Theory for the change of bond character in divalent-metal clusters

To determine the size dependence of the bonding in divalent-metal clusters we use a many-electron Hamiltonian describing the interplay between van der Waals (vdW) and covalent interactions. Using a saddle-point slave-boson method and taking into account the size-dependent screening of charge fluctuations, we obtain for Hg_n a sharp transition from vdW to covalent bonding for increasing n. We show also, by solving the model Hamiltonian exactly, that for divalent metals vdW and covalent bonding coexist already in the dimers.

Relativistic LCAO with Minimax Principle and New Balanced Basis Sets

Relativistic density functional theory is widely applied in molecular calculations with heavy atoms, where relativistic and correlation effects are on the same footing. Variational stability of the Dirac Hamiltonian is a very important field of research from the beginning of relativistic molecular calculations on, among efforts for accuracy, efficiency, and density functional formulation, etc. Approximations of one- or two-component methods and searching for suitable basis sets are two major means for good projection power against the negative continuum. The minimax two-component spinor linear combination of atomic orbitals (LCAO) is applied in the present work for both light and super-heavy one-electron systems, providing good approximations in the whole energy spectrum, being close to the benchmark minimax finite element method (FEM) values and without spurious and contaminated states, in contrast to the presence of these artifacts in the traditional four-component spinor LCAO. The variational stability assures that minimax LCAO is bounded from below. New balanced basis sets, kinetic and potential defect balanced (TVDB), following the minimax idea, are applied with the Dirac Hamiltonian. Its performance in the same super-heavy one-electron quasi-molecules shows also very good projection capability against variational collapse, as the minimax LCAO is taken as the best projection to compare with. The TVDB method has twice as many basis coefficients as four-component spinor LCAO, which becomes now linear and overcomes the disadvantage of great time-consumption in the minimax method. The calculation with both the TVDB method and the traditional LCAO method for the dimers with elements in group 11 of the periodic table investigates their difference. New bigger basis sets are constructed than in previous research, achieving high accuracy within the functionals involved. Their difference in total energy is much smaller than the basis incompleteness error, showing that the traditional four-spinor LCAO keeps enough projection power from the numerical atomic orbitals and is suitable in research on relativistic quantum chemistry. In scattering investigations for the same comparison purpose, the failure of the traditional LCAO method of providing a stable spectrum with increasing size of basis sets is contrasted to the TVDB method, which contains no spurious states already without pre-orthogonalization of basis sets. Keeping the same conditions including the accuracy of matrix elements shows that the variational instability prevails over the linear dependence of the basis sets. The success of the TVDB method manifests its capability not only in relativistic quantum chemistry but also for scattering and under the influence of strong external electronic and magnetic fields. The good accuracy in total energy with large basis sets and the good projection property encourage wider research on different molecules, with better functionals, and on small effects.

Neurochondrin und Rack1 vermitteln die Signalintegration der Proteinkinase A

Die Spezifität und Effizienz zellulärer Signalprozesse wird durch die intrazelluläre Kompartimentierung von Signalmolekülen erreicht. A-Kinase-Ankerproteine (AKAPs) bilden eine Familie aus Gerüstproteinen, die zeitliche und räumliche Lokalisation der cAMP-abhängigen Proteinkinase (PKA) übernehmen. Die direkte Interaktion wird dabei über die Dimerisierungs- und Dockingdomäne (DD-Domäne) der regulatorischen Untereinheiten von PKA vermittelt. Das charakteristische strukturelle Merkmal bei kanonischen AKAPs ist eine amphipathische Helix. Es existiert allerdings auch eine kleine Gruppe von nicht-kanonischen AKAPs, deren Bindung an die DD-Domäne nicht über eine amphipathische Helix vermittelt wird. In dieser Arbeit wurden die zwei potentiellen nicht-kanonischen AKAPs Neurochondrin (neurite-outgrowth promoting protein) und Rack1 (receptor of activated C-kinase 1) charakterisiert. Neurochondrin, dessen Expression mit dem Neuriten-Wachstum in jungen Neuronen korreliert ist und das vermutlich eine entscheidende Funktion bei der Langzeitpotenzierung im Hippocampus übernimmt, zeigt in SPR-Bindungsstudien eine hochaffine, nanomolare Interaktion mit der R-Untereinheit Typ IIalpha von PKA. Kompetitionsanalysen mit dem AKAP-Disruptor-Peptid Ht 31 und Untersuchungen mit der isolierten DD-Domäne von RIIalpha bestätigen eine spezifische Interaktion. Das nicht-kanonische RII-Bindemotiv von Neurochondrin ist aus zwei Domänen aufgebaut, die einen hohen alpha-helikalen Anteil besitzen, aber keine amphipathische Helix bilden. Peptidbasierte Interaktionsstudien der einzelnen Domänen zeigen dennoch ebenfalls nanomolare Affinitäten zu RIIalpha. Rack1 ist ein etabliertes Gerüstprotein mit einer propellerartigen beta-Faltblattstruktur, für das bereits über 100 verschiedene Interaktionspartner beschrieben werden konnten. Die Integration von Rack1 in unterschiedliche Signalprozesse ist äußerst vielfältig. Um dabei die Spezifität jeder einzelnen Interaktion zu gewährleisten, sind individuelle Bindungsstrategien nötig. Die niedrigaffine Interaktion zur RIbeta-Untereinheit von PKA wird daher über multiple Bindestellen vermittelt. Die DD-Domäne von RIbeta übernimmt dabei eine spezifische Funktion, wie unter anderem durch Kompetitionsanalysen mit dem RI-spezifischen AKAP-Disruptor-Peptid RIAD gezeigt werden konnte. Die einzigartige Struktur der DD-Domäne generiert zudem ein Bindemotiv für Rack1, das Ähnlichkeiten mit der „Rack1 interacting-Domäne“ (RAID) von PDE4D5 aufweist. Sowohl Neurochondrin als auch Rack1 besitzen essenzielle neuronale Funktionen. Daher erweitert die Identifizierung der beiden neuen nicht-kanonischen AKAPs nicht nur die strukturelle Diversität der AKAP-Familie, sondern trägt zudem zum Verständnis der neuronalen Signalintegration von PKA bei.

Magnetic interactions between transition metal impurities and clusters mediated by low-dimensional metallic hosts: A first principles theoretical investigation

The magnetic properties and interactions between transition metal (TM) impurities and clusters in low-dimensional metallic hosts are studied using a first principles theoretical method. In the first part of this work, the effect of magnetic order in 3d-5d systems is addressed from the perspective of its influence on the enhancement of the magnetic anisotropy energy (MAE). In the second part, the possibility of using external electric fields (EFs) to control the magnetic properties and interactions between nanoparticles deposited at noble metal surfaces is investigated. The influence of 3d composition and magnetic order on the spin polarization of the substrate and its consequences on the MAE are analyzed for the case of 3d impurities in one- and two-dimensional polarizable hosts. It is shown that the MAE and easy- axis of monoatomic free standing 3d-Pt wires is mainly determined by the atomic spin-orbit (SO) coupling contributions. The competition between ferromagnetic (FM) and antiferromagnetic (AF) order in FePtn wires is studied in detail for n=1-4 as a function of the relative position between Fe atoms. Our results show an oscillatory behavior of the magnetic polarization of Pt atoms as a function of their distance from the magnetic impurities, which can be correlated to a long-ranged magnetic coupling of the Fe atoms. Exceptionally large variations of the induced spin and orbital moments at the Pt atoms are found as a function of concentration and magnetic order. Along with a violation of the third Hund’s rule at the Fe sites, these variations result in a non trivial behavior of the MAE. In the case of TM impurities and dimers at the Cu(111), the effects of surface charging and applied EFs on the magnetic properties and substrate-mediated magnetic interactions have been investigated. The modifications of the surface electronic structure, impurity local moments and magnetic exchange coupling as a result of the EF-induced metallic screening and charge rearrangements are analysed. In a first study, the properties of surface substitutional Co and Fe impurities are investigated as a function of the external charge per surface atom q. At large inter-impurity distances the effective magnetic exchange coupling ∆E between impurities shows RKKY-like oscillations as a function of the distance which are not significantly affected by the considered values of q. For distances r < 10 Å, important modifications in the magnitude of ∆E, involving changes from FM to AF coupling, are found depending non-monotonously on the value and polarity of q. The interaction energies are analysed from a local perspective. In a second study, the interplay between external EF effects, internal magnetic order and substrate-mediated magnetic coupling has been investigated for Mn dimers on Cu(111). Our calculations show that EF (∼ 1eV/Å) can induce a switching from AF to FM ground-state magnetic order within single Mn dimers. The relative coupling between a pair of dimers also shows RKKY-like oscillations as a function of the inter-dimer distance. Their effective magnetic exchange interaction is found to depend significantly on the magnetic order within the Mn dimers and on their relative orientation on the surface. The dependence of the substrate-mediated interaction on the magnetic state of the dimers is qualitatively explained in terms of the differences in the scattering of surface electrons. At short inter-dimer distances, the ground-state configuration is determined by an interplay between exchange interactions and EF effects. These results demonstrate that external surface charging and applied EFs offer remarkable possibilities of manipulating the sign and strength of the magnetic coupling of surface supported nanoparticles.