424 research outputs found

    Giant nonlinear conduction and thyristor-like negative derivative resistance in BaIrO3 single crystals

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    We synthesized single-crystalline samples of monoclinic BaIrO3 using a molten flux method, and measured their magnetization, resistivity, Seebeck coefficient and nonlinear voltage-current characteristics. The magnetization rapidly increases below a ferromagnetic transition temperature TC of 180 K, where the resistivity concomitantly shows a hump-type anomaly, followed by a sharp increase below 30 K. The Seebeck coefficient suddenly increases below TC, and shows linear temperature dependence below 50 K. A most striking feature of this compound is that the anomalously giant nonlinear conduction is observed below 30 K, where a small current density of 20 A/cm2 dramatically suppresses the sharp increase in resistivity to induce a metallic conduction down to 4 K.Comment: 10 pages, 4 figures Submitted to Physical Review Letter

    Modulation Of The Catalytic Activity Of Porphyrins By Lipid- And Surfactant-containing Nanostructures

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    The structural factors modulating porphyrin activity encompass pyrrole and equatorial ligands, as well as the central metal and the number and structure of their axial ligands. Of equal importance is the microenvironment provided by apoproteins, solvents and membranes. Porphyrins are often used to construct supramolecular structures with different applications. The modulation of activity of the porphyrins has been frequently achieved by mimicking nature, i.e., by the provision of different microenvironments for these molecules. The association of porphyrins to surfactant- and lipid-containing nanostructures has changed the activity of these compounds to mimic different enzymes such as SOD, cytochrome P450, peroxidases and others. In determined conditions, the reactive forms of the porphyrins are high-valence states of oxo-metal-π cations and oxo-metal produced by the reaction with peroxides and peracids. The modulation of porphyrin activity by surfactant- and lipid-containing nanostructures has also been achieved for hemeproteins, as the lipid nanostructures affect the conformation of proteins. ©2011 Sociedade Brasileira de QuĂ­mica.22916211633Drain, C.M., Varotto, A., Radivojevic, I., (2009) Chem. Rev., 109, p. 1630Aida, T., Inoue, S., (2000) The Porphyrin Handbook, , Kadish, K., M. Smith, K., M. Guillard R., eds.Academic Press: San Diego ch. 42Ponka, P., (1999) Am. J. Med. Sci., 318, p. 241Da Silva, D.C., De Freitas-Silva, G., Do Nascimento, E., Rebouças, J.S., Barbeira, P.J., De Carvalho, M.E., Idemori, Y.M., (2008) J. Inorg. Biochem., 102, p. 1932Bochot, C., Bartoli, J.F., Frapart, Y., Dansette, P.M., Mansuy, D., Battioni, P., (2007) J. Mol. Catal. A.: Chem., 263, p. 200Alkordi, M.H., Liu, Y.L., Larsen, R.W., Eubank, J.F., Eddaoudi, M., (2008) J. Am. Chem. Soc., 130, p. 12639Suijkerbuijk, B., Schamhart, D.J., Kooijman, H., Spek, A.L., Van Koten, G., Gebbink, R., (2010) Dalton Trans., 39, p. 6198Groves, J.T., Nemo, T.E., (1983) J. Am. Chem. Soc., 10, p. 5786Drain, C.M., Smeureanu, G., Patel, S., Gong, X.C., Garno, J.A., (2006) New. J. Chem., 30, p. 1834Wang, Y.T., Jin, W.J., (2008) Spectrochim. Acta, Part A., 70, p. 871Komatsu, T., Moritake, W., Nakagawa, A., Tsuchida, E., (2002) Chem. - Eur. J., 8, p. 5469Nagami, H., Umakoshi, H., Shimanouchi, T., Kuboi, R., (2004) Biochem. Eng. J., 21, p. 221Szoka, F., Papahadjopoulos, D., (1980) Annu. Rev. Biophys. Bioeng., 9, p. 467Atkin, R., Craig, V.S.J., Wanless, E.J., Biggs, S., (2003) Adv. Colloid Interface Sci., 103, p. 219Grassert, I., Schinkowski, K., Vollhardt, D., Oehme, G., (1998) Chirality, 10, p. 754Hait, S.K., Moulik, S.P., (2001) J. Surfactants Deterg., 4, p. 303Glick, J., Santoyo, G., Casey, P.J., (1996) J. Biol. Chem., 271, p. 2949Maldotti, A., Andreotti, L., Molinari, A., Varani, G., Cerichelli, G., Chiarini, M., (2001) Green Chem., 3, p. 42Batrakova, E.V., Kabanov, A.V., (2008) J. Controlled Release, 130, p. 98Bangham, A.D., Standish, M.M., Watkins, J.C., (1965) J. Mol. Biol., 13, p. 238Johnson, S.M., Bangham, A.D., Hill, M.W., Korn, E.D., (1971) Biochim. Biophys. Acta. Biomembr., 233, p. 820Papahadj, D., Watkins, J.C., (1967) Biochim. Biophys. Acta, Biomembr., 135, p. 639Abramson, M.B., Katzman, R., Gregor, H.P., (1964) J. Biol. Chem., 239, p. 70Hauser, H.O., (1971) Biochem. Biophys. Res. Commun., 45, p. 1049Huang, C.H., (1969) Biochemistry, 8, p. 344Saunders, L., Gammack, D., Perrin, J., (1962) J. Pharm. Pharmacol., 14, p. 567Tien, H.T., (1974) Theory and Practice, , 1th ed.Bilayer Lipid Membranes (BLM): Marcel Dekker: New YorkRazin, S., (1972) Biochim. Biophys. Acta, Biomembr., 265, p. 241Korenbrot, J.I., (1977) Annu. Rev. Physiol., 39, p. 19Batzri, S., Korn, E.D., (1973) Biochim. Biophys. Acta, Biomembr., 298, p. 1015Deamer, D., Bangham, A.D., (1976) Biochim. Biophys. Acta, Biomembr., 443, p. 629Szoka, F., Papahadjopoulos, D., (1978) Proc. Natl. Acad. Sci. U. S. A., 75, p. 4194Mishra, P.P., Bhatnagar, J., Datta, A., (2005) J. Phys. Chem. B., 109, p. 24225Pessoto, F.S., Inada, N.M., Nepomuceno, M.D., Ruggiero, A.C., Nascimento, O.R., Vercesi, A.E., Nantes, I.L., (2009) Chem. Biol. Interact., 181, p. 400Steinbeck, C.A., Hedin, N., Chmelka, B.F., (2004) Langmuir, 20, p. 10399Vanesch, J.H., Feiters, M.C., Peters, A.M., Nolte, R.J.M., (1994) J. Phys. Chem., 98, p. 5541Barber, D.C., Freitagbeeston, R.A., Whitten, D.G., (1991) J. Phys. Chem., 95, p. 4074Maiti, N.C., Mazumdar, S., Periasamy, N.J., (1998) J. Porphyrins Phthalocyanines, 2, p. 369Schmehl, R.H., Whitten, D.G., (1981) J. Phys. Chem., 85, p. 3473Perrin, M.H., (1973) J. Chem. Phys., 59, p. 2090Zhou, X.T., Ji, H.B., (2010) Chem. Eng. J., 156, p. 411Monnereau, C., Ramos, P.H., Deutman, A.B.C., Elemans, J., Nolte, R.J.M., Rowan, A.E., (2010) J. Am. Chem. Soc., 132, p. 1529Merlau, M.L., Grande, W.J., Nguyen, S.T., Hupp, J.T., (2000) J. Mol. Catal. A: Chem., 156, p. 79Anzenbacher, P., Kral, V., Jursikova, K., Gunterova, J., Kasal, A., (1997) J. Mol. Catal. A: Chem., 118, p. 63Zhao, Y.C., Xiang, Y.Z., Pu, L., Yang, M., Yu, X.Q., (2006) Appl. Catal. A, 301, p. 176Zhou, X.T., Tang, Q.H., Ji, H.B., (2009) Tetrahedron Lett., 50, p. 6601Monfared, H.H., Aghapoor, V., Ghorbanloo, M., Mayer, P., (2010) Appl. Catal. A, 372, p. 209Heijnen, J.H.M., De Bruijn, V.G., Van Den Broeke, L.J.P., Keurentjes, J.T.F., (2003) Chem. Eng. Process., 42, p. 223Santos, A.C., Luz, R.A.S., Ferreira, L.G.F., Santos-JĂșnior, J.R., Silva, W.C., (2010) Quim. Nova, 33, p. 539Zhou, Y.B., Ryu, E.H., Zhao, Y., Woo, L.K., (2007) Organometallics, 26, p. 358Nantes, I.L., Crespilho, F.N., Mugnol, K.C.U., Chaves, J.C.A., Luz, R.A.S., Nascimento, O.R., Pinto, S.M.S., (2010) Circular Dichroism: Theory and Spectroscopy, , Rodgers D. S., ed.Nova Science Publishers: New York ch. 8Travascio, P., Sen, D., Bennet, A.J., (2006) Can. J. Chem., 84, p. 613Omodeo-Sale, F., Monti, D., Olliaro, P., Taramelli, D.P., (2001) Biochem. Pharmacol., 61, p. 999Ishigure, S., Mitsui, T., Ito, S., Kondo, Y., Kawabe, S., Kondo Dewa M, T., Mino, H., Nango, M., (2010) Langmuir, 26, p. 7774Umakoshi, H., Morimoto, K., Ohama, Y., Nagami, H., Shimanouchi, T., Kuboi, R., (2008) Langmuir, 24, p. 4451Prieto, T., Marcon, R.O., Prado, F.M., Caires, A.C.F., Di Mascio, P., Brochsztain, S., Nascimento, O.R., Nantes, I.L., (2006) J. Phys.Chem., 8, p. 1963Mugnol, K.C.U., Ando, R.A., Nagayasu, R.Y., Faljoni-Alario, A., Brochsztain, S., Santos, P.S., Nascimento, R.O., Nantes, I.L., (2008) Biophys. J., 94, p. 4066Nagatomo, H., Matsushita, Y., Sugamoto, K., Matsui, T., (2003) Tetrahedron: Asymmetry, 14, p. 2339Cantonetti, V., Monti, D., Venanzi, M., Bombelli, C., Ceccacci, F., Mancini, G., (2004) Tetrahedron: Asymmetry, 15, p. 1969Hiraka, K., Kanehisa, M., Tamai, M., Asayama, S., Nagaoka, S., Oyaizu, K., Yuasa, M., Kawakami, H., (2008) Colloids Surf. B, 67, p. 54Yuasa, M., Oyaizu, K., Horiuchi, A., Ogata, A., Hatsugai, T., Yamaguchi, A., Kawakami, H., (2004) Mol. Pharm., 1, p. 387Aron, J., Baldwin, D.A., Marques, H.M., Pratt, J.M., Adams, P.A., (1986) J. Inorg. Biochem., 27, p. 227Wang, J.S., Vanwart, H.E., (1989) J. Phys. Chem., 93, p. 7925Munro, O.Q., Marques, H.M., (1996) Inorg. Chem., 35, p. 3752Prieto, T., Nascimento, O.R., Tersariol, I.L.S., Faljoni-Alario, A., Nantes, I.L., (2004) J. Phys. Chem. B, 108, p. 11124Prieto, T., Nantes, I.L., Nascimento, O.R., (2004) Prog. Colloid Polym. Sci., 128, p. 1Makarska, M., Radzki, S., Legendziewicz, J., (2002) J. Alloys Compd., 341, p. 233Riposati, A., Prieto, T., Shida, C.S., Nantes, I.L., Nascimento, O.R., (2006) J. Inorg. Biochem., 100, p. 226Claiborne, A., Fridovich, I., (1979) J. Biol. Chem., 254, p. 4245Hiner, A.N.P., Ruiz, J.H., Lopez, J.N.R., Canovas, F.G., Brisset, N.C., Smith, A.T., Arnao, M.B., Acosta, M., (2002) J. Biol. Chem., 277, p. 26879Primus, J.L., Grunenwald, S., Hagedoorn, P.L., Albrecht-Gary, A.M., Mandon, D., Veeger, C.T., (2002) J. Am. Chem. Soc., 124, p. 1214Demontellano, P.R.O., (1992) Annu. Rev. Pharmacol. Toxicol., 32, p. 89Savenkova, M.I., Kuo, J.M., De Montellano, P.R.O., (1998) Biochemistry, 37, p. 10828Smith, A.T., Veitch, N.C., (1998) Curr. Opin. Chem. Biol., 2, p. 269Prieto, T., Mugnol, K.C.U., Araujo, J.C., Sousa, F.L., Soares, V.A., Cilento, G., Nantes, I.L., (2007) Catalysis and Photochemistry in Heterogeneous Media, , Nantes I. L.Brochesztain, S. eds.Research Signpost: Kerala ch. 1Zucchi, M.R., Nascimento, O.R., Faljoni-Alario, A., Prieto, T., Nantes, I.L., (2003) Biochem. J., 370, p. 671Kinnunen, P.K.J., (1992) Chem. Phys. Lipids, 63, p. 251Kawai, C., Prado, F.M., Nunes, G.L.C., Di Mascio, P., Carmona-Ribeiro, A.M., Nantes, I.L., (2005) J. Biol. Chem., 280, p. 34709Araujo, J.C., Prieto, T., Prado, F.M., Trindade, F.J., Nunes, G.L.C., Dos Santos, J.G., Di Masco, P., Nantes, I.L., (2007) J. Nanosci. Nanotechnol., 7, p. 3643Estevam, M.L., Nascimento, O.R., Baptista, M.S., Di Mascio, P., Prado, F.M., Faljoni-Alario, A., Zucchi, M.D., Nantes, I.L., (2004) J. Biol. Chem., 279, p. 39214Kawai, C., Nantes, I.L., Baptista, M.D.S., (2010) FEBS J., 277, p. 224Nantes, I.L., Faljoni-Alario, A., Vercesi, A.E., Santos, K.E., Bechara, E.J.H., (1998) Free Radic. Biol. Med., 25, p. 54

    Geometrical frustration induced (semi-)metal to insulator transition

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    We study the low-energy properties of the geometrically frustrated Hubbard model on a three-dimensional pyrochlore lattice and a two-dimensional checkerboard lattice on the basis of the renormalization group method and mean field analysis. It is found that in the half-filling case, a (semi-)metal to insulator transition (MIT) occurs. Also, in the insulating phase, which has a spin gap, the spin rotational symmetry is not broken, while charge ordering exists. The results are applied to the description of the MIT observed in the pyrochlore system Tl2Ru2O7{\rm Tl_2Ru_2O_7}.Comment: 4 pages, 5 figure

    Classical generalized constant coupling model for geometrically frustrated antiferromagnets

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    A generalized constant coupling approximation for classical geometrically frustrated antiferromagnets is presented. Starting from a frustrated unit we introduce the interactions with the surrounding units in terms of an internal effective field which is fixed by a self consistency condition. Results for the magnetic susceptibility and specific heat are compared with Monte Carlo data for the classical Heisenberg model for the pyrochlore and kagome lattices. The predictions for the susceptibility are found to be essentially exact, and the corresponding predictions for the specific heat are found to be in very good agreement with the Monte Carlo results.Comment: 4 pages, 3 figures, 2 columns. Discussion about the zero T value of the pyrochlore specific heat correcte

    Hemodynamic Assessment of Celiaco-mesenteric Anastomosis in Patients with Pancreaticoduodenal Artery Aneurysm Concomitant with Celiac Artery Occlusion using Flow-sensitive Four-dimensional Magnetic Resonance Imaging

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    ObjectivesMany pancreaticoduodenal artery (PDA) aneurysms are associated with celiac artery (CA) stenosis. The pathogenesis of PDA aneurysm may be associated with hemodynamic changes due to CA stenosis/occlusion. The aim of this study was to assess the hemodynamic changes of celiaco-mesenteric anastomosis in patients with PDA aneurysms concomitant with CA occlusion using four-dimensional flow-sensitive magnetic resonance imaging (4D-Flow).Methods4D-Flow was performed preoperatively on five patients. Seven age- and sex-matched individuals were used as controls. Hemodynamic parameters such as flow volume and maximum flow velocity in PDAs, gastroduodenal arteries, common hepatic arteries, and superior mesenteric arteries were compared between both groups. Wall shear stress (WSS) and oscillatory shear index (OSI) were mapped in both groups.ResultsIn the patient group, 4D-Flow identified retrograde flow of both gastroduodenal arteries and common hepatic arteries. Heterogeneous distribution patterns of both WSS and OSI were identified across the entire PDA in the patient group. OSI mapping showed multiple regions with extremely high OSI values (OSI > 0.3) in all patients. All PDA aneurysms, which were surgically resected, were atherosclerotic.Conclusions4D-Flow identified hemodynamic changes in celiaco-mesenteric arteries in patients with PDA aneurysms with concomitant CA occlusion. These hemodynamic changes may be associated with PDA aneurysm formation

    Quantum generalized constant coupling model for geometrically frustrated antiferromagnets

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    A generalized constant coupling approximation for quantum geometrically frustrated antiferromagnets is presented. Starting from a frustrated unit, we introduce the interactions with the surrounding units in terms of an internal effective field which is fixed by a self consistency condition. Results for the static magnetic susceptibility and specific heat are compared with previous results in the framework of this same model for the classical limit. The range of applicability of the model is discussed.Comment: 11 pages, 6 figures, 1 Tables, typeset using RevTeX 4, small correction in Table

    Spectral functions in itinerant electron systems with geometrical frustration

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    The Hubbard model with geometrical frustration is investigated in a metallic phase close to half-filling. We calculate the single particle spectral function for the triangular lattice within dynamical cluster approximation, which is further combined with non-crossing approximation and fluctuation exchange approximation to treat the resulting cluster Anderson model. It is shown that frustration due to non-local correlations suppresses short-range antiferromagnetic fluctuations and thereby assists the formation of heavy quasi-particles near half-filling.Comment: 4 pages, 5 eps figure

    Critical Dynamics of Singlet Excitations in a Frustrated Spin System

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    We construct and analyze a two-dimensional frustrated quantum spin model with plaquette order, in which the low-energy dynamics is controlled by spin singlets. At a critical value of frustration the singlet spectrum becomes gapless, indicating a quantum transition to a phase with dimer order. This T=0 transition belongs to the 3D Ising universality class, while at finite temperature a 2D Ising critical line separates the plaquette and dimerized phases. The magnetic susceptibility has an activated form throughout the phase diagram, whereas the specific heat exhibits a rich structure and a power law dependence on temperature at the quantum critical point. We argue that the novel quantum critical behavior associated with singlet criticality discussed in this work can be relevant to a wide class of quantum spin systems, such as antiferromagnets on Kagome and pyrochlore lattices, where the low-energy excitations are known to be spin singlets, as well as to the CAVO lattice and several recently discovered strongly frustrated square-lattice antiferromagnets.Comment: 5 pages, 5 figures, additional discussion and figure added, to appear in Phys. Rev.

    The behavior of sympatric sea urchin species across an ecosystem state gradient

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    Background In temperate macroalgal forests, sea urchins are considered as a keystone species due to their grazing ability. Given their potential to shape benthic communities, we monitored the habitat use by three sympatric sea urchin species and compared their behaviors in a vegetated habitat (VH) and an adjacent isoyake habitat (IH). Methods We monitored the environmental conditions and sea urchin density along deep and shallow transects of the VH and IH for over a year. The benthic rugosity at both sites were also surveyed. A mark-recapture experiment was conducted on the two most abundant sea urchins, Diadema setosum and Heliocidaris crassispina, to elucidate sea urchin movement patterns and group dynamics. Results We found that exposure to waves was highest at the VH while the IH was sheltered. The deep IH experienced the least amount of light due to high turbidity. Water temperature patterns were similar across sites. The VH benthic topography was more rugose compared to the smoother and silt-covered IH substate. Peak macroalgal bloom occurred three months earlier in IH, but macroalgae persisted longer at the shallow VH. Among the sympatric sea urchins, H. crassispina was most abundant at the shallow VH and was observed in pits and crevices. The most abundant across IH and in the deep VH was D. setosum, preferring either crevices or free-living, depending on hydrodynamic conditions. The least abundant species was D. savignyi, and most often observed in crevices. Small and medium sea urchins were most often observed at the IH site, whereas larger sea urchins were more likely observed at the VH. The mark-recapture study showed that D. setosum was found to displace further at the IH, and H. crassispina was more sedentary. Additionally, D. setosum was always observed in groups, whereas H. crassispina was always solitary. Discussion The behaviors of sympatric urchins, Diadema savignyi, D. setosum and H. crassispina, differed in response to changes in the benthic environment and physical conditions. Sea urchin displacement increased when rugosity and wave action were low. Habitat preference shifted to crevices in seasons with high wave action. In general, the mark-recapture experiment showed that sea urchins displaced further at night
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