BUSCADOR RECOLECTA

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

Supplementary Note 1. COMSOL Multiphysics simulations S1.1 Details of the numerical simulations S1.2 Permittivities used in the simulations Supplementary Note 2. EEL spectrum for different velocities of the electron beam Supplementary Note 3. Modes of the cylindrical nanoresonator Supplementary Note 4. Multipole decomposition S4.1 Electric dipole S4.2 Electric quadrupole S4.3 Partial scattering contributions of the multipoles moments Supplementary Note 5. Nanodisk fabrication Supplementary Note 6. Nanodisk thickness determination S6.1 Electron energy loss spectroscopy S6.2 Tilted-view STEM imaging S6.3 Optical reflection spectroscopy Supplementary Note 7. Chemical composition from energy dispersive X-ray spectroscopy (EDS) Supplementary Note 8. Experimental EEL spectra Supplementary Note 9. Analysis of anisotropy effects in anapole excitation Supplementary Note 10. Analysis of the anapole-exciton coupled system S10.1 Details of the incident electric field and the scattering channels S10.2 Anapole-exciton coupled system within TCMT S10.3 Reproducing the EEL spectra with TCMT S10.4 Parameters obtained from the TCMT results Supplementary Note 11. Substrate influence in anapole excitation References for Supplementary Information, Peer reviewed

In supplemental material A we elaborate on the structure of the Hamiltonian and how it is obtained under general assumptions. In supplemental material B we provide the details of the tight-binding model used in the second of our letter and analytically show that it reduces to the low-energy model used in the first part of the letter with corrections of higher order in \Delta/\mu. Both supplemental materials are not necessary to understand our letter, but provide additional information on how we obtained our results., Peer reviewed

# Data for the manuscript "Superconductor-ferromagnet hybrids for non-reciprocal electronics and detectors", submitted to Superconductor Science and Technology, arXiv:2302.12732. This archive contains the data for all plots of numerical data in the manuscript. ## Fig. 4 Data of Fig. 4 in the WDX (Wolfram Data Exchange) format (unzip to extract the files). Contains critical exchange fields and critical thicknesses as functions of the temperature. Can be opened with Wolfram Mathematica with the command: Import[FileNameJoin[{NotebookDirectory[],"filename.wdx"}]] ## Fig. 5 Data of Fig. 5 in the WDX (Wolfram Data Exchange) format (unzip to extract the files). Contains theoretically calculated I(V) curves and the rectification coefficient R of N/FI/S junctions. Can be opened with Wolfram Mathematica with the command Import[FileNameJoin[{NotebookDirectory[],"filename.wdx"}]]. ## Fig. 7a Data of Fig. 7a in the ascii format. Contains G in uS as a function of B in mT and V in mV. ## Fig. 7c Data of Fig. 7c in the ascii format. Contains G in uS as a function of B in mT and V in mV. ## Fig. 7e Data of Fig. 7e in the ascii format. Contains G in uS as a function of B in mT and V in mV. The plots 7b, d, and f are taken from the plots a, c and e as indicated in the caption of the figure. ## Fig. 8 Data of Fig. 8 in the ascii format. Contains G in uS as a function V in mV for several values of B in mT. ## Fig. 8 inset Data of Fig. 8 inset in the ascii format. Contains G_0/G_N as a function of B in mT. ## Fig9a_b First raw Magnetic field values in T, first column voltage drop in V, rest of the columns differential conductance in S ## Fig9b_FIT First raw Magnetic field values in T, first column voltage drop in V, rest of the columns differential conductance in S ## Fig9c First raw Magnetic field values in T, first column voltage drop in V, rest of the columns R (real number) ## Fig9c inset First raw Magnetic field values in T, odd columns voltage drop in V, even columns injected current in A ## Fog9d Foist column magnetic field in T, second column conductance ration (real number), sample name in the file name. ## Fig. 12 Data of Fig. 12 in the ascii format. Contains energy resolution as functions of temperature and tunnel resistance with current and voltage readout. ## Fig. 13 Data of Fig. 13 in the ascii format. Contains energy resolution as functions of (a) exchange field, (b) polarization, (c) dynes, and (d) absorber volume with different amplifier noises. ## Fig. 14 Data of Fig. 14 in the ascii format. Contains detector pulse current as functions of (a) temperature change (b) time with different detector parameters. ## Fig. 17 Data of Fig. 17 in the ascii format. Contains dIdV curves as function of the voltage for different THz illumination frequency and polarization. ## Fig. 18 Data of Fig. 18 in the ascii format. Contains the current flowing throughout the junction as function time (arbitrary units) for ON and OFF illumination at 150 GHz for InPol and CrossPol polarization. ## Fig. 21 Data of Fig. 21c in the ascii format. Contains the magnitude of readout line S43 as frequency. Data of Fig. 21d in the ascii format. Contains the magnitude of iKID line S21 as frequency., SuperCONtacts – Solid state diffusion for atomically sharp interfaces in semiconductor-superconductor hybrid structures 101022473. European Commission SUPERTED – Thermoelectric detector based on superconductor-ferromagnet heterostructures 800923. European Commission SuperGate – Gate Tuneable Superconducting Quantum Electronics. 964398. European Commission, Peer reviewed

Supplemental material: -Materials and Methods. -Note 1: Calculation of experimentally measured critical current with edge asymmetry. -Note 2: False “in-plane” magnetic field induced diode effect. -Note 3: Suppression of critical current by out-of-plane magnetic field. -Note 4: Precise removal of the out-of-plane magnetic field. -Note 5: Estimation of the screening current in FM/SC bilayers. ., Peer reviewed

Figure S1 α-BSP2, α-OCN, and α-DMPI immunostaining of 7D-ADSC. Evolution over time at different timepoints. Individual pictures are orthogonal projections of a ≂80 μm Z-stack. Scale bar is 20 μm and pictures are magnified 40 times. Figure S2 α-BSP2, α-OCN, and α-DMPI immunostaining of 14D-ADSC. Evolution over time at different timepoints. Individual pictures are orthogonal projections of a ≂80 μm Z-stack. Scale bar is 20 μm and pictures are magnified 40 times. Table S1 List of acronyms used along the full main text., Peer reviewed

Differentially expressed genes were selected with DESeq2 (p-adj > 0.01, log2 FC ± 1.5)., Peer reviewed