Synthese von Carbolinen durch übergangsmetall-katalysierte [2+2+2]-Cycloaddition von Alkinen und Nitrilen: Ein neuer Weg zur Totalsynthese von Lavendamycin

Carboline sind eine große Gruppe von natürlich vorkommenden Alkaloiden, die eine tricyclische Pyrido[b]indol-Ringstruktur gemeinsam habe. Das breite Spektrum biologischer Eigenschaften dieser Verbindungsklasse macht sie zu einem interessanten Syntheseziel. Die größte Herausforderung in der Darstellung von Carbolinen ist die regioselektive Funktionalisierung an den aromatischen Positionen. Im Rahmen dieser Arbeit konnte ein A ABC-Zugang zu beta- und gamma-Carbolinen entwickelt werden, dessen Schlüsselschritt der Aufbau des Carbolin-Gerüsts durch eine übergangsmetall-katalysierte [2+2+2]-Cycloaddition von 1,6-Diin-Einheiten und Nitrilen ist. Die benötigten Diin-Einheiten wurden in wenigen Schritten ausgehend von 2-Iodanilin durch eine Reaktionssequenz aus Sonogashira-Reaktion mit terminalen Alkinen, N-Tosylierung und N-Ethinylierung mit Alkinyliodonium-Salzen synthetisiert. Eine flexible Funktionalisierung dieser Diine wurde durch palladium-katalysierte sp2-sp-Kreuzkupplungsreaktionen der terminalen Alkine mit Aryl- und Alkenylhalogeniden erreicht. Cp*RuCl- und [Rh(cod)2]BF4/BINAP-katalysierte [2+2+2]-Cycloadditionen der 1,6-Diine mit elektronenarmen Nitrilen lieferte in hoher Regioselektivität beta- oder gamma-Carboline. In Übereinstimmung mit literaturbekannten übergangsmetall-katalysierten [2+2+2]-Cycloadditionen konnte dabei eine starke Abhängigkeit von sterischen und elektronischen Faktoren beobachtet werden. Um das Potential dieser Methode zu demonstrieren, wurde der Einsatz der [2+2+2]-Cycloaddition in Totalsynthese von Lavendamycin untersucht. Lavendamycin, ein aus Bakterien stammendes Chinochinolin-substituiertes beta-Carbolin mit antimikrobieller und signifikanter Antitumor-Aktivität, wurde ausgehend von Hydrochinon und 2-Iodanilin in 14 Schritten und in einer Gesamtausbeute von 29% dargestellt.

Nuovi complessi alchinil tetrazolici di iridio(III) e renio(I): Sintesi, reattività e proprietà fotofisiche.

In this experimental thesis, two luminescent Ir(III) and Re(I) complexes which have a terminal alkynyl group on the tetrazole ligand were prepared. The aim was to use them as building blocks, in order to synthesize more complex structures. We explored two simple reactions: the first one was a coupling, for the formation of Ir(III)/Au(III) and Re(I)/Au(III) hetero binuclear complexes, and the second was a 1,3-dipolar Cu(I)-catalyzed “Click” cycloaddition, between the terminal alkyne and azide. The synthesized products were characterized through photophysical analysis, evaluating how the photoemissive properties of these substrates were affected by the formation of more complex structures. In questo lavoro di tesi sperimentale sono stati preparati due complessi luminescenti di Ir(III) e Re(I) che presentano un alchino terminale sul legante tetrazolico. Lo scopo è stato quello di utilizzarli come building blocks per la sintesi di strutture più complesse. Sono state esplorate due semplici reazioni: la prima di coupling, per la formazione di complessi etero binucleari Ir(III)/Au(III) e Re(I)/Au(III), e la seconda di “click”, ossia una cicloaddizione 1,3-dipolare Cu(I) catalizzata tra l’alchino terminale e un’azide. I prodotti sintetizzati sono stati caratterizzati attraverso analisi fotofisiche, valutando come le proprietà fotoemissive di questi substrati siano influenzate in seguito alla formazione di strutture più complesse.

Synthesis of carbolines and analogues via rhodhium-catalyzed [2+2+2] cycloaddition with alkynyl-ynamides : application to the total synthesis of alkaloids

The main research theme of this dissertation is the synthesis of g- and b-carbolines using a metal-catalyzed [2+2+2] cycloaddition strategy of tethered alkynyl-ynamides (diynes) with nitriles. g- and b-carbolines form the core of a large group of natural product and represent important targets for organic chemists. Many of these carbolines showed pharmacological effects ranging from anti-tumor to anxiolytic and anti-HIV activity. A model study with N-Ethynyl-N-tosyl-2-(2-phenylethynyl)aniline and methyl cyanoformate showed that rhodium-based catalysts promote efficiently the reaction. A further optimization showed that the regioselectivity of the reaction can be tuned by the choice of the solvent or by the catalytic system. Application to a larger scope of diynes showed that the regioselectivity strongly depends on the type of substitution of the alkynyl moieties, giving regioselectivities in the range g:b = 1/0 to g:b = 0/1. This [2+2+2] cycloaddition approach for the synthesis of the g- and b-carboline cores was successfully applied to the first total synthesis of Isoperlolyrine and the total synthesis of Perlolyrine. Extension of this strategy to heterocumulenes as cycloaddition partners allowed the synthesis of a g-carbolinone, a thiopyrano[3,4-b]indol-3-imine and thiopyranothiones.

Cycloaddition Reactions: Reaction of 3-Methyl-2-phenylpyrrocoline with Dimethyl Acteylenedicarboxylate

Reaction of 3-methyl-2-phenylpyrrocoline(I) and dimethyl acetylenedicarboxylate(II) in refluxing toluene furnishes cis-7',8-dihydro.4,5,8,9-tetramethoxycarbonyl-7'-phenyl-7' -methylazocino(2,1,8-cd]pyrrolizine (III) and trans-7',8-dihydro-4,5,8,9-tetramethoxycarbonyl-7-phenyl-7'-methylazocino[2,1,8-cd]pyrrolizine (IV), while the same reaction at ambient temperature yields 1-[(1,2-trans-dimethoxycarbonyl)vinyl]-3-methyl-2-phenylpyrrocoline (V) and 1-[(1,2-cis-di(methoxycarbonyl)vinyl)--methyl-2- phenylpyirocoUne (V) and 1-[(I,2-cis-di(methoxycarbonyl)Yinyl]-3-metbyl-2-phenylpyrrocoline(VI) as the major products. The structure of IV has been determined by X-ray crystallography.A possible mechanism of formation of these products is also discussed.

Nonequilibrium hysteresis and spin relaxation in the mixed-anisotropy dipolar-coupled spin-glass LiHo0.5Er0.5F4

We present a study of the model spin-glass LiHo0.5Er0.5F4 using simultaneous ac susceptibility, magnetization, and magnetocaloric effect measurements along with small angle neutron scattering (SANS) at sub-Kelvin temperatures. All measured bulk quantities reveal hysteretic behavior when the field is applied along the crystallographic c axis. Furthermore, avalanchelike relaxation is observed in a static field after ramping from the zero-field-cooled state up to 200–300 Oe. SANS measurements are employed to track the microscopic spin reconfiguration throughout both the hysteresis loop and the related relaxation. Comparing the SANS data to inhomogeneous mean-field calculations performed on a box of one million unit cells provides a real-space picture of the spin configuration. We discover that the avalanche is being driven by released Zeeman energy, which heats the sample and creates positive feedback, continuing the avalanche. The combination of SANS and mean-field simulations reveal that the conventional distribution of cluster sizes is replaced by one with a depletion of intermediate cluster sizes for much of the hysteresis loop.

Molecular dynamics of a grid-mounted molecular dipolar rotor in a rotating electric field

Classical molecular dynamics is applied to the rotation of a dipolar molecular rotor mounted on a square grid and driven by rotating electric field E(ν) at T ≃ 150 K. The rotor is a complex of Re with two substituted o-phenanthrolines, one positively and one negatively charged, attached to an axial position of Rh\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{2}^{4+}}}\end{equation*}\end{document} in a [2]staffanedicarboxylate grid through 2-(3-cyanobicyclo[1.1.1]pent-1-yl)malonic dialdehyde. Four regimes are characterized by a, the average lag per turn: (i) synchronous (a < 1/e) at E(ν) = |E(ν)| > Ec(ν) [Ec(ν) is the critical field strength], (ii) asynchronous (1/e < a < 1) at Ec(ν) > E(ν) > Ebo(ν) > kT/μ, [Ebo(ν) is the break-off field strength], (iii) random driven (a ≃ 1) at Ebo(ν) > E(ν) > kT/μ, and (iv) random thermal (a ≃ 1) at kT/μ > E(ν). A fifth regime, (v) strongly hindered, W > kT, Eμ, (W is the rotational barrier), has not been examined. We find Ebo(ν)/kVcm−1 ≃ (kT/μ)/kVcm−1 + 0.13(ν/GHz)1.9 and Ec(ν)/kVcm−1 ≃ (2.3kT/μ)/kVcm−1 + 0.87(ν/GHz)1.6. For ν > 40 GHz, the rotor behaves as a macroscopic body with a friction constant proportional to frequency, η/eVps ≃ 1.14 ν/THz, and for ν < 20 GHz, it exhibits a uniquely molecular behavior.

Coinage Metal Complexes as Chiral Catalysts for 1,3-Dipolar Cycloadditions

In this account, we describe the experience of our research group in the implementation of chiral coinage metal complexes into the efficient enantioselective 1,3-DC of azomethine ylides derived from α-amino acids and azlactones with different dipolarophiles. The corresponding chiral metallodipoles were generated in situ and next focused on the synthesis of highly substituted prolines. For this purpose, privileged ligands such as phosphoramidites and binap with silver(I), gold(I) and copper(II) salts are described. Depending from the ligand and mainly from the metal salt it can be possible to control the facial endo/exo-diasteroselectivity and the enantioselectivity of these types of processes. The synthetic processes are also supported by DFT calculations in order to elucidate the most plausible mechanism and the stereochemical results.

Multicomponent Azide-Alkyne Cycloaddition Catalyzed by Impregnated Bimetallic Nickel and Copper on Magnetite

A new bimetallic catalyst derived from nickel and copper has been used successfully for the first time in the multicomponent reaction of terminal alkynes, sodium azide, and benzyl bromide derivatives. The presence of both metallic species on the surface of magnetite seems to have a positive and synergetic effect. The catalyst loading is the lowest ever published for a catalyst of copper anchored on any type of iron support. The catalyst could be easily removed from the reaction media just by magnetic decantation and it could be reused up to ten times without any negative effect on the initial results.

Bistability and hysteresis of dipolar dynamos generated by turbulent convection in rotating spherical shells

Bistability and hysteresis of magnetohydrodynamic dipolar dynamos generated by turbulent convection in rotating spherical fluid shells is demonstrated. Hysteresis appears as a transition between two distinct regimes of dipolar dynamos with rather different properties including a pronounced difference in the amplitude of the axisymmetric poloidal field component and in the form of the differential rotation. The bistability occurs from the onset of dynamo action up to about 9 times the critical value of the Rayleigh number for onset of convection and over a wide range of values of the ordinary and the magnetic Prandtl numbers including the value unity. Copyright © EPLA, 2009.

Influência da interação dipolar nas fases magnéticas de nanopartículas esféricas com estrutura núcleo@camada

Bi-magnetic core@shell nanoparticle has attracted attention several researchers because great applicability that they offer. The possibility of combining different functionalities of magnetic materials make them a key piece in many areas as in data processing permanent magnets and biomagnetics sistems. These nanoparticles are controlled by intrinsic properties of the core and shell materials as well as the interactions between them, besides size and geometry effects. Thus, it was developed in this thesis a theoretical study about dipolar interaction contribution between materials different magnetic properties in bi-magnetic core@shell nanoparticles conventional spherical geometry. The materials were analyzed CoFe2O4, MnFe2O4 e CoFe2 in various combinations and sizes. The results show that the impact of the core dipole field in the shell cause reverse magnetization early its, before of the core, in nanoparticle of CoFe2O4(22nm)@CoFe2(2nm), thereby causing a decrease coercivity field of 65% in comparection with simple nanoparticle of CoFe2O4 (HC=13.6 KOe) of same diameter. The large core anisotropy in conventional nanoparticle makes it the a stable dipolar field source in the shell, that varies length scale of the order of the core radius. Furthermore, the impact of dipolar field is greatly enhanced by the geometrical constraints and by magnetics properties of both core@shell materials. In systems with core coated with a thin shell of thickness less than the exchange length, the interaction interface can hold reversal the shell occurring an uniform magnetization reversal, however this effect only is relevant on systems where the dipole field effects is weak compared with the exchange interaction.