BUSCADOR RECOLECTA

Synthesis of molecular precursors; complementary experimental data referenced in the main paper; four sites Fermi-Hubbard model; complementary DFT calculations., Peer reviewed

Supplementary Table S1. -- 24 pages., The complete results of the analysis performed by micro-XRF on the Castellani jewels of the Museo Nazionale Etrusco di Villa Giulia in Rome are provided. The amounts of gold, silver and copper detected in foils, wires, granules and joining areas are given in weight percentage and normalized to 100. The relative errors of the quantification are 3% for gold, 7% for silver and 22% for copper. Moreover, the ratios Au(L3/M) and Au(L2/L3) for all the spots analysed in the foils, wires and granules are also reported. The results are given for each jewel. The jewels are ordered by museum number., Peer reviewed

The supplementary file includes two Tables where atomic coordinates for the crystal structures of the magnetic topological insulators MnBi2Te4n(Bi2Te3) with n=, 1, 2, 4, 5 (TABLE I) and, n=0, 3 and 6 (TABLE II) are provided., Peer reviewed

"Disruptions_dataset.xlsx" is based on published literature and contains: * a first worksheet tab specifying:1) study ID; 2) YEAR of publication; 3) REALM under study; 4) whether SDD occurred on mainland or an ISLAND, and if so, the type of island (i.e., continental vs. oceanic); 5) ECOSYSTEM under study; 6) type of anthropogenic and non-anthropogenic DRIVERS of SDD; 7) seed DISPERSER under study; 8) in the case of ABIOTIC dispersal, the main seed dispersal vector; 9) RESPONSE VARIABLES that were assessed in each publication; 10) if the study considered SDD at a species- or at community- LEVEL; 11) whether the main results were based on empirical data, simulations, or the combination of these two APPROACHES ; * a second worksheet tab with the full list of references addressed in this review paper., Review of studies on biotic and abiotic seed dispersal disruptions to ascertain the global change drivers addressed, dispersal modes impacted, plant processes affected, and spatial focus of existing research on this topic up-to-date., Peer reviewed

(i) Dielectric relaxation of neat components; (ii) dielectric α-relaxation of SBR/PS blends; (iii) derivative of the calorimetric traces of SBR/PS blends; (iv) determination of the effective interaction parameter from SANS; (v) temperature dependence of the width of concentration fluctuations., Peer reviewed

This Supplementary Material package contains the following files: - gradexp.sage: Implementation of the gradient expansion discussed in the main text, using SageMath (version 9.4). You can run it with ‘sage gradexp.sage‘ and it will print results in text notation, and LaTeX. - gradexp.tex: Source file for generating gradexp.sage, using SageTeX. Contains instructions and detailed explanations. - gradexp.pdf: PDF version of the above, with results embedded. - Makefile.gradexp: Makefile for re-generating output files., Peer reviewed

The Electronic Supporting Information contains: (1) zeta potential measurements of PLL/SDS aggregates, (2) materials and methods, (3) low-Qz compositional analysis: fitting, (4) ellipsometry data on PLL/SDS spread film dynamics, (5) BAM images, (6) full-Qz structural analysis: fitting and parameters, and (7) mid-Qz structural dynamics analysis: fitting., Peer reviewed

We included a supplemental pdf file which contains further information of the details of our calculations, our implemented mean-field Hubbard model with non-equilibrium Green's functions, and extra calculations such as the effect of the Coulomb repulsion parameter on monolayer and bilayer zigzag graphene nanoribbons, other possible (but higher in energy) spin configurations and their transport properties, etc., In this supplementary material we describe our methodology and present additional calculations that may be interesting for a deeper understanding of the reported effects. In Sec. S1 we explain the details of the calculation with the mean- eld Hubbard model (MFH). In Sec. S2 we show the effect of the Coulomb repulsion on the bands of bilayer and monolayer graphene nanoribbons, while in Sec. S3 we show the effect that the size of the scattering region has on the local magnetization of the device. Next in Sec. S4 we plot all the possible spin con gurations resulting from the possible combinations of the spin densities of the four electrodes. In Secs. S6 and S7 we show the gure of merit, where we analyze the quality of the device as a spin-beam splitter or mirror, and the spin polarization at a different electronic energy from the one shown in the main text, respectively. In Sec. S8 we compare the transport properties for different ribbon widths. In Sec. S9 we show the quality of the independent scatterers approximation compared to the exact result for a device with three crossings. In Sec. S10 we compare the spin-averaged transmission probabilities with the unpolarized case. In Sec. S11 we explore how possible distortions, such as a small twist angle or a lateral translation of the on-top ribbon with respect to the bottom one, affect the transport properties of individual crossings. In Sec. S12 we describe the used statistical sampling and analytical expression for the averaged spin-polarization shown in Fig. 4(b) of the main text. Finally, in Sec. S13 we analyze the spin-polarizing beam-splitting effect that can be found in junctions formed with other edge-polarized GNRs, such as those built with crossed bearded GNRs., Peer reviewed

Download of the data available on the publisher platform., Diffraction images of a crystal of the F-BAR domain of PSTPIP1 (residues 1-289), mutant G258A. Data were collected on a single crystal at the beamline i03 of the Diamond Light Source synchrotron (Didcot, UK) using radiation of 0.9999 Å wavelength and a PILATUS3 6M detector. The dataset consists of 2400 images (0.15 degree oscillation per image). Crystals belong to the space group P2(1)2(1)2(1) with unit cell dimensions a=48.19 Å, b=73.02 Å, c=205.25 Å. The asymmetric unit contains an homodimer of the F-BAR domain (~53% solvent content), which is the biological unit. Diffraction data was notably anisotropic. The lowest resolution limit was 2.92 Å in the direction b* and the highest limits were 1.97 Å and 2.09 in the directions a* and c*, respectively., Peer reviewed

Derivation of the stretched exponential function, leading to the expression in eq 10; fabrication of QD in PMMA thin films by spin-coating using a Model KW-4A Spin-Coater; single-particle measurement using photon correlation technique; notes about dark fraction in QDs on (i) how it is related to the fluorescence intermittency (blinking) of QDs, (ii) how it affects the PL decay kinetics, and (iii) how one can use the statistical analysis to identify the formation of a dark fraction in a QD ensemble without measurement of QY and single-particle measurements., Peer reviewed