BUSCADOR RECOLECTA

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

This repository contains research data for all figures of the manuscript. This includes optomechanical simulations of plasmonic nanocavities and experimental SERS spectra from both NPoM nanocavities and SPARK picocavities. All data are provided in .txt files, space separated, with columns labelled in first row. The data are organized in folders for each figure, with individual files for each figure panel containing data. All further information is contained in the captions of the manuscript., Engineering and Physical Sciences Research Council (2275079) EPSRC (2275079) Engineering and Physical Sciences Research Council (EP/N016920/1) Engineering and Physical Sciences Research Council (EP/L027151/1) Engineering and Physical Sciences Research Council (EP/L015978/1) European Commission Horizon 2020 (H2020) Future and Emerging Technologies (FET) (829067) European Commission Horizon 2020 (H2020) Research Infrastructures (RI) (861950) European Commission Horizon 2020 (H2020) ERC (883703), Peer reviewed

Supplementary SEM and AFM images, XPS characterization, Faradaic efficiency, two-electrode test, EIS, SEC data, and TXRF (PDF). Video showing the visual increase in the electrode area (MP4)., Peer reviewed

Computational Details Supplementary Figures Supplementary Tables References, Peer reviewed

1. Materials and Techniques: 1.1. Materials - 1.2. Techniques 2. Synthetic Procedures: 2.1. Metamorphosis of commercial PVC to PVC-single-chain nanoparticles (PVC-SCNPs) with common organic solvents and non-solvents - 2.2. Screening of “green” solvents for the metamorphosis of “waste PVC” to valorized PVC single-chain nanoparticles (vPVC-SCNPs) - 2.3. Metamorphosis of “PVC waste” to vPVC-SCNPs in NBP as “green” solvent and EtOH / H2O (1 / 1 vol.) as non-solvent: 2.3.1. Flexible PVC - 2.3.2. Rigid PVC - 2.4. Preparation of vPVC-SCNPs/Cu(II) as efficient catalytic SCNPs 3. Additional Data: 3.1.Supplementary Tables - 3.2.Supplementary Figures 4. Supplementary References, Peer reviewed

Further details on the introduced concept, the experimental setup, additional CD, and reference measurements; further theory details about the chirality transfer., Peer reviewed

Expression for the circularly polarized fundamental field convenient for an analysis of nonlinear effects; definition of the charge multipoles in cylindrical coordinates and induced potential of the nanowire; analysis of the induced nonlinear near field; definition of the linear multipolar polarizabilities; discussion on the time-to-frequency Fourier transform used to analyze the time-dependent results of the TDDFT and to obtain the frequency-resolved quantities; classical nonretarded calculations of the linear response; extended discussion of the symmetry constraints for the bulk contribution to nonlinear polarization; derivation of the selection rules based on the nonlinear density response formalism; results showing magnetization of the nanowire by a circularly polarized fundamental field pulse; and discussion of the Friedel oscillations of the ground-state electron density (PDF). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the fundamental frequency (n = 1) for circular polarization with SAM = 1 of the incoming field (MP4). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 2 harmonic for circular polarization with SAM = 1 of the incoming field (MP4). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 3 harmonic for circular polarization with SAM = 1 of the incoming field (MP4). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at n = 4 harmonic for circular polarization with SAM = 1 of the incoming field (MP4). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the fundamental frequency (n = 1) for linear polarization of the incoming field (MP4). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 2 harmonic for linear polarization of the incoming field (MP4). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 3 harmonic for linear polarization of the incoming field (MP4). Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 4 harmonic for linear polarization of the incoming field (MP4)., Peer reviewed