Ras Regulates the Polarity of the Yeast Actin Cytoskeleton through the Stress Response Pathway

Polarized growth in yeast requires cooperation between the polarized actin cytoskeleton and delivery of post-Golgi secretory vesicles. We have previously reported that loss of the major tropomyosin isoform, Tpm1p, results in cells sensitive to perturbations in cell polarity. To identify components that bridge these processes, we sought mutations with both a conditional defect in secretion and a partial defect in polarity. Thus, we set up a genetic screen for mutations that conferred a conditional growth defect, showed synthetic lethality with tpm1Δ, and simultaneously became denser at the restrictive temperature, a hallmark of secretion-defective cells. Of the 10 complementation groups recovered, the group with the largest number of independent isolates was functionally null alleles of RAS2. Consistent with this, ras2Δ and tpm1Δ are synthetically lethal at 35°C. We show that ras2Δ confers temperature-sensitive growth and temperature-dependent depolarization of the actin cytoskeleton. Furthermore, we show that at elevated temperatures ras2Δ cells are partially defective in endocytosis and show a delocalization of two key polarity markers, Myo2p and Cdc42p. However, the conditional enhanced density phenotype of ras2Δ cells is not a defect in secretion. All the phenotypes of ras2Δ cells can be fully suppressed by expression of yeast RAS1 or RAS2 genes, human Ha-ras, or the double disruption of the stress response genes msn2Δmsn4Δ. Although the best characterized pathway of Ras function in yeast involves activation of the cAMP-dependent protein kinase A pathway, activation of the protein kinase A pathway does not fully suppress the actin polarity defects, suggesting that there is an additional pathway from Ras2p to Msn2/4p. Thus, Ras2p regulates cytoskeletal polarity in yeast under conditions of mild temperature stress through the stress response pathway.

Fotofísica de enodionas

Em 1906, Albrecht obteve a primeira enodiona conhecida, ao reagir benzoquinona com ciclopentadieno. A estrutura desta enodiona somente foi elucidada em 1928, por Diels e Alder que, entretanto, perceberam ser possív.el existirem dois diferentes isômeros para o composto em questão: endo e exo. A descoberta, em 1958, da reação de fotocilização deste aduto de Diels-Alder, por Cookson e colaboradores, demonstrou que se tratava do isômero endo e esta reação passou a ser utilizada para se comprovar a configuração endo de vários compostos de estrutura análoga. Porém, apesar de sua importância histórica como método para comprovar a configuração dos adutos de Diels-Alder, os dados disponíveis até hoje são insuficientes para o esclarecimento dos processos subjacentes à fotociclização desses compostos, especialmente porque hoje sabemos que existem adutos de configuração endo que não fotociclizam. Visando aumentar o conhecimento sobre o comportamento destes adutos frente à reação de fotociclização, determinaram-se seus espectros de absorção (na região do UVNisível) e de emissão de luminescência e concluiu-se, com base em nossos resultados e daqueles relatados na literatura, que o fato de não ocorrer a fotociclização de alguns adutos de configuração endo não depende exclusivamente da estabilidade dos estados excitados envolvidos, ainda que essa característica e a natureza destes certamente afete os rendimentos quânticos da reação. Antes, parece-nos que estruturas que permitam deslocalizar um dos elétrons do birradical intermediariamente formado neste processo propiciam a reversão deste intermediário ao reagente, ao invés de se formar o produto de fotociclização. Alem disso, reinvestigamos a reação de fotoisomerização endo → exo do aduto de benzoquinona e ciclopentadieno, por irradiação em etanol/trietil-amina, relatada por Pandey e colaboradores em 1990, tendo verificado que tal isomerização não ocorre nas condições descritas na literatura, obtendo-se, ao invés disso, principalmente o tautômero aromático da enodiona e seu produto de fotociclização. Por outro lado, descobrimos que, deixar em repouso, no escuro, o aduto de benzoquinona e ciclopentadieno em etanol/trietil-amina conduz,a um dímero deste aduto, não descrito previamente.

Spin alignment of extra electrons in K-phenanthrene clusters taken from the crystalline tripotassium-intercalated phenanthrene structure

The appearance of ferromagnetic correlations among π electrons of phenanthrene (C14H10) molecules in the herringbone structure is proven for K doped clusters both by ab initio quantum-chemistry calculations and by the direct solution of the many-body Pariser-Parr-Pople Hamiltonian. Magnetic ground states are predicted for one or three additional electrons per phenanthrene molecule. These results are a consequence of the small overlap between the lowest unoccupied molecular orbitals (and lowest unoccupied molecular orbitals + 1) of neutral neighboring phenanthrene molecules, which makes the gain in energy by delocalization similar to the corresponding increase due to the Coulomb interaction.

Criteria for quantum coherent transfer of excitations between chromophores in a polar solvent

We show that the quantum decoherence of Forster resonant energy transfer between two optically active molecules can be described by a spin-boson model. This allows us to give quantitative criteria that are necessary for coherent quantum oscillations of excitations between the chromophores. Experimental tests of our results should be possible with flourescent resonant energy transfer (FRET) spectroscopy. Although we focus on the case of protein-pigment complexes our results are also relevant to quantum dots and organic molecules in a dielectric medium. (c) 2006 Elsevier B.V. All rights reserved.

Decoherence models for discrete-time quantum walks and their application to neutral atom experiments

We discuss decoherence in discrete-time quantum walks in terms of a phenomenological model that distinguishes spin and spatial decoherence. We identify the dominating mechanisms that affect quantum-walk experiments realized with neutral atoms walking in an optical lattice. From the measured spatial distributions, we determine with good precision the amount of decoherence per step, which provides a quantitative indication of the quality of our quantum walks. In particular, we find that spin decoherence is the main mechanism responsible for the loss of coherence in our experiment. We also find that the sole observation of ballistic-instead of diffusive-expansion in position space is not a good indicator of the range of coherent delocalization. We provide further physical insight by distinguishing the effects of short- and long-time spin dephasing mechanisms. We introduce the concept of coherence length in the discrete-time quantum walk, which quantifies the range of spatial coherences. Unexpectedly, we find that quasi-stationary dephasing does not modify the local properties of the quantum walk, but instead affects spatial coherences. For a visual representation of decoherence phenomena in phase space, we have developed a formalism based on a discrete analogue of the Wigner function. We show that the effects of spin and spatial decoherence differ dramatically in momentum space.

Exploiting Collective Effects to Direct Light Absorption in Natural and Artificial Light-harvesters

Photosynthesis –the conversion of sunlight to chemical energy –is fundamental for supporting life on our planet. Despite its importance, the physical principles that underpin the primary steps of photosynthesis, from photon absorption to electronic charge separation, remain to be understood in full. Electronic coherence within tightly-packed light-harvesting (LH) units or within individual reaction centers (RCs) has been recognized as an important ingredient for a complete understanding of the excitation energy transfer (EET) dynamics. However, the electronic coherence across units –RC and LH or LH and LH –has been consistently neglected as it does not play a significant role during these relatively slow transfer processes. Here, we turn our attention to the absorption process, which, as we will show, has a much shorter built-in timescale. We demonstrate that the- often overlooked- spatially extended but short-lived excitonic delocalization plays a relevant role in general photosynthetic systems. Most strikingly, we find that absorption intensity is, quite generally, redistributed from LH units to the RC, increasing the number of excitations which can effect charge separation without further transfer steps. A biomemetic nano-system is proposed which is predicted to funnel excitation to the RC-analogue, and hence is the first step towards exploiting these new design principles for efficient artificial light-harvesting.

Bis(arylene-ethynylene)-s-tetrazines: A Promising Family of n-Type Organic Semiconductors?

We theoretically describe in this work the n-type semiconducting behavior of a set of bis(arylene-ethynylene)-s-tetrazines ((ArCC)2Tz), by comparing their electronic properties with those of their parent diaryl-s-tetrazines (Ar2Tz) after the introduction of ethynylene bridges. The significantly reduced internal reorganization energy for electron transfer is ascribed to an extended delocalization of the LUMO for (ArCC)2Tz as opposite to that for Ar2Tz, which was described mostly localized on the s-tetrazine ring. The largest electronic coupling and the corresponding electron transfer rates found for bis(phenyl-ethynylene)-s-tetrazine, as well as for some halogenated derivatives, are comparable to those reported for the best performing n-type organic semiconductor materials such as diimides and perylenes. The theoretical mobilities for the studied compounds turn out to be in the range 0.3–1.3 cm2 V–1 s–1, close to values experimentally determined for common n-type organic semiconductors used in real devices. In addition, ohmic contacts can be expected when these compounds are coupled to metallic cathodes such as Na, Ca, and Sm. For these reasons, the future application of semiconducting bis(phenyl-ethynylene)-s-tetrazine and its fluorinated and brominated derivatives in optoelectronic devices is envisioned.

[n]cycloparaphenylenes with charges: cyclic conjugation at last

Oligophenylenes (polyphenylenes) are constituted by an array of conjugated benzenes where inter-ring electron delocalization tends to extend over the whole chain (linear conjugation) being intrinsically limited, among other factors, by terminal effects. Alternatively, cyclic conjugation is envisaged as the unlimited free-boundary versionofconjugation which will impact the structure of molecules in rather unknown ways. The cyclic version of oligophenylenes, cycloparaphenylenes ([n]CPPs with n the number of phenyl rings) were first synthesized in 2008 by Beztozzi and Jasti.1 Today the whole [n]CPP series from [5]CPP to [18]CPP has been prepared. [n]CPPs represent ideal models to investigate new insights of the electronic structure of molecules and cyclic conjugation when electrons or charges circulate in a closed circuit without boundaries. Radical cations and dications of [n]CPP from n=5 to n=12 have been prepared and studied by Raman spectroscopy.2 Small [n]CPP dications own their stability to the closed-shell electronic configuration imposed by cyclic conjugation. However, in large [n]CPP dications cyclic conjugation is minimal and these divalent species form open-shell biradicals. The Raman spectra reflect the effect of cyclic conjugation in competition with cyclic strain and biradicaloid aromatic stabilization. Cyclic conjugation provokes the existence of a turning point or V-shape behavior of the frequencies of the G bands as a function of n. In this communication we will show the vibrational spectroscopic fingerprint of this rare form of conjugation. [1] R. Jasti, J. Bhattacharjee, J. B. Neaton, C. R. Bertozzi, “Synthesis, Characterization, and Theory of [9]-, [12]-, and [18]Cycloparaphenylene: Carbon Nanohoop Structures”, J. Am. Chem. Soc. 130 (2008), 17646–17647. [2] M. P. Alvarez, P. M. Burrezo, M. Kertesz, T. Iwamoto, S. Yamago, J. Xia, R. Jasti, J. T. L. Navarrete, M. Taravillo, V. G. Baonza, J. Casado, “Properties of Sizeable [n]CycloParaPhenylenes As Molecular Models of Single-Wall Carbon Nanotubes By Raman Spectroscopy: Structural and Electron-Transfer Responses Under Mechanical Stress”, Angew. Chem. Int. Ed. 53, (2014), 7033−7037.

Insulator-to-metal transition in vanadium supersaturated silicon: variable-range hopping and Kondo effect signatures

We report the observation of the insulator-to-metal transition in crystalline silicon samples supersaturated with vanadium. Ion implantation followed by pulsed laser melting and rapid resolidification produce high quality single-crystalline silicon samples with vanadium concentrations that exceed equilibrium values in more than 5 orders of magnitude. Temperature-dependent analysis of the conductivity and Hall mobility values for temperatures from 10K to 300K indicate that a transition from an insulating to a metallic phase is obtained at a vanadium concentration between 1.1 × 10^(20) and 1.3 × 10^(21) cm^(−3) . Samples in the insulating phase present a variable-range hopping transport mechanism with a Coulomb gap at the Fermi energy level. Electron wave function localization length increases from 61 to 82 nm as the vanadium concentration increases in the films, supporting the theory of impurity band merging from delocalization of levels states. On the metallic phase, electronic transport present a dispersion mechanism related with the Kondo effect, suggesting the presence of local magnetic moments in the vanadium supersaturated silicon material.

Sintese de derivados 3 - substituídos de coumarinas

Este trabalho descreve a síntese de novos derivados de coumarinas 3-substituídas por grupos arilo, etenilarilo e etenil-organometálicos, através de novas metodologias via reacções de Heck e de metátese (Grubbs), com controlo da regioquímica e com significativos rendimentos reaccionais. A aplicação destas metodologias permitiu a síntese dos derivados, 3-fenilcoumarina (131), 3-(4-bromofenil)coumarina, (132), 3-(4-iodofenil)­coumarina (134), 3-(4-nitrofenil)coumarina (136), 3-(4-etilfenil)coumarina (133), 4-(coumarin-3-il)benzaldeído (135), 3-(4-metoxifenil)coumarina (137), (E)-3-acrilato-[4-(coumarin-3-il)fenil] de metilo (138), 6,7-metileno­dioxi-[3-(E)-2'-feniletenil]coumarina (145), 6,7-dimetoxi-[-(E)-2'-fenil­etenil]coumarina (146), 6,7-dimetoxi-[3-(E)-2'-(6'-nitrofenil)etenil]coumarina (147), 4-[2-(E)-(6,7-dimetoxicoumarin-3-il)etenil]benzaldeído (148) e 6,7-dimetoxi-[3-(E)-2'-ferroceniletenil]coumarina (149), dos quais os últimos nove, são compostos novos, identificados e caracterizados pela primeira vez. A deslocalização do sistema de electrões  conjugados, induzida pelos diversos substituintes das coumarinas, foi igualmente avaliada através da espectroscopia de UV/Vis. De referir que parte deste trabalho foi publicado como: "New Methodology for the Synthesis of 3-Substituted Coumarins via Pd-Catalyzed Site-Se/ective Cross-Coupling Reactions”, Sérgio Martins, Paula S. Branco, María C. de la Torre, Miguel A. Sierra e António Pereira, Synlett, 2010 (https://www.thieme-connect.com/ejournals/abstract/ synlett/doi/1 O.1 OS5/s-0030-1259014). ABSTRACT: This work describes the synthesis of new 3-aryl, ethenylaryl and ethenyl-organometallics coumarin derivatives, using a new methodology via Heck and metathesis (Grubbs) reactions, with regiochemistry control and significant reaction yields. The application of these methodologies allowed the synthesis of derivatives, 3-phenylcoumarin (131), 3-(4-bromophenyl)coumarin (132), 3-(4-iodophenyl)coumarin (134), 3-(4-nitrophenyl)coumarin (136), 3-(4-ethylphenyl)coumarin {133), 4-(coumarin-3-yl)benzaldehyde {135), 3-(4-methoxiphenyl)coumarin (137), (E)-ethyl 3-[4(coumarin-3-yl)phenyl]­acrylate (138), 6,7-methylenedioxy-[3-(E)-2'-phenylethenyl]coumarin (145), 6,7-dimethoxy-[-(E)-2'-phenylethenyl]coumarin (146), 6,7-dimethoxy-[3-(E)­-2'-(6'-nitrophenyl)ethenyl]coumarin (147), 4-[2-(E)-(6,7-dimethoxy­coumarin-3-yl)ethenyl]benzaldehyde {148) e 6,7-dimethoxy-[3-(E)-2'-(ferro­ cene)ethenyl]coumarin (149), the last nine of these are new compounds, identified and characterized for the first time. The delocalization of conjugated -electron system, induced by different substituents of coumarins, was also assessed by spectroscopy UV/Vis. Part of this work was published at: "New Methodology for the Synthesis of 3-Substituted Coumarins via Pd-Catalyzed Site-Selective Cross-Coupling Reactions", Sérgio Martins, Paula S. Branco, María C. de la Torre, Miguel A. Sierra e António Pereira, Synlett, 2010 (https://www.thieme­connect.com/ejournaIs/abstract/synlett/doi/1O.1 055/s-0030-1259014).