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Spin-electronic devices are poised to become part of mainstream microelectronic technology .Downsizing them, however, faces the intrinsic difficulty that as ferromagnets become smaller, it becomes more difficult to stabilize their magnetic moment. Antiferromagnets are much more stable, and thus research on antiferromagnetic spintronics has developed into a fast-growing field. Here, we provide proof of concept data that allows us to expand the area of antiferromagnetic spintronics to the hitherto elusive level of individual molecules. In contrast to all previous work on molecular spintronics, our detection scheme of the molecule's spin state does not rely on a magnetic moment. Instead, we use field-effect transistor devices constituting of an isolated, contacted single-wall carbon nanotube covalently bound to a limited number of molecular antiferromagnets incorporating four Mn(II) or Co(II) ions. Time-dependent quantum transport measurement along the functionalized nanotube show step-like transitions between several distinct current levels, which we attribute to transitions between different antiferromagnetic states of individual molecular complexes grafted on the nanotube. A statistical analysis of the switching events using factorial cumulants indicates that the cobalt complexes switch independently from each other, while a coherent superposition of the antiferromagnetic spin states of the molecules along the nanotube is observed for the manganese complexes. The long coherence time (several seconds at 100 mK) is made possible by the absence of spin and orbital momentum in the relevant states of the manganese complex, while the cobalt complex includes a significant orbital momentum contribution due to the pseudo-octahedral d$^7$ metal centers., including supplementary information

Altres ajuts: J.Y., P.K., M.G.M., and Z.Z. acknowledge the computer resources at MareNostrum and the technical support provided by the Barcelona Supercomputing Center through Red Española de Supercomputación (Grants No. RES-FI-2020-1-0018, No. RES-FI-2020-1-0014, and No. RES-FI-2020-2-0039). ICN2 is funded by the Generalitat de Catalunya (CERCA Programme). We acknowledge a PRACE award granting access to MareNostrum4 at Barcelona Supercomputing Center (BSC), Spain (OptoSpin project id. 2020225411). We evidence the possibility for coherent electrical manipulation of the spin orientation of topologically protected edge states in a low-symmetry quantum spin Hall insulator. By using a combination of ab initio simulations, symmetry-based modeling, and large-scale calculations of the spin Hall conductivity, it is shown that small electric fields can efficiently vary the spin textures of edge currents in monolayer 1T'-WTe2 by up to a 90-degree spin rotation, without jeopardizing their topological character. These findings suggest a new kind of gate-controllable spin-based device, topologically protected against disorder and of relevance for the development of topological spintronics.

Some metastable polymorphs of bismuth monolayers (bismuthene) can host non-trivial topological phases. However, it remains unclear whether these polymorphs can become stable through interaction with a substrate, whether their topological properties are preserved, and how to design an optimal substrate to make the topological phase more robust. Using first-principles techniques, we demonstrate that bismuthene polymorphs can become stable over silicon carbide (SiC), silicon (Si), and silicon dioxide (SiO) and that proximity interaction in these heterostructures has a significant effect on the electronic structure of the monolayer, even when bonding is weak. We show that van der Waals interactions and the breaking of the sublattice symmetry are the main factors driving changes in the electronic structure in non-covalently binding heterostructures. Our work demonstrates that substrate interaction can strengthen the topological properties of bismuthene polymorphs and make them accessible for experimental investigations and technological applications., We acknowledge the CERCA programme of the Generalitat de Catalunya (Grant 2017SGR1506), and by the Severo Ochoa programme (MINECO, SEV-2017-0706). Z Z acknowledges financial support by the Ramon y Cajal program (RYC-2016-19344), the Netherlands Sector Plan program 2019–2023, and support from the Dutch Gravity program "Materials for the Quantum Age (QuMat)". P O acknowledges support from Spanish MICIU, AEI and EU FEDER (Grant No. PGC2018-096955-B-C43) and the European Union MaX Center of Excellence (EU-H2020 Grant No. 824143). N W acknowledges support from the European Union's Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie Grant Agreement No. 754558, and the ICN2 Severo Ochoa Outbound Mobility Programme. The work has been performed under the Project HPC-EUROPA3 (INFRAIA-2016-1-730897), with the support of the EC Research Innovation Action under the H2020 Programme. We acknowledge computing resources on MareNostrum4 at Barcelona Supercomputing Center (BSC), provided through the PRACE Project Access (OptoSpin Project 2020225411) and RES (Activity FI-2020-1-0014), resources of SURFsara the on National Supercomputer Snellius (EINF-1858 Project) and technical support provided by the Barcelona Supercomputing Center.

The electronic structure of condensed matter can be significantly affected by the electron-phonon interaction, leading to important phenomena such as electrical resistance, superconductivity or the formation of polarons. This interaction is often neglected in band structure calculations but can have a strong impact on band gaps or optical spectra. Commonly used frameworks for electron-phonon energy corrections are the Allen-Heine-Cardona theory and the Fr\"ohlich model. While the latter shows qualitative agreement with experiment for many polar materials, its simplicity should bring hard limits to its applicability in real materials. Improvements can be made by introducing a generalized version of the model, which considers anisotropic and degenerate electronic bands, and multiple phonon branches. In this work, we search for trends and outliers on over a thousand materials in existing databases of phonon and electron band structures. We use our results to identify the limits of applicability of the standard Fr\"olich model by comparing to the generalized version, and by testing its basic hypothesis of a large radius for the polaronic wavefunction and the corresponding atomic displacement cloud. Among our extended set of materials, most exhibit large polaron behavior as well as validity of the perturbative treatment. For the valence band, there is also a significant fraction of the materials for which the perturbative treatment cannot be applied and/or for which the size of the self-trapping region is close to the atomic repetition distance. We find a large variety of behaviors, and employ much more accurate, fully ab initio Allen-Heine-Cardona calculations to understand extreme cases, where the Fr\"ohlich model should fail and unusually large zero-point renormalization energies occur.

Understanding heat flow in layered transition metal dichalcogenide (TMD) crystals is crucial for applications exploiting these materials. Despite significant efforts, several basic thermal transport properties of TMDs are currently not well understood, in particular how transport is affected by material thickness and the material's environment. This combined experimental–theoretical study establishes a unifying physical picture of the intrinsic lattice thermal conductivity of the representative TMD MoSe. Thermal conductivity measurements using Raman thermometry on a large set of clean, crystalline, suspended crystals with systematically varied thickness are combined with ab initio simulations with phonons at finite temperature. The results show that phonon dispersions and lifetimes change strongly with thickness, yet the thinnest TMD films exhibit an in-plane thermal conductivity that is only marginally smaller than that of bulk crystals. This is the result of compensating phonon contributions, in particular heat-carrying modes around ≈0.1 THz in (sub)nanometer thin films, with a surprisingly long mean free path of several micrometers. This behavior arises directly from the layered nature of the material. Furthermore, out-of-plane heat dissipation to air molecules is remarkably efficient, in particular for the thinnest crystals, increasing the apparent thermal conductivity of monolayer MoSe by an order of magnitude. These results are crucial for the design of (flexible) TMD-based (opto-)electronic applications., The authors thank Andrea Pitillas Martínez for the graphics shown in the ToC and Figure 1a,b. D.S.R. and S.V. would like to acknowledge the support of the Spanish Ministry of Economy through FPI-SO2019 and FPI-SO2018, respectively. R.F., P.O., and Z.Z. acknowledge support by the EU H2020-NMBP-TO-IND-2018 project “INTERSECT” (Grant No. 814487), the EC H2020-INFRAEDI-2018-2020 MaX “Materials Design at the Exascale” CoE (Grant No. 824143), and Spanish MCI/AEI/FEDER-UE (Grant No. PGC2018-096955-B-C43). O.H. acknowledges support from the Swedish Research Council (VR) program 2020-04630. P.W. acknowledges funding from the European Union's Horizon 2020 research and innovation program under the Marie Skłlodowska-Curie Grant Agreement No. 754510 (PROBIST). M.S., A.E.S., E.C.A., and C.M.S.T. acknowledge support of the Spanish MICIN project SIP (PGC2018-101743-B-I00). S.O.V. acknowledges support from MINECO under contract numbers PID2019-111773RB-I00/AEI/10.13039/501100011033. Z.Z. acknowledges financial support by the Netherlands Sector Plan program 2019-2023. M.J.V. acknowledges support from FRS-FNRS Belgium PdR Grant No. T.0103.19—ALPS, and contributions from the Melodica flag-era.net project. K.J.T., M.S., C.M.S.T., S.O.V., and N.F.v.H. acknowledge funding from BIST Ignite project 2DNanoHeat. K.J.T. acknowledges funding from the European Union's Horizon 2020 research and innovation program under Grant Agreement No. 804349 (ERC StG CUHL), RYC fellowship No. RYC-2017-22330, and IAE project PID2019-111673GB-I00. ICN2 was supported by the Severo Ochoa program from Spanish MINECO Grant No. SEV-2017-0706 and Generalitat de Catalunya (CERCA program and Grant 201756R1506).

Interference effects in finite sections of one-dimensional moir\'e crystals are investigated using a Landauer-B\"uttiker formalism within the tight-binding approximation. We explain interlayer transport in double-wall carbon nanotubes and design a predictive model. Wave function interference is visible at the mesoscale: in the strong coupling regime, as a periodic modulation of quantum conductance and emergent localized states; in the localized-insulating regime, as a suppression of interlayer transport, and oscillations of the density of states. These results could be exploited to design quantum electronic devices.

We present a joint experimental and theoretical characterization of the magnetic properties of coordination clusters with an antiferromagnetic core of four magnetic ions. Two different compounds are analyzed, with Co and Mn ions in the core. While both molecules are antiferromagnetic, they display different sensitivities to external magnetic field, according to the different strength of the intra-molecular magnetic coupling. In particular, the dependence of the magnetization versus field of the two molecules switches with temperatures: at low temperature the magnetization is smaller in \{Mn$_4$\}, while the opposite happens at high temperature. Through a detailed analysis of the electronic and magnetic properties of the two compounds we identify a stronger magnetic interaction between the magnetic ions in \{Mn$_4$\} with respect to \{Co$_4$\}. Moreover \{Co$_4$\} displays not negligible spin-orbit related effects that could affect the spin lifetime in future antiferromagnetic spintronic applications. We highlight the necessity to account for these spin-orbit effects for a reliable description of these compounds., 8 pages, 5 figures + supplementary Information

We present a joint experimental and theoretical characterization of the magnetic properties of coordination clusters with an antiferromagnetic core of four magnetic ions. Two different compounds are analyzed, with Co and Mn ions in the core. While both molecules are antiferromagnetic, they display different sensitivities to external magnetic field, according to the different atomic magnetic moments and strength of the intra-molecular magnetic couplings. In particular, the dependence of the magnetization versus field of the two molecules switches with temperature: at low temperature the magnetization is smaller in {Mn4} than in Co4, while the opposite happens at high temperature. Through a detailed analysis of the electronic and magnetic properties of the two compounds we identify a stronger magnetic interaction between the magnetic ions in {Mn4} with respect to {Co4}. Moreover {Co4} displays not negligible spin-orbit related effects that could affect the spin lifetime in future antiferromagnetic spintronic applications. We highlight the necessity to account for these spin-orbit effects together with electronic correlation effects for a reliable description of these compounds., The Authors acknowledge EU H2020 project NFFA (Grant No. 654360) under Transnational Access Activity ID-753. Computational resources in MareNostrum4 at the Barcelona Supercomputing Center were provided by the Red Española de Supercomputacion (Grants FI-2019-2-0038 and FI-2020-1-0022) and PRACE (grant OptoSpin, project id. 2020225411). ZZ acknowledges financial support by the Ramon y Cajal program RYC-2016-19344 (MINECO/AEI/FSE, UE) and the Netherlands Sector Plan program 2019-2023. PO, HX and ZZ thank the support by the EU H2020-NMBP-TO-IND-2018 project “INTERSECT” (Grant No. 814487), the EC H2020-INFRAEDI-2018-2020 MaX “Materials Design at the Exascale” CoE (Grant No. 824143), Grant PGC2018-096955-B-C43 funded by MCIN/AEI/10.13039/501100011033 (Spain) and “ERDF A way of making Europe” (European Union), the “Centro de Excelencia Severo Ochoa” Grant SEV-2017-0706 funded by MCIN/AEI/ 10.13039/501100011033 (Spain) and Generalitat de Catalunya (CERCA program and Grant 2017SGR1506). CM acknowledges funding by Niedersächsisches Vorab, Akz. 11-76251-14-3/15(ZN3141).

The quantitative analysis of electron-optical phase images recorded using off-axis electron holography often relies on the use of computer simulations of electron propagation through a sample. However, simulations that make use of the independent atom approximation are known to overestimate experimental phase shifts by approximately 10%, as they neglect bonding effects. Here, we compare experimental and simulated phase images for few-layer WSe2 . We show that a combination of pseudopotentials and all-electron density functional theory calculations can be used to obtain accurate mean electron phases, as well as improved atomic-resolution spatial distribution of the electron phase. The comparison demonstrates a perfect contrast match between experimental and simulated atomic-resolution phase images for a sample of precisely know thickness. The low computational cost of this approach makes it suitable for the analysis of large electronic systems, including defects, substitutional atoms and material interfaces.

Graphene and magnetoelectric multiferroics are promising materials for spintronic devices with high performance and low energy consumption. A very long spin diffusion length and high carrier mobility make graphene attractive for spintronics. The coupling between ferroelectricity and magnetism, which characterises magnetoelectrics, opens the way towards unique device architectures. In this work, we combine the features of both materials by investigating the interface between graphene and BaMnO3, a magnetoelectric multiferroic. We show that electron charge is transferred across the interface and magnetization is induced in the graphene sheet due to the strong interaction between C and Mn. Depending on the relative orientation of graphene and BaMnO3, a quasi-half-metal or a magnetic semiconductor can be obtained. A remarkably large proximity induced spin splitting of the Dirac cones (~300 meV) is achieved. We also show how doping with acceptors can make the high-mobility region of the electronic bands experimentally accessible. This suggests a series of possible applications in spintronics (e.g. spin filters, spin injectors) for hybrid organic-multiferroic materials and reveals hybrid organic-multiferroics as a new class of materials that may exhibit exotic phenomena such as the quantum anomalous Hall effect and a Rashba spin-orbit induced topological gap.

Combining structural and functional measurements, we have mapped the phase diagram of BiFeO3/LaFeO3 superlattices grown by off-axis sputtering on (110)o DyScO3 substrates. The phase diagram displays three distinct regions as a function of BiFeO3 fraction, with a BiFeO3-like ferroelectric phase and a LaFeO3-like paraelectric phase at its extremities, and a complex intermediate region, as supported by first-principles calculations. This intermediate region shows unusual, mixed functional behavior, most likely due to competing phases driven by substitution with a same-size central ion and the specific boundary conditions imposed by the superlattice structure. In the BiFeO3 rich superlattices, scaling of the ferroelectric-to-paraelectric transition temperature with the BiFeO3 thickness could provide an alternate route for studying ferroelectric size effects in BiFeO3.

First-principles techniques are used to investigate the behavior of BiFeO$_{3}$/LaFeO$_{3}$ perovskite oxide superlattices epitaxially grown on a (001)-SrTiO$_3$ substrate. The calculations show that 1/1 superlattices exhibit a $Pmc2_1$ ground state combining a trilinear coupling of one polar and two oxygen rotational lattice modes, and weak ferromagnetism. The microscopic mechanism allowing one to manipulate the magnetization with an electric field in such systems is presented and its dependence on strain and chemical substitution is discussed. BiFeO$_{3}$/LaFeO$_{3}$ artificial superlattices appear to be good candidates to achieve electric switching of magnetization at room temperature.

The structural and electronic properties of the wurtzite phase of the InAs and GaAs compounds are, for the first time, studied within the framework of Density Functional Theory (DFT). We used the full-potential linearized augmented plane wave (LAPW) method and the local density approximation (LDA) for exchange and correlation and compared the results to the corresponding pseudopotential calculations. From the structural optimization of the wurtzite polymorph of InAs we found that the c/a ratio is somewhat greater than the ideal one and that the internal parameter u/c has a value slightly smaller than the ideal one. In the all-electron approach the wurtzite polymorph has a smaller equilibrium volume per InAs pair and a higher binding energy when compared to the zinc-blende phase whereas the situation is reversed in the pseudo treatment. The energy differences are, however, smaller than the accuracy of standard density-functional codes (~30 meV) and a theoretical prediction of the relative stability of the two phases cannot be made. In order to investigate the possibility of using an LDA calculation as a starting point for many-body calculations of excitations properties, we here also present the band-structures of these materials. The bands are calculated with and without relativistic effects. In InAs we find that the energy gaps of both polymorphs are positive when obtained from a non-relativistic calculation and negative otherwise. For both semiconductors, we determine the spin-orbit splittings for the zinc-blende and the wurtzite phases as well as the crystal-field splittings for the new wurtzite polymorphs., 8 pages, 5 figures, 4 tables

Scientific reports 6(31346), 1-6 (2016). doi:10.1038/srep31346, Published by Nature Publishing Group, London

In this thesis, we present a theoretical study of two types of ferroic instabilities: the ferroelectric instability in novel confined geometries and magnetic instabilities controlled by the distortion of the underlying crystal lattice. On the one hand, we consider in detail the ferroelectric instability, specifically, in the nanotubes and the spherical nanoshells and develop a phenomenological theory for describing such an instability. We determine how the emergence of polarization is affected bythe thickness of the nanoparticle, the dielectric properties of the surrounding media and the interfacial boundary conditions. We finnd an intriguing topological finite-size effect that can promote an unexpected competition between two different types of distribution of polarization - irrotational and vortex-like - in the ultra-thin limit. One the other hand, we employ a different formalism to investigate the structural, electronic and magnetic properties of the rare-earth manganites. Specifically,we conduct a theoretical investigation from first-principles calculations. First, we predict a pressure-induced A-AFM insulator to FM metal transition on EuMnO3 under hydrostatic pressure, that is unprecedented in the multiferroic rare-earth manganites RMnO3. This investigation is extended to the study to the epitaxial strain effects on both EuMnO3 and TbMnO3 thin films. We show that epitaxial strain generates a much richer phase diagram compared to hydrostatic pressure. We predict novel magnetically-induced insulator { metal and polar { non-polar transitions. More specifically, we find that both the multiferroic E-AFM order and the polar metallic E*-AFM state are stabilized in TbMnO3 by means of epitaxial strain. In the contrast, we find a novel epitaxial-strain-induced multiferroic E-AFM state in EuMnO3 that cannot be obtained by means of just hydrostatic pressure., Dans cette thèse de doctorat nous présentons une étude théorique de deux types d'instabilitésferroélectriques: celles apparaissant dans des géométries confinés et celles induites par le magnétismedans dans composés massifs de structure perovskite. Dans une première partie nous abordons leproblème des instabilités ferroélectriques apparaissant dans des nanotubes et des nanocoquillesoù nous développons un modèle théorique phénoménologique approprié à ces structures. Nousétudions comment l'émergence de la polarisation est affectée par (i) l'épaisseur des nanostructures,(ii) par la réponse diélectrique des matériaux environant la couche ferroélectrique et (iii) les conditionsaux interfaces. Nous observons un effet de taille finie topologique qui peut promouvoirune compétition inhabituelle entre deux types de distribution de la polarization, irrotationel eten vortex, dans la limite des très petites épaisseurs. Dans une deuxième partie nous utilisons descalculs ab-initio à base de la théorie de la fonctionnelle de la densité pour étudier les instabilitésferroélectriques des perovskites manganites à base de terres rares (RMnO3). A partir de ces calculsnous prédisons qu'il est possible d'induire une transition de phase sous pression dans EuMnO3 lefaisant transiter d'un ordre antiferromagnétique de type A isolant vers un ordre ferromagnétiquemétallique sous pression. Ce type de transition n'avait jamais été reporté précédemment dans lesmatériaux RMnO3. Nous étendons ensuite cette analyse à l'étude des effets de strain épitaxial dansles films minces de TbMnO3 et EuMnO3. Nos résultats montrent que le diagramme de phase souscontrainte d'épitaxie est bien plus riche que celui sous pression hydrostatique. Nous trouvons queles types antiferromagnétiques E-AFM et E*-AFM sont stabilisés dans le cas de TbMnO3, où letype E*-AFM est une phase métallique polaire. Dans le cas de EuMnO3, nous trouvons une phaseantiferromagnétique de type E qui n'a pas été observée sous pression hydrostatique.