BUSCADOR RECOLECTA

11 pages. -- Materials and methods: 1.1 Molecular weight determined by gel permeation chromatography. -- 1.2 Film bursting tests by monitoring pressure given on the GMTA film. -- 1.3 An in vitro degradation profile of GMTA films in fetal bovine serum. -- 1.4 Cytotoxicity tests by agar diffusion methods. -- 1.5 Subcutaneous implantation and histology staining. -- Figures S1-S7. -- Movie S1. TA spray curing on an uncured GM film showing enhanced interfacial adhesion on a freshly prepared porcine heart., Peer reviewed

Supplementary Figure 1. TP antibody specificity and affinity. a.-- Supplementary Figure 2. a, Proliferation capability of OSCAR T cells upon rechallenge with OHS cell line.-- Supplementary Figure 3. In vitro effector function of OSCAR -1 and OSCAR -3 T cells towards LM7 OS cells. a.-- Supplementary Figure 4. In vivo effector function of OSCAR-1 and OSCAR-3 T cells in lung metastatic mouse models. a.-- Supplementary Figure. 5 Staining of target cells in figure 5b with anti ALPL, TP-1 and TP-3 antibodies. Isotype and secondary antibody controls (grey).-- Supplementary methods., Peer reviewed

Table S1. Daily dust optical depth at 532 nm (DOD532) for fine dust (Df), coarse dust (Dc) and total dust (DD) along the particular dust periods for the five Iberian lidar stations (ARN, GRA, EVO, TRJ and BCN). The standard deviation values are in brackets. The Df-to-total dust DOD ratio (ftr_DOD) is also included. Table S2. Daily mass loading (𝑀2, in mg m-2) for fine dust (Df), coarse dust (Dc) and total dust (DD) along the particular dust periods for the five Iberian lidar stations (ARN, GRA, EVO, TRJ and BCN). The standard deviation values are in brackets. The Df-to-total dust mass ratio (𝑓𝑡𝑟_𝑀DD) is also included. Figure S1. Percent of HYSPLIT 5-day back-trajectories originated in the Sahara desert area and arrived at each station (from NE to SW, by decreasing latitude): (a) Barcelona (BCN), (b) Torrejón/Madrid (TRJ), (c) Évora (EVO), (d) Granada (GRA) and (e) El Arenosillo/Huelva (ARN). Figure S2. Temporal evolution of the dust outbreak by crossing the Iberian Peninsula in springtime 2021 in terms of the hourly fine dust CoM height (𝑍Df com), blue circles), and their daily values (white squares), for the five Iberian lidar stations as latitude decreases (from up to down panels): (a) BCN, (b) TRJ, (c) EVO, (d) GRA and (e) ARN. Figure S3. The same as Fig. S2, but for the coarse dust CoM height (𝑍Df com). Hourly and daily values are shown by red circles and white squares, respectively., Peer reviewed

46 pages. -- S1. Materials and methods. -- S1.1 Materials and characterization. -- S1.2 Crystallography. -- S1.3. Synthetic procedures. -- S2. Characterization of organic linkers. -- S3. Characterization of Rh2(bdc)4 complexes. -- S4. Characterization of HET-MOP-1. -- S5. Characterization of HET-MOP-2. -- S6. Characterization of HET-MOP-3, Peer reviewed

We include the dataset corresponding to the figures of the paper "Nonlinear Optical Response of a Plasmonic Nanoantenna to Circularly Polarized Light: Rotation of Multipolar Charge Density and Near-Field Spin Angular Momentum Inversion" by M. Quijada, A. Babaze, J. Aizpurua, and A.G. Borisov, published in the journal ACS Photonics, with DOI: 10.1021/acsphotonics.3c00783 . The set includes data to generate: optical spectra, charge density maps, time evolution of multipolar moments, and all the plots in the paper., Peer reviewed

Supporting information: Figures S1–S8: Animations showing average ΔTEC variations (in σ units—semi-transparent colour scale) for the studied locations for each of the analysed storms. Figure S1—January 2015, S2—March 2015, S3—June 2015, S4—May 2017, S5—September 2017, S6—August 2018, S7—November 2021, S8—November 2022. Non-transparent grey—no data., Peer reviewed

120 pages. -- SA. Synthesis of Au NPs using ROH. -- SB. Experimental section. -- SC. Effect of mono-alcohol, mono-alcohol content and cation. -- SD. Effect of experimental parameters: HAuCl4 concentration, volume of solution, type of container used, light. -- SE. Effect of the nature of the alcohols. -- SF. Kinetics of the reduction. -- SG. Influence of the temperature. -- SH. Influence of base concentration. -- SI. Influence of gas atmosphere. -- SJ. Influence of the order of addition of the chemicals. -- SK. Discussion of Au NP formation. -- SL. Reproducibility. -- SM. Scalability. -- SN. Mixture of mono-alcohols. -- SO. Cation and surfactant effects . -- SP. Electrochemical characterization of Au NPs. -- SQ. Supported NPs. -- SR. Pd and bimetallic NPs. -- SS. Nanocomposites. -- ST. Electrochemical characterization of AuxPdy NPs and [x Au + y Pd] nanocomposites. -- SU. Outlook into multi-metallic nanomaterials. -- SV. Comparison of different catalysts. -- SW. References, Gold nanoparticles (Au NPs) and gold-based nanomaterials combine unique properties relevant for medicine, imaging, optics, sensing, catalysis, and energy conversion. While the Turkevich–Frens and Brust–Schiffrin methods remain the state-of-the-art colloidal syntheses of Au NPs, there is a need for more sustainable and tractable synthetic strategies leading to new model systems. In particular, stabilizers are almost systematically used in colloidal syntheses, but they can be detrimental for fundamental and applied studies. Here, a surfactant-free synthesis of size-controlled colloidal Au NPs stable for months is achieved by the simple reduction of HAuCl4 at room temperature in alkaline solutions of low-viscosity mono-alcohols such as ethanol or methanol and water, without the need for any other additives. Palladium (Pd) and bimetallic AuxPdy NPs, nanocomposites and multimetallic samples, are also obtained and are readily active (electro)­catalysts. The multiple benefits over the state-of-the-art syntheses that this simple synthesis bears for fundamental and applied research are highlighted., Peer reviewed

Germination data of sterilized and non-sterilized oak (Quercus ilex) seeds on sterilized and non-sterilized oak and pine soils, added with microbial extracts from oak and pine soils, plus a control of distilled water., Junta de Andalucía Regional Government (grant PY2020-0223), Spanish Research Agency (grant MCIN/AEI 10.13039/501100011033), Peer reviewed

31 pages. -- Experimental procedures. -- Figure S1 1H NMR spectrum of 2CF3-PMABr. -- Figure S2 XRD patterns of perovskite film and 2CF3-PMABr powder. -- Figure S3 XPS spectra of Br 3d and I 3d S9. -- Figure S4 FTIR spectra of 2CF3-PMABr powder and 2CF3-PMABr/PbI2 mixture. -- Figure S5 1H NMR spectrum of mixture. -- Figure S6 TRPL measurements. -- Figure S7 Image of perovskite thickness. -- Figure S8 SCLC curves of electron-only devices. -- Figure S9 Image of ToF-SIMS depth profiles. -- Figure S10 AFM and SEM images. -- Figure S11 Absorption spectra of perovskite films. -- Figure S12 UPS spectra of perovskite films and HTL. -- Figure S13 Statistic of photovoltaic parameter small area cells. -- Figure S14 The relationship of JSC with light intensity. -- Figure S15 Absorption spectra and microscopic images of large area perovskite films. -- Figure S16 VOC, JSC and FF evolution of modules. -- Figure S17 Image of water contact angle. -- Table S1 NMR peak position and area of 2CF3-PMABr mixture with FAI or MABr. -- Table S2 NMR peak position and area of PEABr mixture with FAI or MABr. -- Table S3 TRPL fitting data of perovskite films modified with different concentration. -- Table S4 TRPL fitting data of perovskite films post-annealed at different temperature. -- Table S5 TRPL fitting data of perovskite films with different thickness. -- Table S6 Photovoltaic parameters of solar cells. -- Table S7 Fitting parameters of the EIS., Peer reviewed

14 pages. -- 1. Synthesize and characterization on Cu1.5Te NPs. -- 2. Surface treatment with SeL solution. -- 3. Characterization on consolidated pellets. -- 4. High temperature XRD and TE properties. -- 5. Stability and repeatability. -- 6. Anisotropic characterizations. -- Figures S1-S18. -- Table S1. Refined lattice parameters (from Rietveld refinement of the XRD patterns) of different crystal structures at corresponding temperatures. -- Table S2. Relative densities of Cu1.5Te, Cu1.5-xTe-OL and Cu1.5-xTe-Cu2Se pellets obtained from absolute values measured with the Archimedes’ method., Cu2–xS and Cu2–xSe have recently been reported as promising thermoelectric (TE) materials for medium-temperature applications. In contrast, Cu2–xTe, another member of the copper chalcogenide family, typically exhibits low Seebeck coefficients that limit its potential to achieve a superior thermoelectric figure of merit, zT, particularly in the low-temperature range where this material could be effective. To address this, we investigated the TE performance of Cu1.5–xTe–Cu2Se nanocomposites by consolidating surface-engineered Cu1.5Te nanocrystals. This surface engineering strategy allows for precise adjustment of Cu/Te ratios and results in a reversible phase transition at around 600 K in Cu1.5–xTe–Cu2Se nanocomposites, as systematically confirmed by in situ high-temperature X-ray diffraction combined with differential scanning calorimetry analysis. The phase transition leads to a conversion from metallic-like to semiconducting-like TE properties. Additionally, a layer of Cu2Se generated around Cu1.5–xTe nanoparticles effectively inhibits Cu1.5–xTe grain growth, minimizing thermal conductivity and decreasing hole concentration. These properties indicate that copper telluride based compounds have a promising thermoelectric potential, translated into a high dimensionless zT of 1.3 at 560 K., Peer reviewed