Abstract:Molecular spintronics is made possible by the coupling between electronic configuration and magnetic polarization of the molecules. For control and application of the individual molecular states it is necessary to both read and write their spin states. Conventionally, this is achieved by means of external magnetic fields or ferromagnetic contacts, which may change the intentional spin state and may present additional challenges when downsizing devices. Here, we predict that coupling magnetic molecules together… Show more
“…This prediction is based on the (electronically mediated) indirect exchange interaction between the localized spins which controls the charge transport properties [51,52]. Similar effects were reported in Ref.…”
Section: Introductionsupporting
confidence: 75%
“…In such set-ups, the effective magnetic interaction parameter J between the two spins can be calculated using the expression, see Refs. [51,53],…”
Section: Exchange Interactionsmentioning
confidence: 99%
“…For the details about the interdependence between the electronic structure in the molecular orbitals and the spin-spin exchange we refer to Refs. [51,53]. The temperatures of the leads are included in the respective Fermi function on which the exchange interaction within the spin dimer depends, see Eq.…”
Section: Non-equilibrium Variationsmentioning
confidence: 99%
“…Theoretical predictions suggest all electrical control for both reading and writing spin states in molecular dimers * Electronic address: Jonas.Fransson@physics.uu.se [51,52]. This prediction is based on the (electronically mediated) indirect exchange interaction between the localized spins which controls the charge transport properties [51,52].…”
Section: Introductionmentioning
confidence: 99%
“…[51,53] for dimers of magnetic molecules in which the effective spin-spin interactions are mediated by the properties of the delocalized electrons and extend to thermally induced magnetic and transport properties. In particular we study thermal transport and its response to changes of the magnetic configurations.…”
We consider charge and thermal transport properties of magnetically active paramagnetic molecular dimer. Generic properties for both transport quantities are reduced currents in the ferro-and anti-ferromagnetic regimes compared to the paramagnetic and efficient current blockade in the anti-ferromagnetic regime. In contrast, while the charge current is about an order of magnitude larger in the ferromagnetic regime, compared to the antiferromagnetic, the thermal current is efficiently blockaded there as well. This disparate behavior of the thermal current is attributed to current resonances in the ferromagnetic regime which counteract the thermal flow. The temperature difference strongly reduces the exchange interaction and tends to destroy the magnetic control of the transport properties. The weakened exchange interaction opens up a possibility to tune the system into thermal rectification, for both the charge and thermal currents.
“…This prediction is based on the (electronically mediated) indirect exchange interaction between the localized spins which controls the charge transport properties [51,52]. Similar effects were reported in Ref.…”
Section: Introductionsupporting
confidence: 75%
“…In such set-ups, the effective magnetic interaction parameter J between the two spins can be calculated using the expression, see Refs. [51,53],…”
Section: Exchange Interactionsmentioning
confidence: 99%
“…For the details about the interdependence between the electronic structure in the molecular orbitals and the spin-spin exchange we refer to Refs. [51,53]. The temperatures of the leads are included in the respective Fermi function on which the exchange interaction within the spin dimer depends, see Eq.…”
Section: Non-equilibrium Variationsmentioning
confidence: 99%
“…Theoretical predictions suggest all electrical control for both reading and writing spin states in molecular dimers * Electronic address: Jonas.Fransson@physics.uu.se [51,52]. This prediction is based on the (electronically mediated) indirect exchange interaction between the localized spins which controls the charge transport properties [51,52].…”
Section: Introductionmentioning
confidence: 99%
“…[51,53] for dimers of magnetic molecules in which the effective spin-spin interactions are mediated by the properties of the delocalized electrons and extend to thermally induced magnetic and transport properties. In particular we study thermal transport and its response to changes of the magnetic configurations.…”
We consider charge and thermal transport properties of magnetically active paramagnetic molecular dimer. Generic properties for both transport quantities are reduced currents in the ferro-and anti-ferromagnetic regimes compared to the paramagnetic and efficient current blockade in the anti-ferromagnetic regime. In contrast, while the charge current is about an order of magnitude larger in the ferromagnetic regime, compared to the antiferromagnetic, the thermal current is efficiently blockaded there as well. This disparate behavior of the thermal current is attributed to current resonances in the ferromagnetic regime which counteract the thermal flow. The temperature difference strongly reduces the exchange interaction and tends to destroy the magnetic control of the transport properties. The weakened exchange interaction opens up a possibility to tune the system into thermal rectification, for both the charge and thermal currents.
A methodology implemented to compute photoionization cross sections beyond the electric dipole approximation using Gaussian type orbitals for the initial state and plane waves for the final state is applied to molecules of various sizes. The molecular photoionization cross sections computed for valence molecular orbitals as a function of photon energy present oscillations due to the wave-like nature of both the outgoing photoelectron and of the incoming photon. These oscillations are damped by rotational and vibrational averaging or by performing a k-point summation for the solid state case. For core orbitals, the corrections introduced by going beyond the electric dipole approximation are comparable to the atomic case. For valence orbitals, nondipole corrections to the total photoinization cross sections can reach up to 20% at photon energies above 1 keV. The corrections to the differential cross sections calculated at the magic angle are larger, reaching values between 30% and 50% for all molecules included. Our findings demonstrate that photoelectron spectroscopy, especially angle-resolved, on, e.g., molecules and clusters on surfaces, using high photon energies, must be accompanied by theories that go beyond the electric dipole approximation.
It is established that density functional theory (DFT) + U is a better choice compared to DFT for describing the correlated electron metal center in organometallics. The value of the Hubbard U parameter may be determined from linear response, either by considering the response of the metal site alone or by additionally considering the response of other sites in the compound. We analyze here in detail the influence of ligand shells of increasing size on the U parameter calculated from the linear response for five transition metal phthalocyanines. We show that the calculated multiple-site U is larger than the single-site U by as much as 1 eV and the ligand atoms that are mainly responsible for this difference are the isoindole nitrogen atoms directly bonded to the central metal atom. This suggests that a different U value may be required for computations of chemisorbed molecules compared to physisorbed and gas-phase cases.
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