Resultados de investigación

Experimental procedures, estimation of domain size, and additional supporting figures regarding DSC, viscosity, and diffraction results., Peer reviewed

Additional details on convergence tests, electronic structure of the isolated molecules and pristine crystals at the mean-field level, geometry optimization and charge population analysis, and results obtained from the PBE0 hybrid functional., 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

This is a data repository for the manuscript "Photoluminescence upconversion in monolayer WSe2 activated by plasmonic cavities through resonant excitation of dark excitons" by Niclas S. Mueller, Rakesh Arul, Gyeongwon Kang, Ashley P. Saunders, Amalya C. Johnson, Ana Sánchez-Iglesias, Shu Hu, Lukas A. Jakob, Jonathan Bar-David, Bart de Nijs, Luis M. Liz-Marzán, Fang Liu, and Jeremy J. Baumberg in Nature Communications (2023), DOI: https://doi.org/10.1038/s41467-023-41401-8., European Commission Horizon 2020 (H2020) ERC (883703) European Commission Horizon 2020 (H2020) Research Infrastructures (RI) (861950), 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

We first provide the explicit expressions of Fresnel and Mie coefficients under the duality and resonant mixing conditions. Then, we also attach the calculus of the expected value of helicity maps in the large and small sphere regime. Finally, we include the technical details of the time-independent perturbation theory applied to the photon hamiltonian., 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

See Supplemental Material at http://link.aps.org/supplemental/*** for computational details, crystal structures, electron localization functions, phonon dispersion relations, convex hull of Li-Au phases, electronic band structures, Eliashberg spectral function a2F() and frequency-dependent EPC parameter (), estimated Tc's, density of states and superconducting gaps, visualization of vibrational modes, and supplemental tables. (Includes Refs. [36-53])., 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