller, M. Lorenz, A. Schwuchow, M. Leich, A. Lorenz, K. Wondraczek, M. J\u00e4ger<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Research SQUARE <\/em>(2024)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.21203\/rs.3.rs-3837039\/v1\">https:\/\/doi.org\/10.21203\/rs.3.rs-3837039\/v1<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Pr<sup>3+<\/sup>-doped YPO<sub>4<\/sub> nanocrystal embedded into an optical fiber.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">D. Dorosz, M. Kochanowicz, <strong>R. Valiente<\/strong>, A. Diego-Rucabado, <strong>F. Rodr\u00edguez<\/strong>, N. Si\u00f1eriz-Niembro, J. I Espeso, M. Lesniak, P. Miluski, S. Conzendorf, J. Posseckardt, Z. Liao, G. L.Jimenez, R. M\u00fcller, M. Lorenz, A. Schwuchow, M. Leich, A. Lorenz, K. Wondraczek, M. J\u00e4ger<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Scientific Reports<\/em>, 14(1), 7404 (2024) <em>\u201copen access\u201d.<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1038\/s41598-024-57307-4\">https:\/\/doi.org\/10.1038\/s41598-024-57307-4<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Pr<sup>3+<\/sup>-doped Y<sub>2<\/sub>O<sub>3<\/sub> nanocrystals embedded in Y<sub>2<\/sub>O<sub>3<\/sub> thin films as a sandwich-like structure prepared by pulsed laser deposition<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">A. Diego-Rucabado, A. Segura<strong>, F. Aguado<\/strong>, M. Pollnau, <strong>R. Valiente<\/strong>, R. Mart\u00edn-Rodr\u00edguez, I. Cano<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>J. Lumin.<\/em> 252, 119378 (2022)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1016\/j.jlumin.2022.119378\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/doi.org\/10.1016\/j.jlumin.2022.119378<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Visible Light Active Ce-Doped and Cu\u2013Ce co-doped TiO<sub>2<\/sub> Nanocrystals and Optofluidics for Clean Alcohol Production from CO<sub>2<\/sub><\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">A. Diego-Rucabado, I. Merino-Garcia, J. I Espeso, J. Gonz\u00e1lez, B. Arce, <strong>R. Valiente<\/strong>, G. Beobide, I. Cano, R. Mart\u00edn-Rodr\u00edguez, I. de Pedro, J. Albo<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>ACS Sustainable Chem. Eng.<\/em> 11, 13260\u201313273 (2023)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acssuschemeng.3c01925\">https:\/\/doi.org\/10.1021\/acssuschemeng.3c01925<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Optical fibre doped with YPO<sub>4<\/sub>:Pr<sup>3+<\/sup> nanocrystals &#8211; glass powder doping technique for new laser transitions<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">D. Dorosz, M. Kochanowicz, <strong>R. Valiente<\/strong>, A. Diego-Rucabado, N. Si\u00f1eriz-Niembro, M. Lesniak, J. Posseckardt, G. L. Jimenez, R. M\u00fcller, M. Lorenz, A. Schwuchow, M. Leich, K. Wondraczek, M. J\u00e4ger<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>The European Conference on Lasers and Electro-Optics<\/em> 2023<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Munich, Alemania, 26\u201330 junio 2023<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/opg.optica.org\/abstract.cfm?URI=CLEO_Europe-2023-ce_1_4\">https:\/\/opg.optica.org\/abstract.cfm?URI=CLEO_Europe-2023-ce_1_4<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Glass powder doping of nanocrystal-doped fibres: challenges and results<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">D. Dorosz, M. Kochanowicz, M. Lesniak, R. M\u00fcller, M. Lorenz, J. Kobelke, K. Wondraczek, <strong>R. Valiente<\/strong>, A. Diego-Rucabado, I. Cano, <strong>F. Aguado<\/strong>, J. Gluch, I. Kinski, M. J\u00e4ger,<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>SPIE Photonics Europe, 2022<\/em>. Strasbourg, France (25 May 2022). <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1117\/12.2624448\">https:\/\/doi.org\/10.1117\/12.2624448<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Comparison of different synthesis routes to prepare Pr<sup>3+<\/sup>-doped Y<sub>2<\/sub>O<sub>3<\/sub> nanocrystals optically active in the biological windows<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">A. Diego Rucabado, M.T. Candela, <strong>F. Aguado<\/strong>, J. Gonz\u00e1lez, <strong>F. Rodr\u00edguez<\/strong>, <strong>R. Valiente<\/strong>, R. Mart\u00edn, Rodr\u00edguez, I. Cano.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>3rd Conference of the Nanomaterials Applied to Life Science<\/em> NALS 2022. 27-29 abril 2022, Santander, Espa\u00f1a<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Conferencia invitada: \u201cOptimization of Y<sub>2<\/sub>O<sub>3<\/sub>:Pr<sup>3+<\/sup> nanocrystals and stability after embedding in a glass matrix\u201d<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">A. Diego-Rucabado, I. Cano, R. Martin-Rodr\u00edguez, <strong>F. Aguado<\/strong>, D. Dorosz, M. Kochanowicz, R. M\u00fcller, M. J\u00e4ger, J. Posseckardt, <strong>R. Valiente<\/strong>. <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>International Symposium on Photoluminescence in Rare Earths: Photonic Materials PRE\u20192<\/em>. 11-14 septiembre&nbsp; 2022 Szczawnica, Polonia<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>High-pressure structural stability and luminescence studies of nanoclays for environmental applications.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">A.C. Perdig\u00f3n; M. Candela; <strong>F. Aguado<\/strong>; J. Gonz\u00e1lez; C. Renero-Lecuna, R. Mart\u00edn-Rodr\u00edguez.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>28<sup>th<\/sup> AIRAPT and 60<sup>th<\/sup> EHPRG International Conference on High Pressure Science and Technology<\/em> 23-28 julio 2023. Edimburgo. Reino Unido.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Stability and High-Pressure behaviour of Paracetamol polymorphs through Raman spectroscopy.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>F. Aguado<\/strong>, M. T. Candela, A. C. Perdig\u00f3n, J. A. Gonz\u00e1lez, <strong>R. Valiente.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>28<sup>th<\/sup> AIRAPT and 60<sup>th<\/sup> EHPRG International Conference on High Pressure Science and Technology<\/em>. 23-28 julio 2023. Edimburgo. Reino Unido<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>An appraisal of Understanding Pressure Effects on Structural, Optical, and Magnetic Properties of CsMnF<sub>4<\/sub> and Other 3d<sup>n<\/sup> Compounds<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Fernando Rodriguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">2025\/3\/27<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>arXiv preprint arXiv:2503.21451<\/em> <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">DOI: 10.48550\/arXiv.2503.21451 (Repositorio, Cornell University)<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-accent-color\"><strong>Publicaciones en libros<\/strong><\/mark><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Avance al estudio del arte rupestre de la cueva de la brazada (Riba, Ruesga, Cantabria, Espa\u00f1a)<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">R. Onta\u00f1\u00f3n, R. Montes, E. Mu\u00f1oz, J.M. Morlote, V. Vayarri, J. Herrera, E. Castillo, E. Palacio, J. Gonz\u00e1lez, J.A. Barreda-Arg\u00fceso, <strong>F. Rodr\u00edguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Cap\u00edtulo del libro \u201cIm\u00e1genes de la Prehistoria. Estudios en homenaje al Profesor Alfonso Moure Romanillo\u201d Ed. Universidad de Cantabria, pgs. 313-344 (2025). ISBN 978-84-19897-01-5<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.22429\/Euc2025.003\">https:\/\/doi.org\/10.22429\/Euc2025.003<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Caracterizaci\u00f3n por Espectroscopia Raman y difracci\u00f3n de rayos X Cap\u00edtulo del libro \u201cLa cueva de Errotalde I : un dep\u00f3sito funerario aziliense en el Pirineo navarro\u201d <\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">J. Gonz\u00e1lez, <strong>F. Rodr\u00edguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Ed. Gobierno de Navarra, Departamento de Cultura, Deporte y Turismo, pgs. 211-217 (2025). ISBN: 978-84-235-3720-4 <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/web.unican.es\/portal-investigador\/publicaciones\/detalle-publicacion?pi=LIB7218\">https:\/\/web.unican.es\/portal-investigador\/publicaciones\/detalle-publicacion?pi=LIB7218<\/a><\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-accent-color\">Patentes<\/mark><\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Procedimiento de fabricaci\u00f3n de un sustrato met\u00e1lico con recubrimiento de grafeno<\/strong><br><br>Inventores\/as: D. FERRE\u00d1O, J. A. GONZALEZ, <strong>F. RODR\u00cdGUEZ<\/strong><br>Patente Nacional, N\u00famero de solicitud: P20243021722\/03\/2024 (Licenciada)<\/p>\n\n\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><tbody><tr><td><\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><tbody><tr><td><br><\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><tbody><tr><td><\/td><\/tr><\/tbody><\/table><\/figure>\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2025\/12\/logo-1024x141.jpg\" alt=\"La imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es logo-1024x141.jpg\"\/><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>MODIFICACIONES ELECTRONICAS Y MAGNETICAS EN DOBLES PEROVSKITAS DE HIERRO BAJO EXTREMAS CONDICIONES <\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">MINISTERIO DE CIENCIA E INNOVACI\u00d3N\/ FEDER UE<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/09\/2022 \u2013 31\/08\/2025 Budget: 78.650 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI1: V. Monteseguro Padr\u00f3n; PI2: J. Ruiz Fuertes<\/p>\n\n\n\n<figure class=\"wp-block-image size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"261\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2022\/12\/imagen-2.png\" alt=\"\" class=\"wp-image-693\" style=\"width:453px;height:115px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2022\/12\/imagen-2.png 1024w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2022\/12\/imagen-2-300x76.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2022\/12\/imagen-2-768x196.png 768w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2022\/12\/imagen-2-600x153.png 600w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>MICROESPECTROSCOP\u00cdA RAMAN CONFOCAL COMO HERRAMIENTA DE DIAGN\u00d3STICO PARA EL SARS-COV-2 Y OTROS CORONAVIRUS<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">IDIVAL<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2021-31\/12\/2022 Budget: 18.000 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: R. Valiente<\/p>\n\n\n\n<figure class=\"wp-block-image size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"387\" height=\"130\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/IDIVAL.png\" alt=\"\" class=\"wp-image-485\" style=\"width:290px;height:98px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/IDIVAL.png 387w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/IDIVAL-300x101.png 300w\" sizes=\"auto, (max-width: 387px) 100vw, 387px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DESARROLLO DE UN DISPOSITIVO ENDOSC\u00d3PICO PARA EL TRATAMIENTO DE C\u00c1NCER DE CABEZA-CUELLO MEDIANTE HIPERTERMIA FOTOINDUCIDA CON NANOPART\u00cdCULAS MULTIFUNCIONALES <\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">AES\/DTS&nbsp; Instituto Salud Carlos III<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2020 &#8211; 31\/12\/2021&nbsp;&nbsp;&nbsp; Budget: 56.100 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: M. L\u00f3pez Fanarraga<\/p>\n\n\n\n<figure class=\"wp-block-image size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"382\" height=\"132\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/Carlos_III.png\" alt=\"\" class=\"wp-image-484\" style=\"width:287px;height:99px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/Carlos_III.png 382w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/Carlos_III-300x104.png 300w\" sizes=\"auto, (max-width: 382px) 100vw, 382px\" \/><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>MODIFICACION MEDIANTE ALTA PRESION DE LAS PROPIEDADES PLASMONICAS Y LUMINISCENTES DE NANOPARTICULAS DE METALES Y OXIDOS DESNUDAS Y RECUBIERTAS (PGC2018-101464-B-I00) MCI\/AEI\/FEDER,UE <\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2019 \u2013 31\/12\/2021&nbsp;&nbsp; Budget: 96.800 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez, R. Valiente<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/Resumen.pdf\">RESUMEN POYECTO\/PROJECT SUMMARY<\/a><\/p>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Las siguientes publicaciones y proceedings de congresos son resultados de invesitigaci\u00f3n del proyecto de I+D+i <strong>PGC2018-101464-B-I00<\/strong>, financiado por MCIN\/ AEI\/10.13039\/501100011033\/ y \u201cFEDER Una manera de hacer Europa\u201d.<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Pressure dependence of the crystal-field spectrum of KNiF3: Single and double excitations<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> J. A. Barreda-Arg\u00fceso and F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> PHYSICAL REVIEW B 103, (2021)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 103 <strong>Pag:<\/strong> 085115&nbsp;&nbsp;<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> This work investigates the Ni-F distance dependence of the crystal-field (CF) transitions of Ni2+ in KNiF3 by high-pressure spectroscopy. All peaks shift to higher energy with pressure according to trends foreseen by the Tanabe-Sugano diagram. At ambient conditions, we obtain Racah and CF splitting parameters of B = 0.118 eV, 10Dq = 0.908 eV; C\/B = 4.4 (10Dq\/B = 7.7). B and 10Dq vary with pressure as \u2202B \u2202P= \u20130.11 meVGPa\u20131and \u220210Dq\u2202P = 24 meVGPa\u20131. Similar to KCoF3, the slight decrease of B with pressure reflects the strong ionic character of the Ni-F bond and its high stability against compression. We have correlated the measured pressure dependence of 10Dq with the Ni-F bond distance, showing that it follows a potential law as 10Dq = CR\u2013n with an exponent n = 6.6 \u00c5} 0.5, thus providing experimental data for checking the suitability of theoretical models aiming to explain the slight deviations of observed R dependencies of 10Dq from the CF theory (n = 5).We have applied the experimental 10Dq(R) relationship to determine the real Ni-F bond distances in fluoroperovskites ABF3 : Ni2+ from the spectroscopically measured 10Dq as an alternative method for determining bond distances, RNi\u2212F, in impurity systems. We show that the so-obtained RNi\u2212F deviates from the bond distance of the host site, RB\u2212F, proportionally to the difference RB\u2212F \u2212 R0, with R0 being the sum of ionic radii RF\u2212 + RNi2+ . The behavior is compared to that found for Mn2+ along the fluoroperovskite series ABF3 : Mn2+. Finally, weak UV peaks observed below the charge-transfer band gap (Eg _ 10 eV) in the absorption spectrum, the assignment of which still remains controversial, have been assigned to single and double excitation transitions. The assignment was unveiled on the basis of their energy and pressure shift.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> OPTICAL<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI<\/strong>: 10.1103\/PhysRevB.103.085115<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">3D optimal light distribution in brain tumors for photodynamic therapy<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> R. de la Nuez-D\u00edaz, J. L. Arce-Diego, F. Fanjul-V\u00e9lez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> Proceedings Optical Interactions with Tissue and Cells XXXII; 116400D (2021)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 11640 <strong>Pag:<\/strong> 0 <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> Photodynamic therapy is a treatment technique that takes advantage of the effects induced by the body itself, together with a photosensitizer, to destroy unwanted tumor volumes with high accuracy and low invasiveness. This study analyzes treatment volume by 3D optical distributions in a realistic way from MRI images. First of all a volumetric model of a real head is built from MRI images. Optical distributions generated by the source over the tissue are considered at different brain tumor stages, and with multitude of processes that occur within the volume to be treated. By means of Monte Carlo we can estimate the photonic density that is absorbed by the tissues, whose optical properties are previously collected. This application considers that a reasonable time has passed for the photosensitizer to have reached the area under study, and that there is a minimum concentration in adjoining areas during radiation exposure. With this approach it is possible to estimate the level of radiation exposure and the affected volume. This is very relevant due to the fact that, as the radiation increases, different areas with different energy densities appear. This makes it much more complicated to apply a certain known optimal radiation on the treatment volume. A non-optimal high radiation density would damage healthy tissue, while, on the contrary, a non-optimal low radiation would not bring unwanted tissue to necrosis or apoptosis for tumor destruction, generating recurrence. This tool could be of great interest in treatment planning.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> OPTICAL<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI<\/strong>: <a href=\"https:\/\/doi.org\/10.1117\/12.2578313\">https:\/\/doi.org\/10.1117\/12.2578313<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Digital Histology by Phase Imaging Specific Biomarkers for Human Tumoral Tissues Discrimination<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> Jos\u00e9&nbsp; Luis Ganoza-Quintana, F\u00e9lix Fanjul-V\u00e9lez and Jos\u00e9&nbsp; Luis Arce-Diego<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> Digital Histology by Phase Imaging Specific Biomarkers for Human Tumoral Tissues Discrimination. Appl. Sci. 2021, 11, 6142<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 11640 <strong>Pag:<\/strong> 0 <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> Histology is the diagnosis gold standard. Conventional biopsy presents artifacts, delays, or human bias. Digital histology includes automation and improved diagnosis. It digitalizes microscopic images of histological samples and analyzes similar parameters. The present approach proposes the novel use of phase contrast in clinical digital histology to improve diagnosis. The use of label-free fresh tissue slices prevents processing artifacts and reduces processing time. Phase contrast parameters are implemented and calculated: the external scale, the fractal dimension, the anisotropy factor, the scattering coefficient, and the refractive index variance. Images of healthy and tumoral samples of liver, colon, and kidney are employed. A total of 252 images with 10_, 20_, and 40_ magnifications are measured. Discrimination significance between healthy and tumoral tissues is assessed statistically with ANOVA (p-value &lt; 0.005). The analysis is made for each tissue type and for different magnifications. It shows a dependence on tissue type and image magnification. The p-value of the most significant parameters is below 10\udbc0\udc005. Liver and colon tissues present a great overlap in significant phase contrast parameters. The 10_ fractal dimension is significant for all tissue types under analysis. These results are promising for the use of phase contrast in digital histology clinical praxis<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> digital histology; phase contrast imaging; biomarkers; biomedical optics; fractal analysis<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI<\/strong>: <a href=\"https:\/\/doi.org\/10.1117\/12.2578313\">https:\/\/doi.org\/ 10.3390\/app11136142<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Stokes and upconverted luminescence in Er3+\/Yb3+-doped Y3Ga5O12 nano-garnets<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> Virginia Monteseguro, Vemula Venkatramu, Ulises R. Rodr\u00edguez-Mendoza &nbsp;and&nbsp; Victor Lav\u00edn Luis Arce-Diego<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> Dalton Transactions <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 50 <strong>Pag:<\/strong> 9512-9518<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> The green, red, near-infrared and near-infrared-to-visible upconverted luminescence properties of Er3+\/Yb3+ codoped Y3Ga5O12 nanocrystalline powders have been studied using laser spectroscopy. A diffuse reflectance and luminescence spectra confirm that Er3+ and Yb3+ ions occupy the Y3+ sites of the single-phase cubic nano-garnet. Very bright green and red luminescence of the Er3+ ions are detected by the naked eyes, even for a laser power as low as 15 mW, when the Yb3+ ions are excited at 970 nm. The red upconverted emission is more intense than that under direct excitation of the Er3+ ions. The power dependence and the dynamics of the near-infrared-to-green and near-infrared-to-red upconverted emissions show the existence of different two-photon energy transfer upconversion processes. The results here presented indicate that Er3+\/Yb3+ codoped Y3Ga5O12 can be a good candidate as an optical nanoheater and nanothermometer in biomedicine applications in the first biological window.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> digital histology; phase contrast imaging; biomarkers; biomedical optics; fractal analysis<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI<\/strong>: <strong>:<\/strong> <a href=\"https:\/\/doi.org\/10.1039\/D1DT00976A\">https:\/\/doi.org\/10.1039\/D1DT00976A<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">A custom-made functionalization method to control the biological identity of nanomaterials<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> E. Pad\u00edn-Gonz\u00e1lez, E. Navarro-Palomares, L. Valdivia, N. Iturrioz-Rodr\u00edguez, M. A. Correa, <strong>R. Valiente<\/strong>, M. L. Fanarraga<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong><em> <\/em><em>Nanomedicine, Nanotechnology, Biology, and Medicine<\/em>ctions <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong>  <strong>Pag:<\/strong> <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> Here we propose a one-step strategy to endow nanomaterials with a custom-designed bio-identity. This study designs a universal &#8216;nanomaterial binding domain&#8217; that can be genetically attached to any protein ensuring precise and spontaneous protein orientation. We demonstrate how, despite the simplicity of the method, the bioconjugation achieved: (i) is highly efficient, even in the presence of competing proteins, (ii) is stable at extreme physiological conditions (pH ranges 5.2-9.0; NaCl concentrations 0-1 M); (iii) prevents unwanted protein biofouling days after incubation in biologically-relevant conditions; and finally, (iv) avoids nanoparticle interaction with promiscuous unspecific receptors. In summary, this protein biocoating technique, applicable to a wide array of nano-designs, integrates material science and molecular biology procedures to create hybrid nanodevices with well-defined surfaces and predictable biological behaviors, opening a chapter in precision nanodiagnostics, nanosensing or nanotherapeutic applications.ological window.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> Biofouling; Biotechnology; Chimera protein; Electrostatic interaction; Nano\u2013bio interface.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI<\/strong>: <strong>:<\/strong> <a href=\"https:\/\/doi.org\/10.1039\/D1DT00976A\">https:\/\/doi.org\/<\/a>10.1016\/j.nano.2020.102268<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Exploiting optical properties of nanopolycrystalline diamond in high pressure experiments<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> J. A. Barreda-Arg\u00fceso, J. Gonz\u00e1lez, R. Valiente, T. Irifune and F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>High Pressure Research<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 40&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 117-118<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract<\/strong>: We investigated the optical properties (absorption, luminescence and Raman spectra) of nanopolycrystalline diamond (NPD) aiming at exploring its capabilities as a pressure sensor and as a pressure-cell anvil for combined X-ray\/neutron and optical studies. Notably, we analysed the Raman peak shift and broadening with pressure using a Moissanite Anvil Cell (MAC). The results are compared with those obtained in a DAC, where Raman signals from NPD chips and diamond anvils strongly overlap. Its pressure behaviour in the hydrostatic and non-hydrostatic regimes were investigated. We showed that the nanopolycrystalline structure induces remarkable differences in the peak shift and broadening between NPD and natural type IIa single-crystal diamond, making NPD suitable as pressure gauge for pressure determination and testing hydrostaticity of pressure transmitting medium.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> Raman spectroscopy Luminescence Pressure gauge Pressure sensitivity Nanopolycrystalline diamond<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI:<\/strong><a href=\"https:\/\/doi.org\/10.1021\/acs.jpcc.0c01419\"> <\/a><a href=\"https:\/\/doi.org\/10.1080\/08957959.2019.1702173\">10.1080\/08957959.2019.1702173<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Plasmonic Sensing of Refractive Index and Density in Methanol\u2013Ethanol Mixtures at High Pressure<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> <strong>C. Mart\u00edn-S\u00e1nchez<\/strong>, A. S\u00e1nchez-Iglesias, P. Mulvaney, L. M. Liz-Marz\u00e1n, and <strong>F. Rodr\u00edguez<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>The Journal of Physical Chemistry C<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 124 (16)&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 8978-8983<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract<\/strong>: The localized surface plasmon resonance (LSPR) of gold nanospheres dispersed in methanol\u2013ethanol 4:1 was measured as a function of pressure up to 60 GPa. The LSPR exhibits an intense red-shift with pressure in the range of 0\u201310 GPa, followed by a slower blue-shift at higher pressures. This is because an increase in the solvent refractive index with pressure leads to a red-shift of the LSPR peak wavelength while an increase in the electron density of the gold nanospheres with pressure leads to a blue-shift. Solvent solidification at 10 GPa and associated nonhydrostatic effects have a negligible influence on the LSPR shifts in the case of nanospheres. Here we show that both the LSPR shifts and changes in the nanospheres absorption coefficient can be explained on the basis of Gans\u2019 model, and this enables the solvent refractive index and the density of the solvent to be determined across the hydrostatic pressure range from 0 to 60 GPa. Interestingly, plasmonic sensing shows no evidence of crystallization or glass phase transitions in MeOH\u2013EtOH 4:1 within the explored pressure range.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> Metal nanoparticles, Gold, Optical properties, Surface plasmon resonance, Solvents<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Pressure-and temperature induced phase transitions, piezochromism, NLC behaviour and pressure controlled Jahn-Teller switching in a Cu-based framework.<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> C. McMonagle, P. Comar, G. S. Nichol, D. R. Allan, <strong>J. A. Barreda-Arg\u016beso, J. A. Gonzalez, F. Rodriguez, R. Valiente, <\/strong>G. Turner, E. K. Brechin and St. A. Moggach<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>Chemical Science<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 11&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 3788793-8799<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract<\/strong>: <em>In situ<\/em> single-crystal diffraction and spectroscopic techniques have been used to study a previously unreported Cu-framework bis[1-(4-pyridyl)butane-1,3-dione]copper(II) (CuPyr-I). CuPyr-I was found to exhibit high-pressure and low-temperature phase transitions, piezochromism, negative linear compressibility, and a pressure induced Jahn\u2013Teller switch, where the switching pressure was hydrostatic media dependent.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI:<\/strong> <a href=\"https:\/\/doi.org\/10.1039\/D0SC03229H\">https:\/\/doi.org\/10.1039\/D0SC03229H<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Comment on \u201cCopper-Substituted Lead Perovskite Materials Constructed with Different Halides for Working (CH3NH3)2CuX4\u2010Based Perovskite Solar Cells from Experimental and Theoretical View\u201d<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> R. Valiente and F. Rodriguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>JACS Applied Materials &amp; Interfaces<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 12&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 37807-37810<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract<\/strong>: In recent years, two-dimensional perovskites have received considerable attention for their potential applications for optoelectronics. Contrary to previous publications, we demonstrate that (CH<sub>3<\/sub>NH<sub>3<\/sub>)<sub>2<\/sub>CuCl<sub>4<\/sub> hybrid organic\u2013inorganic layered perovskite does not show any room-temperature photoluminescence (PL) under UV excitation. This statement can be extended to other perovskites with general formula <em>AMX<\/em><sub>3<\/sub> or <em>A<\/em><sub>2<\/sub><em>MX<\/em><sub>4<\/sub>, based on <em>M<\/em>: Cu<sup>2+<\/sup> and <em>X<\/em>: Cl<sup>\u2013<\/sup> or Br<sup>\u2013<\/sup>. These materials, the object of increasing interest because of their efficient light absorption in a wide UV\u2013vis\u2013NIR range ideal for solar cells and optoelectronics, lack PL at room temperature, in contrast to recent findings reporting PL properties in this and other similar Cu<sup>2+<\/sup>-related materials.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> Absorption, Crystal structure, Solar cells, Optoelectronics, Perovskites<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Exploring pressure effects on metallic nanoparticles and surrounding media through plasmonic sensing<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> C. Mart\u00edn-S\u00e1nchez, S. Seibt, J. A. Barreda-Arg\u00fceso and F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>Journal of Physics: Conference Series<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 1609(1)&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 012009 (7p)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract<\/strong>: The sensing capabilities of gold nanorods under high-pressure conditions were investigated in methanol-ethanol mixtures (up to 13 GPa) and in water (up to 9 GPa) through their optical extinction. The longitudinal SPR band of AuNR exhibits a redshift with pressure which is the result of two main competing effects: compression of the conduction electrons which increases the bulk plasma frequency (blueshift) and increase in the solvent density (redshift). The variation in de SPR peak wavelength allows us to estimate the bulk modulus of the gold nanoparticles with a precision of 10 % and to obtain analytical functions providing the pressure dependence of the refractive index of water in three phases: liquid, ice VI and ice VII. Furthermore, the SPR band shows abrupt jumps at the liquid to ice phase VI and ice phase VII transitions, which are in accordance with the first-order character of these transitions.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI: <\/strong><a href=\"https:\/\/doi.org\/10.1088\/1742-6596\/1609\/1\/012009\">10.1088\/1742-6596\/1609\/1\/012009<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">High Pressure optical nanothermometer based on Er3+ photoluminescence<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> V. Guti\u00e9rrez-Cano, R. Valiente, J.A. Gonz\u00e1lez, and F. Rodriguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>Journal of Physics: Conference Series<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 1609(1)&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 12004 (9p)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract<\/strong>:<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">The optical properties of a sparsely investigated material, LaGdO3 doped with Er3+, are explored regarding its suitability as nanothermometer. Besides its excellent capabilities for dielectric applications, when doping with Er3+, this material provides a highly efficient upconversion photoluminescence (PL) for high temperature thermometry at high pressure due to its structural stability. LaGdO3 belongs to the perovskite-type ABO3 compounds with a B-type monoclinic C2\/m space group (a = 14.43 \u00c5; b = 3.69 \u00c5; c = 9.00 \u00c5; and \u03b2 = 100.70\u00ba) at ambient conditions. It undergoes a structural phase transition to a hexagonal \ud835\udc433#\ud835\udc5a1 phase at 3 GPa yielding a notable PL enhancement, thus enabling it as a potential high-pressure hightemperature nanothermometer.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">DOI: <a href=\"http:\/\/dx.doi.org\/10.1088\/1742-6596\/1609\/1\/012005\">doi:10.1088\/1742-6596\/1609\/1\/012004<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">CaCu3Ti4O12: pressure dependence of electronic and vibrational structures<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> E. Jara, J. Gonz\u00e1lez, F. Aguado, R. Valiente and F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>Journal of Physics: Conference Series<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 1609(1)&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 12005 (7p)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract<\/strong>: The effects of pressure in electronic and vibrational properties of the double perovskite CaCu3Ti4O12 have been investigated in the 0-25 GPa range by optical absorption and Raman spectroscopy. Besides a full structural characterization, we aim at unveiling whether the ambient Im3 crystal structure is stable under high pressure conditions and how its giant dielectric permitivity and electronic gap varies with pressure. Results show that there is evidence of neither structural phase transition nor metallization in CaCu3Ti4O12 in the explored pressure range. We have observed the eight Raman active modes associated with its Im3 crystal phase and obtained their corresponding frequency and pressure shift. Moreover, the direct electronic band gap (2.20 eV), which is mainly associated with the oxygen-to-copper charge transfer states, increases slightly with pressure at a rate of 13 meV GPa?1 from 0 to 10 GPa. Above this pressure is almost constant (Eg = 2.3 eV). The results highlight the high stability of the compound in its Im3 phase against compression.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI:<\/strong> <a href=\"http:\/\/dx.doi.org\/10.1088\/1742-6596\/1609\/1\/012005\">10.1088\/1742-6596\/1609\/1\/012005<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Structural Correlations in Jahn\u2013Teller Systems of Mn3+ and Cu2+: Unraveling Local Structures through Spectroscopic Techniques<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> M. T. Candela, E. Jara, F. Aguado, R. Valiente, and F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>Inorganic Chemistry<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 124&nbsp;&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 22692-22703<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> An experimental correlation study between the low-symmetry 3d orbital splitting pattern, \u0394<sub>e<\/sub> and \u0394<sub>t<\/sub>, determined by optical spectroscopy, and the local distortion \u03c1, determined by X-ray diffraction, for different Cu<sup>2+<\/sup> and Mn<sup>3+<\/sup> fluorides and chlorides is presented. Single crystals of different dimensionalities were explored, some of them studied under high-pressure conditions. The collection of structural and spectroscopic data provides structural correlations relating \u03c1 and \u0394<sub>e<\/sub> and \u0394<sub>t<\/sub> in Cu<sup>2+<\/sup> and Mn<sup>3+<\/sup> systems, showing that \u0394<sub>e<\/sub> (and \u0394<sub>t<\/sub>) scales with \u03c1. Such correlations can be used to estimate local distortions of Cu<sup>2+<\/sup> (or Mn<sup>3+<\/sup>) introduced as impurities in different chloride and fluoride host lattices from spectroscopic data. The results can be interpreted in the framework of the Jahn\u2013Teller theory and provide support for the proposed structural scenario. The influence of the crystal anisotropy in the local structure is analyzed as well and compared with transition metal ion systems having <em>E<\/em>\u2297<em>e<\/em> Jahn\u2013Teller (Cu<sup>2+<\/sup>, Mn<sup>3+<\/sup>) and singly orbital (Ni<sup>2+<\/sup>, Mn<sup>2+<\/sup>, Fe<sup>3+<\/sup>) ground states in octahedral symmetry.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> Group theory, Crystals, Anions, Transition metals, Ions<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI: <a href=\"https:\/\/doi.org\/10.1021\/acs.jpcc.0c07243\">https:\/\/doi.org\/10.1021\/acs.jpcc.0c07243<\/a><\/strong><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Application of Classification Algorithms to Diffuse Reflectance Spectroscopy Measurements for Ex Vivo Characterization of Biological Tissues<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Autors:<\/strong> F\u00e9lix Fanjul-V\u00e9lez, Sandra Pamp\u00edn-Su\u00e1rez and Jos\u00e9&nbsp; Luis Arce-Diego<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> Biological tissue identification in real clinical scenarios is a relevant and unsolved medical problem, particularly in the operating room. Although it could be thought that healthy tissue identification is an immediate task, in practice there are several clinical situations that greatly impede this process. For instance, it could be challenging in open surgery in complex areas, such as the neck, where di_erent structures are quite close together, with bleeding and other artifacts a_ecting visual inspection. Solving this issue requires, on one hand, a high contrast noninvasive technique and, on the other hand, powerful classification algorithms. Regarding the technique, optical di_use reflectance spectroscopy has demonstrated such capabilities in the discrimination of tumoral and healthy biological tissues. The complex signals obtained, in the form of spectra, need to be adequately computed in order to extract relevant information for discrimination. As usual, accurate discrimination relies on massive &nbsp;easurements, some of which serve as training sets for the classification algorithms. In this<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">work, di_use reflectance spectroscopy is proposed, implemented, and tested as a potential technique for healthy tissue discrimination. A specific setup is built and spectral measurements on several ex vivo porcine tissues are obtained. The massive data obtained are then analyzed for classification purposes. First of all, considerations about normalization, detrending and noise are taken into account.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Dimensionality reduction and tendencies extraction are also considered. Featured spectral characteristics, principal component or linear discrimination analysis are applied, as long as classification approaches based on k-nearest neighbors (k-NN), quadratic discrimination analysis (QDA) or Na\u00efve Bayes (NB).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Relevant parameters about classification accuracy are obtained and compared, including ANOVA tests. The results show promising values of specificity and sensitivity of the technique for some classification algorithms, even over 95%, which could be relevant for clinical applications in the operating room.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Keywords:<\/strong> di_use reflectance spectroscopy; biological tissues; tissue classification; multiple classification<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> Entropy, 22, 736<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Doi<\/strong>:10.3390\/e22070736<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Exciton and Mn2+ emissions in CsPbCl3: Mn2+ at high pressure<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Autors:<\/strong> Jos\u00e9 Antonio Barreda, Jesus Gonz\u00e1lez. Rafael Valiente, Fernando Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source: <\/strong>Conference: 58th European High Pressure Research Group International Conference (EHPRG) September 2020, Universidad de La Laguna, Tenerife, Spain<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> CsPbCl3 is considered as a structural archetype for hybrid organic-inorganic lead perovskite halides: APbX3 with A: organic cation, i.e. alkylammonium; X: Cl, Br, I [1-5]. Their enhanced optoelectronic and photovoltaic properties and the difficulty to establish structural correlations in these compouns make it the study of simple perovskites necessary. In addition, these compounds exhibit a rich structural phase-transition sequence in both inorganic and hybrid organic-inorganic perovskites that in the latter case are more complex as they are related to rotation and tioltiltinb of PbX6 octahedra induced by reorientational ordering associated with the organic cations. This structural variety becomes more intricated in nanoparticles [6-8]. Here, we present a structural correlation study in CsPbCl3: Mn2+ through the study of the band gap and the excitonic emission and Mn2+-related extrinsic emission as a function of pressure and temperature. In addition, we analyze the Raman spectrum as a structural probe and phonon study. We use single crystal of CsPbCl3: Mn2+ (1 mol%) grown by Bridgman (Orthorhombic, space group Pbm) [9]. The doping with Mn2+ acts as structure stabilizer and provides orange-red photoluminescence (PL) induced either through energy transfer from Pb2+ (band gap excitation) or by direct excitation into the Mn2+ excited states [6-8]. This characteristic makes it to exhibit both red and blue PL, the relative intensity of which can be tuned by means of different structural parameters: NC size, Mn concentration, temperature, pressure, etc. The investigation focuses on the energy variations of the band gap (Eg = 2.90 eV), exciton emission (2.83 eV) and Mn2+ PL (2.14 eV) as a function of pressure and temperature aiming to correlate those shifts with the corresponding variations of crystal volume, i.e. Pb-Cl bond distance, hence how it affects temperature energy shifts. Also, how these structural effects influence the relative exciton-to-impurity PL is the main objective of this work. The results are compared with previous high-pressure studies reported elsewhere [6-9]. Figure1: Absorption spectrum (blue) and time-resolved photoluminescence spectrum (red) of CsPbCl3: Mn2+ under excitation at 395 nm (200 kHz). The inset shows the intensity time dependence I(t) along the Mn2+ PL band.<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Plasmonic Sensing of Refractive Index and Density in Methanol-Ethanol Mixtures at High Pressure<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Autors:<\/strong> Camino Martin-Sanchez, Ana Sanchez-Iglesias, Paul Mulvaney, Luis M Liz-Marzan, Fernando Rodriguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> JOURNAL OF PHYSICAL CHEMISTRY C<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI:<\/strong> <a href=\"https:\/\/www.doi.org\/10.1021\/acs.jpcc.0c01419\">10.1021\/acs.jpcc.0c01419<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract: <\/strong>The localized surface plasmon resonance (LSPR) of gold nanospheres dispersed in methanol-ethanol 4:1 was measured as a function of pressure up to 60 GPa. The LSPR exhibits an intense red-shift with pressure in the range of 0-10 GPa, followed by a slower blue-shift at higher pressures. This is because an increase in the solvent refractive index with pressure leads to a red-shift of the LSPR peak wavelength while an increase in the electron density of the gold nanospheres with pressure leads to a blue-shift. Solvent solidification at 10 GPa and associated nonhydrostatic effects have a negligible influence on the LSPR shifts in the case of nanospheres. Here we show that both the LSPR shifts and changes in the nanospheres absorption coefficient can be explained on the basis of Gans&#8217; model, and this enables the solvent refractive index and the density of the solvent to be determined across the hydrostatic pressure range from 0 to 60 GPa. Interestingly, plasmonic sensing shows no evidence of crystallization or glass phase transitions in MeOH-EtOH 4:1 within the explored pressure range.<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Modelado de la propagaci\u00f3n \u00f3ptica a trav\u00e9s de tejidos biol\u00f3gicos anisotr\u00f3picos utilizando las funciones de Green<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Autors:<\/strong> Ganoza Quintana, Jos\u00e9 Luis; Fanjul V\u00e9lez, F\u00e9lix; Arce Diego, Jos\u00e9 Luis;<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> XXXVIII Congreso Anual de la Sociedad Espa\u00f1ola de Ingenier\u00eda Biom\u00e9dica (CASEIB)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract: <\/strong>Los tejidos biol\u00f3gicos son medios turbulentos debido a que las c\u00e9lulas que los componen tienen una gran cantidad de org\u00e1nulos, tales como las mitocondrias, los ribosomas, el citoplasma, etc. Todas estas estructuras tienen diferentes \u00edndices de refracci\u00f3n, por tanto, estos org\u00e1nulos act\u00faan como esparcidores en la propagaci\u00f3n de un haz \u00f3ptico incidente en un tejido biol\u00f3gico. La influencia de una distribuci\u00f3n particular de esparcidores puede ser analizada por las funciones de Green. En este trabajo se introduce un par\u00e1metro de anisotrop\u00eda geom\u00e9trica en el espectro de potencia del tejido biol\u00f3gico y se estudian sus efectos sobre las estad\u00edsticas de los haces \u00f3pticos que se propagan por el mismo. Adem\u00e1s de los efectos de otros par\u00e1metros, como la variaci\u00f3n del \u00edndice de refracci\u00f3n, la pendiente del espectro de potencia y las escalas internas \/ externas del tejido. Tambi\u00e9n se presentan algunas t\u00e9cnicas de obtenci\u00f3n de estos par\u00e1metros biol\u00f3gicos que influyen en el modelo matem\u00e1tico de la propagaci\u00f3n de la luz. ; Este trabajo ha sido parcialmente financiado por el proyecto del Plan Nacional de I+D+i \u201cModificaci\u00f3n mediante alta presi\u00f3n de las propiedades plasm\u00f3nicas y luminiscentes de nanopart\u00edculas de metales y \u00f3xidos desnudas y recubiertas\u201d (PGC2018-101464-B-I00), del Ministerio de Ciencia, Innovaci\u00f3n y Universidades, cofinanciado con fondos FEDER y por la Fundaci\u00f3n San C\u00e1ndido<\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">In vivo animal image-guided surgery by fluorescence imaging applied to nerve<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Autors:<\/strong> F. Fanjul-V\u00e9lez, A. M. D\u00edaz-Mart\u00ednez, E. Garro-Mart\u00ednez, and J. L. Arce-Diego<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> OSA Technical Digest (Optical Society of America, 2019),<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract: <\/strong>Biological tissues identification is of utmost relevance in guided surgery. Nerve contrast is particularly critical, as undesired damage could cause severe collateral effects on patients. Fluorescence imaging could contribute to this aim.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI<\/strong>: <a href=\"https:\/\/doi.org\/10.1364\/FIO.2019.FTu1F.2\">https:\/\/doi.org\/10.1364\/FIO.2019.FTu1F.2<\/a><\/p>\n<\/div><\/details><\/div>\n\n\n\n<div class=\"wp-block-genesis-blocks-gb-accordion gb-block-accordion\"><details><summary class=\"gb-accordion-title\">Upconversion and Optical Nanothermometry in LaGdO3: Er3+ Nanocrystals in the RT-900 K Range dependence of electronic structures<\/summary><div class=\"gb-accordion-text\">\n<p class=\"wp-block-paragraph\"><strong>Author(s):<\/strong> V. Guti\u00e9rrez-Cano, F. Rodr\u00edguez, J. A. Gonz\u00e1lez, and R. Valiente<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Source:<\/strong> <em>PapThe Journal of Physical Chemistry C<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Volume:<\/strong> 123 (49)&nbsp;&nbsp;&nbsp; <strong>P\u00e1ginas:<\/strong> 29818-29828<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Abstract:<\/strong> The search of material hosts being able to incorporate Er<sup>3+<\/sup> impurities with a thermally stable structure and high melting temperature is priority in optical thermometry. In this work, we report on the structural and spectroscopic characterization of Er<sup>3+<\/sup>\u2013doped and Yb<sup>3+<\/sup>\/Er<sup>3+<\/sup>\u2013co-doped LaGdO<sub>3<\/sub> nanocrystals synthesized via the sol-gel Pechini method. X-ray diffraction (XRD) and Raman spectroscopy unequivocally show that the synthesis method provides nanocrystals with a single-phase B-type monoclinic structure (space group: C2\/m). Intensity decay curves I(t) were measured to investigate the efficiency of upconversion processes yielding green emission. We showed that an energy transfer upconversion (ETU) process involving Yb\u2013Er pairs governs visible emission upon NIR excitation. The temperature dependence of the thermalized green luminescence at 525 nm (<sup>2<\/sup>H11\/2\u2192<sup>4<\/sup>I<sub>15\/2<\/sub>) and 549 nm (<sup>4<\/sup>S<sub>3\/2<\/sub>\u2192<sup>4<\/sup>I<sub>15\/2<\/sub>) was checked for thermometric applications in the RT\u2013900 K temperature range. We demonstrate that the B-type monoclinic phase of LaGdO<sub>3<\/sub> is stable from low temperature up to 900 K. Doped with Er<sup>3+<\/sup>, it shows suitable thermometer capabilities with a maximum sensitivity of S = 4.3\u00b710<sup>\u22123<\/sup> K<sup>\u22121<\/sup> at 554 K, and a relative sensitivity decreasing from its maximum value at 0 K to S<sub>R<\/sub> = 1.2 \u00b7 10<sup>\u22122<\/sup> K<sup>\u22121<\/sup> at 298 K. The results suggest that LaGdO<sub>3<\/sub> in its B-type monoclinic phase is a promising material as a wide-range temperature sensor, without any further surface protection.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>KeyWords Plus:<\/strong> Luminescence, Power, Materials, Lasers, Ions<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>&nbsp;DOI:<\/strong> <a href=\"https:\/\/doi.org\/10.1021\/acs.jpcc.9b06959\">http:\/\/dx.doi.org\/10.4279\/PIP.110004<\/a><\/p>\n<\/div><\/details><\/div>\n<\/div><\/details><\/div>\n\n\n\n<figure class=\"wp-block-image size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"261\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/micin-uefeder-aei-1024x261.jpg\" alt=\"\" class=\"wp-image-589\" style=\"width:512px;height:131px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/micin-uefeder-aei-1024x261.jpg 1024w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/micin-uefeder-aei-300x76.jpg 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/micin-uefeder-aei-768x196.jpg 768w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/micin-uefeder-aei-1536x392.jpg 1536w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/micin-uefeder-aei-600x153.jpg 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/micin-uefeder-aei.jpg 1808w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>NANOPART\u00cdCULAS MULTIFUNCIONALES PARA TRATAMIENTO DE C\u00c1NCER DE CABEZA\/CUELLO MEDIANTE HIPERTERMIA FOTOINDUCIDA<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">IDIVAL<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">07\/12\/2018 \u2013 07\/12\/2020&nbsp;&nbsp;&nbsp;&nbsp; Budget: 8.000 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: R. Valiente<\/p>\n\n\n\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"387\" height=\"130\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/IDIVAL.png\" alt=\"\" class=\"wp-image-485\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/IDIVAL.png 387w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/IDIVAL-300x101.png 300w\" sizes=\"auto, (max-width: 387px) 100vw, 387px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>NCLAS: NANOCRYSTALS IN FIBRE LASERS <\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">H2020-FETOPEN- 2018-01-829161<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">EU Commission<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2019 \u2013 31\/12\/2022&nbsp;&nbsp;&nbsp; UC Budget: 579.020\u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: R. Valiente<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-17-1024x704.png\" alt=\"Esta imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es imagen-17-1024x704.png\" style=\"width:335px;height:231px\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>EQUIPAMIENTO DE ESPECTROMETR\u00cdA DE FLUORESCENCIA DE RAYOS X EN LOS SERVICIOS CIENMODIFICACION MEDIANTE ALTA PRESION DE LAS PROPIEDADES PLASMONICAS Y LUMINISCENTES DE NANOPARTICULAS DE METALES Y OXIDOS DESNUDAS Y RECUBIERTAS<\/strong> <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">MINISTERIO CIENCIA, INNOVACI\u00d3N Y UNIVERSIDADES<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2019-31\/12\/2022&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Budget: &nbsp;96.800 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img decoding=\"async\" src=\"https:\/\/upload.wikimedia.org\/wikipedia\/commons\/thumb\/a\/ad\/Logotipo_del_Ministerio_de_Ciencia%2C_Innovaci%C3%B3n_y_Universidades.svg\/1280px-Logotipo_del_Ministerio_de_Ciencia%2C_Innovaci%C3%B3n_y_Universidades.svg.png\" alt=\"Resultado de imagen de MINISTERIO DE CIENCIA, INNOVACION Y UNIVERSIDADES\" style=\"width:320px;height:83px\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>LARGE VOLUME DIAMOND ANVIL CELLS FOR RESEARCH UNDER EXTREME CONDITIONS (B19).<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Collaborative Research at Premier Research Institute for Ultrahigh-pressure Sciences (PRIUS).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Geodynamics Research Center, Ehime Institute (Japan).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Institutions involved: UNIVERSIDAD DE CANTABRIA, ICMA and PRIUS<\/p>\n\n\n\n<hr class=\"wp-block-separator has-css-opacity\"\/>\n\n\n\n<p class=\"wp-block-paragraph\">&nbsp;PI: F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/04\/2016 \u2013 31\/03\/2017 \/\/ 01\/04\/2017 \u2013 31\/03\/2018 \/\/01\/04\/2018 \u2013 31\/03\/2019 \/\/ 01\/04\/2019 \u2013 31\/03\/2020&nbsp; (prorrogable)<\/p>\n\n\n\n<figure class=\"wp-block-image size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"257\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/LOGO_prius-1024x257.png\" alt=\"\" class=\"wp-image-501\" style=\"width:256px;height:64px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/LOGO_prius-1024x257.png 1024w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/LOGO_prius-300x75.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/LOGO_prius-768x193.png 768w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/LOGO_prius-1536x385.png 1536w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/LOGO_prius-2048x514.png 2048w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/LOGO_prius-600x151.png 600w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>MEJORA DE LA CONDUCTIVIDAD T\u00c9RMICA EN CAPAS CONDUCTORAS DE GO DEPOSITADAS SOBRE L\u00c1MINAS DE ACERO INOXIDABLE DE BSH<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Collaborative action Univ. Cantabria (High Pressure and Spectroscopy Group)&nbsp; \u2013 BSH (Electrodom\u00e9sticos Espa\u00f1a, S.A))<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">15\/11\/2019-15\/08\/2020&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; UC Budget: 27.830 \u20ac <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-20.png\" alt=\"Esta imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es imagen-20.png\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>EQUIPAMIENTO DE ESPECTROMETR\u00cdA DE FLUORESCENCIA DE RAYOS X EN LOS SERVICIOS CIENT\u00cdFICO-T\u00c9CNICOS DE INVESTIGACI\u00d3N DE LA UC<\/strong> <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Scientific infrastructure project) EQC2018-004430-P<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">&nbsp;MINISTERIO\nDE CIENCIA, INNOVACION Y UNIVERSIDADES <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2018 &#8211; 31\/12\/2019.&nbsp;&nbsp;&nbsp;&nbsp; Budget: 156.216,50 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img decoding=\"async\" src=\"https:\/\/upload.wikimedia.org\/wikipedia\/commons\/thumb\/a\/ad\/Logotipo_del_Ministerio_de_Ciencia%2C_Innovaci%C3%B3n_y_Universidades.svg\/1280px-Logotipo_del_Ministerio_de_Ciencia%2C_Innovaci%C3%B3n_y_Universidades.svg.png\" alt=\"Resultado de imagen de MINISTERIO DE CIENCIA, INNOVACION Y UNIVERSIDADES\" style=\"width:373px;height:97px\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>AN\u00c1LISIS NO DESTRUCTIVO DE LA FRAGMENTACI\u00d3N DE VIDRIOS TEMPLADOS DE ENCIMERAS DE GAS MEDIANTE LUZ POLARIZADA<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Collaborative action Univ. Cantabria (High Pressure and Spectroscopy Group)&nbsp; \u2013 BSH)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">03\/06\/2019-03\/03\/2020<strong>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; <\/strong>UC Budget: 29.863 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-20.png\" alt=\"Esta imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es imagen-20.png\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><em><strong>MATERIA A ALTA PRESI\u00d3N<\/strong><\/em><strong>, MATTER AT HIGH PRESSURE \u201cMALTA\u201d&nbsp; )<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">CSD2007-00045<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">INGENIO-CONSOLIDER Program, Spanish Government for supporting Groups of Excellence<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/12\/2007 \u2013 31\/12\/2014&nbsp;(Project extended up to 2019)&nbsp;&nbsp; UC Budget: 883.389\u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"200\" height=\"101\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2021\/10\/MALTA_web_v4.png\" alt=\"\" class=\"wp-image-585\"\/><\/figure>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-2.png\" alt=\"\" class=\"wp-image-225\" style=\"width:434px;height:116px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-2.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-2-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>NUEVAS FASES ACTIVAS EN NANO-OXIDOS DE METALES DE TRANSICION Y TIERRAS RARAS ESTABILIZADAS A ALTA PRESION<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">MAT2015-69508-P<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">MINECO\/FEDER, UE<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2016 &#8211; 31\/07\/2019.&nbsp; &nbsp;&nbsp;&nbsp;Budget: 106.722 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"640\" height=\"319\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-23.png\" alt=\"\" class=\"wp-image-251\" style=\"width:321px;height:160px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-23.png 640w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-23-600x299.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-23-300x150.png 300w\" sizes=\"auto, (max-width: 640px) 100vw, 640px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>CARACTERIZACI\u00d3N DE MUESTRAS BASADAS EN TiO2 EN POLVO O EN CAPA VITRIFICADA SOBRE L\u00c1MINAS DE ACERO Y OPTIMIZACI\u00d3N DE LAS PROPIEDADES FOTOCATAL\u00cdTICAS MEDIANTE MODIFICACI\u00d3N DE LA FUENTE DE ILUMINACI\u00d3N O DEL GAP DEL MATERIAL<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Convenio VITRISPAN\u2013UC)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">16\/04\/2018 \u2013&nbsp;15\/04\/2019. &nbsp;UC Budget: 35.870 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI:&nbsp; R. Valiente<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"http:\/\/www.vitrispan.com\/img\/logo\/logo.png\" alt=\"Resultado de imagen de Vitrispan\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>M\u00c9TODO DE CONTROL DE CALIDAD DE VIDRIOS DE CER\u00c1MICOS, VIDRIOS TEMPLADOS Y MATERIALES CER\u00c1MICOS POR ESPECTROSCOPIA RAMAN PARA ELECTRODOM\u00c9STICOS <\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Collaborative action Univ. Cantabria (High Pressure and Spectroscopy Group) \u2013 BSH)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/11\/2014 \u2013 02\/09\/2019 UC Budget: 188.135 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI:&nbsp; R. Valiente<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-20.png\" alt=\"Esta imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es imagen-20.png\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>NUEVOS M\u00c9TODOS DE CONTROL DE CALIDAD DE VIDRIOS DE CER\u00c1MICOS, VIDRIOS TEMPLADOS Y MATERIALES CER\u00c1MICOS POR ESPECTROSCOPIA RAMAN PARA ELECTRODOM\u00c9STICOS.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Collaborative action Univ. Cantabria (High Pressure and Spectroscopy Group)&nbsp; \u2013 BSH)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/11\/2015 \u2013 31\/10\/2017&nbsp;&nbsp;&nbsp; UC Budget: 48.400 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-20.png\" alt=\"Esta imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es imagen-20.png\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>OLEDS Infrarrojos basados en tierras raras<\/strong>  <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">MINECO, Spanish Ministry of Economy Universidad de Cantabria<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">2015-2018, UC Budget: 60.000 \u20ac&nbsp;&nbsp; <\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-18.png\" alt=\"Esta imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es imagen-18.png\" style=\"width:361px;height:96px\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>M\u00c9TODO DE CONTROL DE CALIDAD DE VIDRIOS DE CER\u00c1MICOS, VIDRIOS TEMPLADOS Y MATERIALES CER\u00c1MICOS POR ESPECTROSCOPIA RAMAN PARA ELECTRODOM\u00c9STICOS<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Collaborative action. BSH &#8211; U. Cantabria)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">15\/12\/2016-14\/12\/2018 &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;UC Budget: 169.400 \u20ac <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-20.png\" alt=\"Esta imagen tiene un atributo ALT vac\u00edo; su nombre de archivo es imagen-20.png\"\/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>MATERIALS CHARACTERIZATION BY SPECROSCOPIC TECHNIQUES<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Scientific service in\nsupport to industry)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">&nbsp;24\/3\/2015-31\/12\/2018&nbsp;&nbsp; Income: 25.029,79 \u20ac <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>MEJORA DE LA CALIDAD FINAL DE NUEVOS RECUBRIMIENTOS EN PIEZAS DE FUNDICI\u00d3N DE HIERRO MEDIANTE INVESTIGACI\u00d3N SOBRE LA EVOLUCI\u00d3N DE LA CORROSI\u00d3N EN PIEZAS CINCADAS<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Colabborative project CHASSIS BRAKES INTL. SPAIN &#8211;\nUC)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/06\/2015 \u2013 31\/05\/2016&nbsp;&nbsp;&nbsp; UC Budget: 5.915,77 \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"411\" height=\"123\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/image.png\" alt=\"\" class=\"wp-image-250\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/image.png 411w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/image-300x90.png 300w\" sizes=\"auto, (max-width: 411px) 100vw, 411px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>LA ESPECTROSCOPIA RAMAN INFRARROJA COMO SONDA NO DESTRUCTIVA DE CARACTERIZACI\u00d3N ESTRUCTURAL EN TECNOLOG\u00cdA DE NUEVOS MATERIALES<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Universidad de Cantabria- SODERCAN) JS06<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/06\/2015 Duraci\u00f3n del proyecto: 1 a\u00f1o &#8211; 1 d\u00eda. Budget: 30.000\u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"935\" height=\"137\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22.png\" alt=\"\" class=\"wp-image-245\" style=\"width:532px;height:76px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22.png 935w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22-600x88.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22-300x44.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-22-768x113.png 768w\" sizes=\"auto, (max-width: 935px) 100vw, 935px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>CELDAS DE GRAN VOLUMEN PARA EL ESTUDIO DE MATERIALES EN CONDICIONES EXTREMAS DE ALTA PRESI\u00d3N, CAMPO MAGN\u00c9TICO Y TEMPERATURA (UCelda)<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(Universidad de Cantabria- Cryovac)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">24\/02\/2015 \u2013 31\/12\/2017&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Budget: 152.156&nbsp; \u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">RTC-2015-4304-3<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"138\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-21-1024x138.png\" alt=\"\" class=\"wp-image-244\" style=\"width:594px;height:80px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-21-1024x138.png 1024w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-21-600x81.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-21-300x40.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-21-768x103.png 768w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-21.png 1040w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>FUENTE SUPER-CONTINUA DE ALTA LUMINOSIDAD PARA APLICACI\u00d3N EN NANOMATERIALES Y BIOTECNOLOG\u00cdA<\/strong><br> UCAN10-4E-489   (01\/01\/2010 al 02\/01\/2016)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2010 &#8211; 31\/12\/2014&nbsp;&nbsp; UC Budget: 63.658\u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-18.png\" alt=\"\" class=\"wp-image-241\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-18.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-18-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>CHROMOPHORE- SENSITIZED UP -CONVERSION IN LANTHANIDE MATERIALS<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">FP7-PEOPLE-2011-CIG-303535 (01\/09\/2012 al 01\/09\/2016)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">\n\n\n\n\n\n\n\n\n\nMembrete\n\n\n\n\n\n\n\n\nUC Budget: 100.000\u20ac\n\n\n\n<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"704\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-17-1024x704.png\" alt=\"\" class=\"wp-image-240\" style=\"width:270px;height:185px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-17.png 1024w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-17-600x413.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-17-300x206.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-17-768x528.png 768w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>ESTUDIO DE LAS PROPIEDADES \u00d3PTICAS Y MAGN\u00c9TICAS DE ZnO IMPURIFICADO CON METALES DE TRANSICIONES Y SUS APLICACIONES EN BIOMEDICINA<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">MAT2012-38664-C02-01 (1-1-2010 al 02-01-2016)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">01\/01\/2012 &#8211; 02\/01\/2015&nbsp;&nbsp; Budget: 81.900\u20ac<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-16.png\" alt=\"\" class=\"wp-image-239\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-16.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-16-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>NUEVOS VIDRIOS FOTOACTIVOS DE ALTA TRANSMITANCIA PARA APLICACIONES FOTOVOLTAICAS<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">IPT-2011-1868-920000 SAINT GOBAIN (AVILES R &amp; D CENTRE)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">04\/05\/2011 &#8211; 30\/04\/2014&nbsp;&nbsp;&nbsp; UC Budget: 199.000\u20ac<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(2011-2013)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"733\" height=\"114\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-15.png\" alt=\"\" class=\"wp-image-238\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-15.png 733w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-15-600x93.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-15-300x47.png 300w\" sizes=\"auto, (max-width: 733px) 100vw, 733px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>ESTUDIO DE LAS PROPIEDADES \u00d3PTICAS Y MAGN\u00c9TICAS DEL ZnO IMPURIFICADO CON METALES DE TRANSICI\u00d3N Y SUS APLICACIONES EN BIOMEDICINA<\/strong> (1-1-2013 al 31-12-2015)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-14.png\" alt=\"\" class=\"wp-image-237\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-14.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-14-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>CONCEPCI\u00d3N DE CELDAS DE DIFRACCI\u00d3N DE NEUTRONES EN ALTAS PRESIONES\nCON GRAN VOLUMEN DE MUESTRA<\/strong><strong>\ufeff<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Financiado por CDTI(numero de expediente: IDC-20101166) Entidades participantes:Cryovac <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"625\" height=\"137\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-13.png\" alt=\"\" class=\"wp-image-236\" style=\"width:417px;height:91px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-13.png 625w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-13-600x132.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-13-300x66.png 300w\" sizes=\"auto, (max-width: 625px) 100vw, 625px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>CARACTERIZACI\u00d3N MICROESTRUCTURAL DE TUBOS DE FUNDICI\u00d3N D\u00daCTIL MEDIANTE ESPECTROSCOPIA RAMAN<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Financiado por SODERCAN Entidades participantes:Saint Gobain PAM<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"762\" height=\"140\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-11.png\" alt=\"\" class=\"wp-image-234\" style=\"width:421px;height:76px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-11.png 762w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-11-600x110.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-11-300x55.png 300w\" sizes=\"auto, (max-width: 762px) 100vw, 762px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>OPTIMIZACI\u00d3N DEL PROCESO DE COLADA Y MEJORA DE LA CALIDAD FINAL DE LOS COMPONENTES MEDIANTE LA T\u00c9CNICA DE AN\u00c1LISIS T\u00c9RMICO<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Financiado por SODERCAN Entidades participantes:Nissan Motor Iberica, S.A<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"368\" height=\"90\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-10.png\" alt=\"\" class=\"wp-image-233\" style=\"width:428px;height:105px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-10.png 368w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-10-300x73.png 300w\" sizes=\"auto, (max-width: 368px) 100vw, 368px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>ENSAYOS RELATIVOS A PROPIEDADES T\u00c9RMICAS DE MATERIALES DE CONSTRUCCI\u00d3N <\/strong><\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1000\" height=\"312\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-7.png\" alt=\"\" class=\"wp-image-230\" style=\"width:412px;height:128px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-7.png 1000w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-7-600x187.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-7-300x94.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-7-768x240.png 768w\" sizes=\"auto, (max-width: 1000px) 100vw, 1000px\" \/><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\">(2010) Financiado por SODERCAN Entidades participantes:TECNALIA<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">PI: F. Rodr\u00edguez<\/p>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>ESTUDIO DE LAS PROPIEDADES \u00d3PTICAS Y MAGN\u00c9TICAS DE ZNO IMPURIFICADO CON METALES DE TRANSICIONES EN DIFERENTES CONFORMACIONES ESTRUCTURALES<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">(MAT2011-28868-C02-01 (1-1-2012 al 31-12-2012)A<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-6.png\" alt=\"\" class=\"wp-image-229\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-6.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-6-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>ESPECTR\u00d3METRO PARA TIEMPOS DE VIDA DE FLUORESCENCIAS Y ESTADO ESTACIONARIO (2010)<\/strong><\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-5.png\" alt=\"\" class=\"wp-image-228\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-5.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-5-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>ANALISIS DE NANOCOMPUESTOS POLIMERICOS MEDIANTE ESPECTROSCOPIA RAMAN. NANOCIT (2009) <\/strong><\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"248\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-4-1024x248.png\" alt=\"\" class=\"wp-image-227\" style=\"width:430px;height:104px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-4-1024x248.png 1024w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-4-600x146.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-4-300x73.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-4-768x186.png 768w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>PROPIEDADES OPTICAS Y MAGNETICAS DE IONES DE TRANSICION EN OXIDOS SOMETIDOS A ALTAS PRESIONES: CORRELACIONES ESTRUCTURALES (2009)<\/strong><\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-3.png\" alt=\"\" class=\"wp-image-226\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-3.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-3-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DESARROLLO DE NUEVOS MATERIALES LUMINISCENTES PARA CELULAS FOTOVOLTAICAS DE MAYOR EFICIENCIA (2007)<\/strong><\/p>\n\n\n\n<figure class=\"wp-block-image is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"794\" height=\"229\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-1.png\" alt=\"\" class=\"wp-image-224\" style=\"width:434px;height:125px\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-1.png 794w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-1-600x173.png 600w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-1-300x87.png 300w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-1-768x222.png 768w\" sizes=\"auto, (max-width: 794px) 100vw, 794px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>NUEVOS FENOMENOS LUMINISCENTES INDUCIDOS POR CAMBIOS ESTRUCTURALES A ALTAS PRESIONES (2005)<\/strong><\/p>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"434\" height=\"116\" src=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen.png\" alt=\"\" class=\"wp-image-223\" srcset=\"https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen.png 434w, https:\/\/grupos.unican.es\/apye\/wp-content\/uploads\/2019\/03\/imagen-300x80.png 300w\" sizes=\"auto, (max-width: 434px) 100vw, 434px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-css-opacity has-background\" style=\"background-color:#10a7e8;color:#10a7e8\"\/>\n","protected":false},"excerpt":{"rendered":"<p>PLATAFORMA TECNOL\u00d3GICA MULTIUSO PARA EL ESTUDIO DE PINTURAS, RESTOS \u00d3SEOS Y \u00daTILES PREHIST\u00d3RICOS POR MEDIO DE MICRO-ESPECTROSCOPIA RAMAN PORT\u00c1TIL.PROYECTOS PROYECTOS DE I+D CONVOCATORIA 2021 SODERCAN Gobierno de Cantabria Budget: 20000 \u20ac PI1: F. Rodr\u00edguez MEMORIA FINAL DE PROYECTO (ver memoria) FOTOLUMINISCENCIA AMPLIFICADA POR PLASMONES SUPERFICALES EN NANOMATERIALES DOPADOS CON LANTANIDOS [&hellip;]<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-222","page","type-page","status-publish","hentry"],"featured_image_src":null,"featured_image_src_square":null,"_links":{"self":[{"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/pages\/222","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/comments?post=222"}],"version-history":[{"count":34,"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/pages\/222\/revisions"}],"predecessor-version":[{"id":742,"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/pages\/222\/revisions\/742"}],"wp:attachment":[{"href":"https:\/\/grupos.unican.es\/apye\/wp-json\/wp\/v2\/media?parent=222"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}