People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Koch, Norbert
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (40/40 displayed)
- 2024Ion-induced field screening as a dominant factor in perovskite solar cell operational stabilitycitations
- 2024Non-equilibrium transport in polymer mixed ionic–electronic conductors at ultrahigh charge densitiescitations
- 2024Two Isomeric Thienoacenes in Thin Films: Unveiling the Influence of Molecular Structure and Intermolecular Packing on Electronic Properties
- 2023Surface doping of rubrene single crystals by molecular electron donors and acceptors
- 2023Enantiopure Dinaphtho[2,3-b:2,3-f]thieno[3,2-b]thiophenes: Reaching High Magnetoresistance Effect in OFETscitations
- 2023Defect-Dependent Optoelectronic Properties at a Molecular p-dopant/Monolayer WS2 Interface
- 2023Realization of Conductive n‐Type Doped <i>α</i>‐Ga<sub>2</sub>O<sub>3</sub> on <i>m</i>‐Plane Sapphire Grown by a Two‐Step Pulsed Laser Deposition Processcitations
- 2023Effect of ground state charge transfer and photoinduced charge separation on the energy level alignment at metal halide perovskite/organic charge transport layer interfaces
- 2023Molecular p-doping induced dielectric constant increase of polythiophene films determined by impedance spectroscopy Editor’s Pick
- 2023Charge Selective Contacts to Metal Halide Perovskites Studied with Photoelectron Spectroscopy ; X-Ray, Ultraviolet, and Visible Light Induced Energy Level Realignment
- 2023Recrystallization of MBE‐Grown MoS2 Monolayers Induced by Annealing in a Chemical Vapor Deposition Furnace
- 2023Improving the Resistance of Molecularly Doped Polymer Semiconductor Layers to Solvent
- 2023Enantiopure Dinaphtho[2,3-b:2,3-f]thieno[3,2-b]thiophenes: Reaching High Magnetoresistance Effect in OFETs.citations
- 2023Y‐Stabilized ZrO2 as a Promising Wafer Material for the Epitaxial Growth of Transition Metal Dichalcogenides
- 2023Enantiopure Dinaphtho[2,3‐<i>b</i>:2,3‐<i>f</i>]thieno[3,2‐<i>b</i>]thiophenes: Reaching High Magnetoresistance Effect in OFETscitations
- 2022Illumination-Driven Energy Level Realignment at Buried Interfaces between Organic Charge Transport Layers and a Lead Halide Perovskite
- 2022The Electronic Properties of a 2D Ruddlesden‐Popper Perovskite and its Energy Level Alignment with a 3D Perovskite Enable Interfacial Energy Transfercitations
- 2022Electronic properties of metal halide perovskites and their interfaces: the basics
- 2022Understanding performance limiting interfacial recombination in pin Perovskite solar cellscitations
- 2022Atomic Layer Deposition of MoS2 Decorated TiO2 Nanotubes for Photoelectrochemical Water Splittingcitations
- 2021Energy Level Alignment at the C60/Monolayer‐WS2 Interface on Insulating and Conductive Substratescitations
- 2021Mechanism and Timescales of Reversible p‐Doping of Methylammonium Lead Triiodide by Oxygencitations
- 2021Mechanism and Timescales of Reversible p‐Doping of Methylammonium Lead Triiodide by Oxygencitations
- 2021Understanding and suppressing non-radiative losses in methylammonium-free wide-bandgap perovskite solar cellscitations
- 2021Band gap engineering in blended organic semiconductor films based on dielectric interactionscitations
- 2021The Schottky–Mott Rule Expanded for Two-Dimensional Semiconductors: Influence of Substrate Dielectric Screening
- 2021Photoinduced energy-level realignment at interfaces between organic semiconductors and metal-halide perovskitescitations
- 2021Reversible oxygen-induced p-doping of mixed-cation halide perovskites
- 2020Conductive Polymer Work Function Changes due toResidual Water: Impact of Temperature-DependentDielectric Constant
- 2019Constructing the Electronic Structure of CH3NH3PbI3 and CH3NH3PbBr3 Perovskite Thin Films from Single-Crystal Band Structure Measurementscitations
- 2019Unraveling the Electronic Properties of Lead Halide Perovskites with Surface Photovoltage in Photoemission Studiescitations
- 2019The impact of energy alignment and interfacial recombination on the internal and external open-circuit voltage of perovskite solar cellscitations
- 2019High open circuit voltages in pin-type perovskite solar cells through strontium additioncitations
- 2018Interface Engineering of Solution-Processed Hybrid Organohalide Perovskite Solar Cellscitations
- 2017Reduced Interface-Mediated Recombination for High Open-Circuit Voltages in CH3NH3PbI3 Solar Cellscitations
- 2016Metal nanoparticle mediated space charge and its optical control in an organic hole-only devicecitations
- 2016Correlation of annealing time with crystal structure, composition, and electronic properties of CH3NH3PbI3-xClx mixed-halide perovskite filmscitations
- 2012Fluorinated copolymer PCPDTBT with enhanced open-circuit voltage and reduced recombination for highly efficient polymer solar cellscitations
- 2009Key role of molecular kinetic energy in early stages of pentacene island growthcitations
- 2003Interplay between morphology, structure, and electronic properties at diindenoperylene-gold interfacescitations
Places of action
Organizations | Location | People |
---|
article
Enantiopure Dinaphtho[2,3‐<i>b</i>:2,3‐<i>f</i>]thieno[3,2‐<i>b</i>]thiophenes: Reaching High Magnetoresistance Effect in OFETs
Abstract
<jats:title>Abstract</jats:title><jats:p>Chiral molecules are known to behave as spin filters due to the chiral induced spin selectivity (CISS) effect. Chirality can be implemented in molecular semiconductors in order to study the role of the CISS effect in charge transport and to find new materials for spintronic applications. In this study, the design and synthesis of a new class of enantiopure chiral organic semiconductors based on the well‐known dinaphtho[2,3‐<jats:italic>b</jats:italic>:2,3‐<jats:italic>f</jats:italic>]thieno[3,2‐<jats:italic>b</jats:italic>]thiophene (DNTT) core functionalized with chiral alkyl side chains is presented. When introduced in an organic field‐effect transistor (OFET) with magnetic contacts, the two enantiomers, (<jats:italic>R</jats:italic>)‐DNTT and (<jats:italic>S</jats:italic>)‐DNTT, show an opposite behavior with respect to the relative direction of the magnetization of the contacts, oriented by an external magnetic field. Each enantiomer displays an unexpectedly high magnetoresistance over one preferred orientation of the spin current injected from the magnetic contacts. The result is the first reported OFET in which the current can be switched on and off upon inversion of the direction of the applied external magnetic field. This work contributes to the general understanding of the CISS effect and opens new avenues for the introduction of organic materials in spintronic devices.</jats:p>