9 research outputs found
IpgB1 and IpgB2, two homologous effectors secreted via the Mxi-Spa type III secretion apparatus, cooperate to mediate polarized cell invasion and inflammatory potential of Shigella flexenri.
Type III secretion systems (T3SS) are present in many pathogenic gram-negative bacteria and mediate the translocation of bacterial effector proteins into host cells. Here, we report the phenotypic characterization of S. flexneri ipgB1 and ipgB2 mutants, in which the genes encoding the IpgB1 and IpgB2 effectors have been inactivated, either independently or simultaneously. Like IpgB1, we found that IpgB2 is secreted by the T3SS and its secretion requires the Spa15 chaperone. Upon infection of semi-confluent HeLa cells, the ipgB2 mutant exhibited the same invasive capacity as the wild-type strain and the ipgB1 mutant was 50% less invasive. Upon infection of polarised Caco2-cells, the ipgB2 mutant did not show a significant defect in invasion and the ipgB1 mutant was slightly more invasive than the wild-type strain. Entry of the ipgB1 ipgB2 mutant in polarized cells was reduced by 70% compared to the wild-type strain. Upon infection of the cornea in Guinea pigs, the ipgB2 mutant exhibited a wild-type phenotype, the ipgB1 mutant was hypervirulent and elicited a more pronounced proinflammatory response, while the ipgB1 ipgB2 mutant was highly attenuated. The attenuated phenotype of the ipgB1 ipgB2 mutant was confirmed using a murine pulmonary model of infection and histopathology and immunochemistry studies.Journal ArticleResearch Support, Non-U.S. Gov'tSCOPUS: ar.jinfo:eu-repo/semantics/publishe
Cardiopulmonary values and organ blood flows before and during heat stress: data in nine subjects at rest in the upright position
Physiological changes associated with thermoregulation can influence the kinetics of chemicals in the human body, such as alveolar ventilation (VA) and redistribution of blood flow to organs. In this study, the influence of heat stress on various physiological parameters was evaluated in nine male volunteers during sessions of exposure to wet blub globe temperatures (WBGT) of 21, 25 and 30C for four hours. Skin and core temperatures and more than twenty cardiopulmonary parameters were measured. Liver, kidneys, brain, skin and muscles blood flows were also determined based on published measurements. Results show that most subjects (8 out of 9) have been affected by the inhalation of hot and dry air at the WBGT of 30C. High respiratory rates, superficial tidal volumes and low VA values were notably observed. The skin blood flow has increased by 2.16-fold, whereas the renal blood flow and liver blood flow have decreased by about by 11 and 18% respectively. A complete set of key cardiopulmonary parameters in healthy male adults before and during heat stress was generated for use in PBPK modeling. A toxicokinetic studies are ongoing to evaluate the impact of heat stress on the absorption, biotransformation and excretion rates of volatile xenobiotics.The presentation of the authors' names and (or) special characters in the title of the pdf file of the accepted manuscript may differ slightly from what is displayed on the item page. The information in the pdf file of the accepted manuscript reflects the original submission by the author
Ectopic expression of pRB2/p130 suppresses the tumorigenicity of the c-erb-2-overexpressing SKOV3 tumor cell line
We investigated the in vitro and in vivo effects of the ectopic expression of the pRb2/p130 cell cycle regulator on c-erB-2-associated tumorigenicity. SKOV3 ovarian cancer cells, which display c-erB-2 gene amplification and oncoprotein (p185(HER2)) overexpression, were stably transfected with a plasmid containing the coding sequence for human wild-type pRb2/p130 (wtRb2), or with pcDNA3 empty vector. Three wtRb2-transfected clones (cl. 24, cl. 49, cl. 100) and one empty vector-transfected clone (cl. mock) were randomly picked and further analysed. Western blot analysis revealed high levels of pRb2/p130 in the three clones compared to mock cells. Levels of p185(HER2) and the extent of its tyrosine phosphorylation were similar in all transfectant clones, as were levels of pRb1 and p107. In anchorage-independent growth assays, the number of colonies from wtRb2 clone-transfectants was about 90% less than that arising from mock cells (P < 0.001). Tumor take rates of the three wtRb2-transfected clones xenografted in nu/nu mice were much lower than those of mock cells, and tumor was decreased by 80% (P < 0.001). A volume mutant version of pRb2/p130 deleted of the pocket region (mut-Rb2) was also transfected into SKOV3 cells and studied in parallel with the wtRb2-transfected and pcDNA empty vector-transfected bulk populations. mutRb2 transfected cells showed no inhibition of in vitro colony formation and were fully tumorigenic. Together, these findings indicate that Rb2 acts as a tumor suppressor gene in vivo and in vitro in SKOV3 cells and that the intact pocket region is required for the suppressor activity
Antibody response after vaccination with antigen-pulsed dendritic cells
Dendritic cells (DCs) are the most potent antigen-presenting cells of the immune system capable of initiating immune responses to antigens. It is also well documented that cancer patients often experience anergy against tumor antigens. In this study we selected the best protocol for inducing the production of antibodies against the HER2 oncoprotein using DCs to overcome anergy. Murine DCs were pulsed in vitro, using different protocols, with recombinant HER2 fused to a human Fc (in order to improve DC antigen uptake) and were used to vaccinate mice. The obtained results indicate that antigen-pulsed DCs can induce an antibody response and that adding CpG after antigen pulsing greatly increases anti-HER2 antibody production
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Intercomparison on the usage of computational codes in radiation dosimetry
International audience'QUADOS', a Concerted Action of the European Commission, has run an intercomparison aimed at evaluating the use of computational codes for dosimetry in radiation protection and medical physics. This intercomparison was open to all users of Monte Carlo, analytic and semi-analytic codes or deterministic methods. Its main aim was to provide a snapshot of the methods and codes currently in use. It also intended to furnish information on the methods used to assess the reliability of computational results and disseminate 'good practice' throughout the radiation dosimetry community. Eight problems were selected for their relevance to the radiation dosimetry community, three of which involve neutron transport. This paper focuses on the analysis of the neutron problems. © Oxford University Press 2004; all rights reserved
Magnetic And Structural Properties Of Fcc/hcp Bi-crystalline Multilayer Co Nanowire Arrays Prepared By Controlled Electroplating
We report on the structural and magnetic properties of crystalline bi-phase Co nanowires, electrodeposited into the pores of anodized alumina membranes, as a function of their length. Co nanowires present two different coexistent crystalline structures (fcc and hcp) that can be controlled by the time of pulsed electrodeposition. The fcc crystalline phase grows at the early stage and is present at the bottom of all the nanowires, strongly influencing their magnetic behavior. Both structural and magnetic characterizations indicate that the length of the fcc phase is constant at around 260-270 nm. X-ray diffraction measurements revealed a strong preferential orientation (texture) in the (1 0-1 0) direction for the hcp phase, which increases the nanowire length as well as crystalline grain size, degree of orientation, and volume fraction of oriented material. The first-order reversal curve (FORC) method was used to infer both qualitatively and quantitatively the complex magnetization reversal of the nanowires. Under the application of a magnetic field parallel to the wires, the magnetization reversal of each region is clearly distinguishable; the fcc phase creates a high coercive contribution without an interaction field, while the hcp phase presents a smaller coercivity and undergoes a strong antiparallel interaction field from neighboring wires. © 2011 American Institute of Physics.1098Routkevitch, D., Tager, A.A., Haruyama, J., Almawlawi, D., Moskovits, M., Xu, J.M., (1996) IEEE Trans. Electron Devices, 43, p. 1646. , 10.1109/16.536810Ross, C.A., Patterned magnetic recording media (2001) Annual Review of Materials Science, 31, pp. 203-235. , DOI 10.1146/annurev.matsci.31.1.203Zhong, Z., Wang, D., Cui, Y., Bockrath, M.W., Lieber, C.H., Nanowire Crossbar Arrays as Address Decoders for Integrated Nanosystems (2003) Science, 302 (5649), pp. 1377-1379. , DOI 10.1126/science.1090899Ono, T., Miyajima, H., Shigeto, K., Mibu, K., Hosoito, N., Shinjo, T., Propagation of a magnetic domain wall in a submicrometer magnetic wire (1999) Science, 284 (5413), pp. 468-470. , DOI 10.1126/science.284.5413.468Atkinson, D., Allwood, D.A., Xiong, G., Cooke, M.D., Faulkner, C.C., Cowburn, R.P., (2003) Nature Mater., 2, p. 85. , 10.1038/nmat803Beach, G.S.D., Nistor, C., Knutson, C., Tsoi, M., Erskine, J.L., Dynamics of field-driven domain-wall propagation in ferromagnetic nanowires (2005) Nature Materials, 4 (10), pp. 741-744. , DOI 10.1038/nmat1477Cowburn, R., Petit, D., Spintronics: Turbulence ahead (2005) Nature Materials, 4 (10), pp. 721-722. , DOI 10.1038/nmat1503Hernandez-Velez, M., Pirota, K.R., Paszti, F., Navas, D., Climent, A., Vazquez, M., Magnetic nanowire arrays in anodic alumina membranes: Rutherford backscattering characterization (2005) Applied Physics A: Materials Science and Processing, 80 (8), pp. 1701-1706. , DOI 10.1007/s00339-005-3234-0Nielsch, K., Wehrspohn, R.B., Barthel, J., Kirschner, J., Gosele, U., Fischer, S.F., Kronmuller, H., (2001) Appl. Phys. Lett., 79, p. 1360. , 10.1063/1.1399006Nielsch, K., Wehrspohn, R.B., Barthel, J., Kirschner, J., Fischer, S.F., Kronmuller, H., Schweinbock, T., Gosele, U., High density hexagonal nickel nanowire array (2002) Journal of Magnetism and Magnetic Materials, 249 (1-2), pp. 234-240. , DOI 10.1016/S0304-8853(02)00536-X, PII S030488530200536XSellmyer, D.J., Zheng, M., Skomski, R., Magnetism of FE, CO and NI nanowires in self-assembled arrays (2001) Journal of Physics Condensed Matter, 13 (25), pp. R433-R460. , DOI 10.1088/0953-8984/13/25/201, PII S0953898401201581Metzger, R.M., Konovalov, V.V., Sun, M., Xu, T., Zangari, G., Xu, B., Benakli, M., Doyle, W.D., (2000) IEEE Trans. Magn., 36, p. 30. , 10.1109/20.824421Ferré, R., Ounadjela, K., George, J.M., Piraux, L., Dubois, S., (1997) Phys. Rev. B, 56, p. 14066. , 10.1103/PhysRevB.56.14066Budendorff, J.L., Mény, C., Beaurepaire, E., Panissod, P., Bucher, J.P., (2000) Eur. Phys. J. 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Nanosci. Nanotechnol., 8, p. 2944. , 10.1166/jnn.2008.159Béron, F., Carignan, L.-P., Ménard, D., Yelon, A., (2010) Electrodeposited Nanowires and Their Applications, , edited by N. Lupu (IN-TECH, Vienna)Beron, F., Clime, L., Ciureanu, M., Menard, D., Cochrane, R.W., Yelon, A., Reversible and quasireversible information in first-order reversal curve diagrams (2007) Journal of Applied Physics, 101 (9), pp. 09J107. , DOI 10.1063/1.271217
A Novel Method For Identifying The Local Magnetic Viscosity Process Of Heterogeneous Magnetic Nanostructures
The relaxation mechanism known as magnetic viscosity has been attracting the attention of the scientific community for more than seven decades. However, a complete model to fully describe the phenomenon is difficult to achieve, owing to its possible different sources and microscopic mechanisms. This work proposes a new experimental approach, based on the combination of static and dynamic first-order reversal curve diagrams. With this technique, one can decouple the responsible mechanism presented by different phases of an inhomogeneous magnetic sample. Moreover, it can also be used to distinguish the microscopic origin of magnetic viscosity (i.e. eddy currents or thermal activation). We successfully applied this novel approach to characterize the local viscosity processes occurring in a nanocrystalline Fe-based soft magnetic ribbon. Owing to the generality of its principles, it can be used to investigate the viscosity of a wide range of systems. © 2013 IOP Publishing Ltd.464Kazantseva, N., Hinzke, D., Nowak, U., Chantrell, R.W., Atxitia, U., Chubykalo-Fesenko, O., (2008) Phys. Rev., 77 (18). , 10.1103/PhysRevB.77.184428 1098-0121 B 184428Suzuki, I.S., Suzuki, M., (2008) Phys. Rev., 78 (21). , 10.1103/PhysRevB.78.214404 1098-0121 B 214404Anand, V.K., Adroja, D.T., Hillier, A.D., (2012) Phys. Rev., 85 (1). , 10.1103/PhysRevB.85.014418 1098-0121 B 014418Suzuki, M., Fullem, S.I., Suzuki, I.S., Wang, L., Zhong, C.-J., (2009) Phys. Rev., 79 (2). , 10.1103/PhysRevB.79.024418 1098-0121 B 024418Titov, S.V., Déjardin, P.-M., El Mrabti, H., Kalmykov, Y.P., (2010) Phys. Rev., 82. , B 100413(R)De Oliveira, L.A.S., Sinnecker, J.P., Vieira, M.D., Pentón-Madrigal, A., (2010) J. Appl. Phys., 107 (9). , 10.1063/1.3362927 0021-8979 09D907Kesserwan, H., Manfredi, G., Bigot, J.-Y., Hervieux, P.A., (2011) Phys. 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