BUSCADOR RECOLECTA

The supplemental material provides: - Computational details and parameters that are needed to reproduced the calculations. - The model system that we use. - Technical details about the two-temperature model. - Technical details about the inclusion of the chemical potential in our calculations., Peer reviewed

This PDF file includes: Figs. S1 to S10 Legends for tables S1 to S6, Other Supplementary Material includes the following: Tables S1 to S6, Peer reviewed

Additional STM topographs and spectroscopy data and further results from DFT calculations., Peer reviewed

Supplementary information files: -Dynamical Hall responses.nb -Dynamical Hall responses.pdf The derivation of some equations in the paper are provided in the Dynamical Hall responses.nb Mathematica notebook. In addition, the notebook provides the full code to generate the plots in the paper. We also provide a PDF copy of the notebook for readers without access to Mathematica software., Special Instructions The notebook has been uploaded to the Notebook Archive at [https://notebookarchive.org/2023-08-dd45k93], which allows to visualize the Mathematica notebook and running it in Wolfram Cloud (free monthly computation time for all users). Another alternative to visualize the Mathematica code is to install the Wolfram Player software., Peer reviewed

Multimedia component 1. S1. Costs used for LCCA calculations S2. Details of the modelling approach used in the dynamic part of the study S2.1. Parameters used for finding a Pareto frontier using gamultiobj Matlab function S2.2. Physical parameters of the components used for the calculations and modelling in this study, Peer reviewed

The Supplemental Material contains the following sections: -RESISTIVITIES OF THE DIFFERENT ELECTRODES IN THE Py/Cu/W LSV -STEM CHARACTERIZATION OF THE Cu/W INTERFACE -STOICHIOMETRIC COMPOSITION OF THE WOx LAYER -3D FEM SIMULATION FOR THE WOx RESISTIVITY -DERIVATION OF THE SPIN SIGNAL AND THE SPIN ABSORPTION IN A LSV -SPIN PROPERTIES OF THE Py AND Cu -SPIN DIFFUSION LENGTH FOR BULK SPIN ABSORPTION -DERIVATION OF THE SPIN-CHARGE SIGNAL IN A LSV -SHUNTING FACTOR IN THE Cu/WOx/W HETEROSTRUCTURE USING A 3D FEM SIMULATION -REPRODUCIBLE SPIN-TO-CHARGE INTERCONVERSION IN DIFFERENT DEVICES -CONTROL SPIN-CHARGE INTERCONVERSION EXPERIMENT IN Cu/SiO2, Peer reviewed

STM/STS data of additional dimers on Ag(111), spin density and Kondo map of 1+, large-scale images of fused products on Au(111), tip-induced deprotonation experiments of 4, resonance structures of 3 and 4, molecular orbitals of 2, density of states for 2, 3, and 4 adsorbed on Au(111), molecular orbitals of 3+ and 4+, comparative Kondo resonances of the various probed molecules, STS point spectra and experimental and simulated conductance maps of 4+, STM and STS analysis of trimers, relaxed structures of molecules adsorbed on Au(111), calculated molecular orbitals of 2+, STS point spectra, conductance maps, and molecular orbitals of 4″+, frontier molecular orbitals of 4″ before and after charge transfer, methods description of STM measurements, and DFT calculations., Peer reviewed

Figure S1 - QCM-D overtones plots for SLB formation with HKM and HKT buffer Figure S2 - QCM-D overtones plots for SLB formation with variable PIP2 % Figure S3 - QCM-D overtones plots for SLB with PIP2 and CD4 Figure S4 - ΔD versus Δf/n plots of SLB Figure S5 - Voigt-Voinova fitting Figure S6 - Lipid composition of unilamellar lipid vesicles for SLB formation Figure S7 - DLS particle size distribution profile for the conversion of MLV into SUV Figure S8 - Z-potential of lipid vesicles for SLB formation Table S1 - Lipid composition of unilamellar lipid vesicles for SLB formation Table S2 - Fitted parameters for NR data analysis Table S3 - Fixed parameters for NR data analysis Table S4 - DLS size and polydispersity index for the conversion of MLV into SUV Table S5 - DLS size and polydispersity index of the vesicles used for SLB formation, Peer reviewed

1. Large-scale morphology of 1T-TaSe2/1H-TaSe2 heterobilayers 2. Temperature-dependent low-energy electronic structure 3. Lower and upper Hubbard band in 1T-TaSe2 on 1H-TaSe2 4. The 1H-TaSe2/BLG substrate 5. Uncertainty band of Δ 6. Measurement of the non-linear behavior of Δ with the magnetic field 7. Absence of magnetism in single-layer TaSe2 8. Band structure calculations and estimate of Kondo hybridization 9. References, Peer reviewed

The supplemental material is organized as follows. In Section S1, we provide the details of the derivations of the parameter Γ, describing the magnetoelectric effect, for magnetic impurities in Rashba superconductors and superconducting Dirac systems. We consider two cases: in one case, the size of the magnetic impurity is comparable with the coherence length and hence the induced exchange field can be treated as homogeneous; in the other case, the magnetic impurity is point-like and the induced exchange field has a form of a delta-function. In Section S2, we provide the details of the derivation of the superconductivity-induced magnetic interaction. In Section S3, we show that in the limiting case where the current-induced magnetic field can be neglected, we reproduce the previous result of Ref. [15] (in the main text) in the absence of a magnetic field. Finally, in Section S4, we present a microscppic analysis of the surface of iron-based superconductor with a Dirac band., Supplementary material includes the derivations of Γ parameters in different systems, the derivations of the superconductivity-induced magnetic interaction, a comparison with the previous work, and a microscopic analysis of Fe(Se,Te)., Peer reviewed