437 research outputs found

    Generation of marker- and/or backbone-free transgenic wheat plants via Agrobacterium-mediated transformation

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    Horizontal transfer of antibiotic resistance genes to animals and vertical transfer of herbicide resistance genes to the weedy relatives are perceived as major biosafety concerns in genetically modified (GM) crops. In this study, five novel vectors which used gusA and bar as a reporter gene and a selection marker gene, respectively, were constructed based on the pCLEAN dual binary vector system. Among these vectors, 1G7B and 5G7B carried two T-DNAs located on two respective plasmids with 5G7B possessing an additional virGwt gene. 5LBTG154 and 5TGTB154 carried two T-DNAs in the target plasmid with either one or double right borders, and 5BTG154 carried the selectable marker gene on the backbone outside of the T-DNA left border in the target plasmid. In addition, 5BTG154, 5LBTG154, and 5TGTB154 used pAL154 as a helper plasmid which contains Komari fragment to facilitate transformation. These five dual binary vector combinations were transformed into Agrobacterium strain AGL1 and used to transform durum wheat cv Stewart 63. Evaluation of the co-transformation efficiencies, the frequencies of marker-free transgenic plants, and integration of backbone sequences in the obtained transgenic lines indicated that two vectors (5G7B and 5TGTB154) were more efficient in generating marker-free transgenic wheat plants with no or minimal integration of backbone sequences in the wheat genome. The vector series developed in this study for generation of marker- and/or backbone-free transgenic wheat plants via Agrobacterium-mediated transformation will be useful to facilitate the creation of “clean” GM wheat containing only the foreign genes of agronomic importance

    Study of the expression levels of Hepatocyte nuclear factor 4 alpha and 3 beta in patients with different outcome of HBV infection

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    Hepatocyte nuclear factors 4 alpha (HNF4α) and 3 beta (HNF3ÎČ) are members of a group of liver-enriched transcription factors (LETFs) that play important roles in regulating the replication of hepatitis B virus (HBV) and liver inflammation. However, the relationship of the level of HNF4α and HNF3ÎČ with the severity of HBV-infected liver diseases is unclear. In this study, liver tissue samples from different types of HBV patients were collected, and HNF4α and HNF3ÎČ expression were detected by immunohistochemistry. The expression of HNF4α was significant higher in patients with severe hepatitis B(SHB) than those with chronic hepatitis B(CHB) and liver cirrhosis(LC) (both P < 0.05), but similar between patients with CHB and LC (P > 0.05). And the expression of HNF3ÎČ was similar among patients with CHB, LC and SHB (P > 0.05 for all pairwise comparison). This suggests that the expression level of HNF4α was different in patients with different outcome of HBV infection, high expression level of HNF4α may correlate with occurrence of SH

    ĐœŃ–ĐœŃ–ĐŒŃ–Đ·Đ°Ń†Ń–Ń ĐŸĐżĐŸŃ€Ńƒ ĐżĐ”Ń€ŃĐŸĐœĐ°Đ»Ńƒ ĐŸŃ€ĐłĐ°ĐœŃ–Đ·Đ°Ń†Ń–ĐčĐœĐžĐŒ Đ·ĐŒŃ–ĐœĐ°ĐŒ ĐœĐ° ĐżŃ–ĐŽĐżŃ€ĐžŃ”ĐŒŃŃ‚ĐČі

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    ĐžĐ±Ò‘Ń€ŃƒĐœŃ‚ĐŸĐČĐ°ĐœĐŸ ĐżŃ–ĐŽŃ…ĐŸĐŽĐž ĐŽĐŸ ĐŒŃ–ĐœŃ–ĐŒŃ–Đ·Đ°Ń†Ń–Ń— ĐŸĐżĐŸŃ€Ńƒ ĐżĐ”Ń€ŃĐŸĐœĐ°Đ»Ńƒ ĐŸŃ€ĐłĐ°ĐœŃ–Đ·Đ°Ń†Ń–ĐčĐœĐžĐŒ Đ·ĐŒŃ–ĐœĐ°ĐŒ ĐœĐ° ĐżŃ–ĐŽĐżŃ€ĐžŃ”ĐŒŃŃ‚ĐČі. На ĐŸŃĐœĐŸĐČі Đ°ĐœĐ°Đ»Ń–Đ·Ńƒ ĐœĐ”ĐŽĐŸĐ»Ń–ĐșіĐČ Ń–ŃĐœŃƒŃŽŃ‡ĐžŃ… ĐżŃ–ĐŽŃ…ĐŸĐŽŃ–ĐČ Đ·Đ°ĐżŃ€ĐŸĐżĐŸĐœĐŸĐČĐ°ĐœĐŸ ĐșĐŸĐœŃ†Đ”ĐżŃ‚ŃƒĐ°Đ»ŃŒĐœŃ– ĐżĐŸĐ»ĐŸĐ¶Đ”ĐœĐœŃ ĐŒŃ–ĐœŃ–ĐŒŃ–Đ·Đ°Ń†Ń–Ń— ĐŸĐżĐŸŃ€Ńƒ ĐżĐ”Ń€ŃĐŸĐœĐ°Đ»Ńƒ ĐŸŃ€ĐłĐ°ĐœŃ–Đ·Đ°Ń†Ń–ĐčĐœĐžĐŒ Đ·ĐŒŃ–ĐœĐ°ĐŒ ĐœĐ° ĐżŃ–ĐŽĐżŃ€ĐžŃ”ĐŒŃŃ‚ĐČах, у Ń€Đ°ĐŒĐșах рДалізації яĐșох Ń€ĐŸĐ·Ń€ĐŸĐ±Đ»Đ”ĐœĐŸ піЮхіЮ ĐŽĐŸ ĐŸŃ†Ń–ĐœĐșĐž ріĐČĐœŃ ĐżŃ–ĐŽŃ‚Ń€ĐžĐŒĐșĐž ĐŸŃ€ĐłĐ°ĐœŃ–Đ·Đ°Ń†Ń–ĐčĐœĐžŃ… Đ·ĐŒŃ–Đœ у ĐșĐŸĐ»Đ”ĐșтоĐČі ĐżŃ–ŃĐ»Ń Ń–ĐœŃ„ĐŸŃ€ĐŒĐ°Ń†Ń–ĐčĐœĐŸŃ— ĐČĐ·Đ°Ń”ĐŒĐŸĐŽŃ–Ń— ĐŒŃ–Đ¶ спіĐČŃ€ĐŸĐ±Ń–Ń‚ĐœĐžĐșĐ°ĐŒĐž та піЮхіЮ ĐŽĐŸ проĐčĐœŃŃ‚Ń‚Ń Ń€Ń–ŃˆĐ”ĐœŃŒ у сфДрі упраĐČĐ»Ń–ĐœĐœŃ ĐŒŃ–ĐœŃ–ĐŒŃ–Đ·Đ°Ń†Ń–Ń”ŃŽ ĐŸĐżĐŸŃ€Ńƒ ĐżĐ”Ń€ŃĐŸĐœĐ°Đ»Ńƒ ĐŸŃ€ĐłĐ°ĐœŃ–Đ·Đ°Ń†Ń–ĐčĐœĐžĐŒ Đ·ĐŒŃ–ĐœĐ°ĐŒ ĐœĐ° ĐżŃ–ĐŽĐżŃ€ĐžŃ”ĐŒŃŃ‚ĐČі, Ń‰ĐŸ Đ±Đ°Đ·ŃƒŃ”Ń‚ŃŒŃŃ ĐœĐ° ĐŸĐżŃ‚ĐžĐŒŃ–Đ·Đ°Ń†Ń–ĐčĐœŃ–Đč ĐŒĐŸĐŽĐ”Đ»Ń– ĐČĐžĐ±ĐŸŃ€Ńƒ ĐŸĐżŃ‚ĐžĐŒĐ°Đ»ŃŒĐœĐžŃ… Ń€Ń–ŃˆĐ”ĐœŃŒ. ЗЮіĐčŃĐœĐ”ĐœĐŸ праĐșŃ‚ĐžŃ‡ĐœŃƒ Đ°ĐżŃ€ĐŸĐ±Đ°Ń†Ń–ŃŽ Đ·Đ°ĐżŃ€ĐŸĐżĐŸĐœĐŸĐČĐ°ĐœĐžŃ… ĐżŃ–ĐŽŃ…ĐŸĐŽŃ–ĐČ ĐœĐ° ĐŽŃ–ŃŽŃ‡ĐŸĐŒŃƒ ĐżŃ€ĐŸĐŒĐžŃĐ»ĐŸĐČĐŸĐŒŃƒ ĐżŃ–ĐŽĐżŃ€ĐžŃ”ĐŒŃŃ‚ĐČі та ŃŃ„ĐŸŃ€ĐŒŃƒĐ»ŃŒĐŸĐČĐ°ĐœĐŸ пДрспДĐșтоĐČĐž ĐżĐŸĐŽĐ°Đ»ŃŒŃˆĐžŃ… ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœŃŒ.ĐžĐ±ĐŸŃĐœĐŸĐČĐ°ĐœŃ‹ ĐżĐŸĐŽŃ…ĐŸĐŽŃ‹ Đș ĐŒĐžĐœĐžĐŒĐžĐ·Đ°Ń†ĐžĐž ŃĐŸĐżŃ€ĐŸŃ‚ĐžĐČĐ»Đ”ĐœĐžŃ ĐżĐ”Ń€ŃĐŸĐœĐ°Đ»Đ° ĐŸŃ€ĐłĐ°ĐœĐžĐ·Đ°Ń†ĐžĐŸĐœĐœŃ‹ĐŒ ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžŃĐŒ ĐœĐ° ĐżŃ€Đ”ĐŽĐżŃ€ĐžŃŃ‚ĐžĐž. На ĐŸŃĐœĐŸĐČĐ” Đ°ĐœĐ°Đ»ĐžĐ·Đ° ĐœĐ”ĐŽĐŸŃŃ‚Đ°Ń‚ĐșĐŸĐČ ŃŃƒŃ‰Đ”ŃŃ‚ĐČующох ĐżĐŸĐŽŃ…ĐŸĐŽĐŸĐČ ĐżŃ€Đ”ĐŽĐ»ĐŸĐ¶Đ”ĐœŃ‹ ĐșĐŸĐœŃ†Đ”ĐżŃ‚ŃƒĐ°Đ»ŃŒĐœŃ‹Đ” ĐżĐŸĐ»ĐŸĐ¶Đ”ĐœĐžŃ ĐŒĐžĐœĐžĐŒĐžĐ·Đ°Ń†ĐžĐž ŃĐŸĐżŃ€ĐŸŃ‚ĐžĐČĐ»Đ”ĐœĐžŃ ĐżĐ”Ń€ŃĐŸĐœĐ°Đ»Đ° ĐŸŃ€ĐłĐ°ĐœĐžĐ·Đ°Ń†ĐžĐŸĐœĐœŃ‹ĐŒ ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžŃĐŒ ĐœĐ° ĐżŃ€Đ”ĐŽĐżŃ€ĐžŃŃ‚ĐžŃŃ…, ĐČ Ń€Đ°ĐŒĐșах рДалОзацОО ĐșĐŸŃ‚ĐŸŃ€Ń‹Ń… Ń€Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚Đ°ĐœŃ‹ ĐżĐŸĐŽŃ…ĐŸĐŽ Đș ĐŸŃ†Đ”ĐœĐșĐ” ŃƒŃ€ĐŸĐČĐœŃ ĐżĐŸĐŽĐŽĐ”Ń€Đ¶ĐșĐž ĐŸŃ€ĐłĐ°ĐœĐžĐ·Đ°Ń†ĐžĐŸĐœĐœŃ‹Ń… ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžĐč ĐČ ĐșĐŸĐ»Đ»Đ”ĐșтоĐČĐ” ĐżĐŸŃĐ»Đ” ĐžĐœŃ„ĐŸŃ€ĐŒĐ°Ń†ĐžĐŸĐœĐœĐŸĐłĐŸ ĐČĐ·Đ°ĐžĐŒĐŸĐŽĐ”ĐčстĐČоя ĐŒĐ”Đ¶ĐŽŃƒ ŃĐŸŃ‚Ń€ŃƒĐŽĐœĐžĐșĐ°ĐŒĐž Đž ĐżĐŸĐŽŃ…ĐŸĐŽ Đș ĐżŃ€ĐžĐœŃŃ‚ĐžŃŽ Ń€Đ”ŃˆĐ”ĐœĐžĐč ĐČ ŃŃ„Đ”Ń€Đ” упраĐČĐ»Đ”ĐœĐžŃ ĐŒĐžĐœĐžĐŒĐžĐ·Đ°Ń†ĐžĐ”Đč ŃĐŸĐżŃ€ĐŸŃ‚ĐžĐČĐ»Đ”ĐœĐžŃ ĐżĐ”Ń€ŃĐŸĐœĐ°Đ»Đ° ĐŸŃ€ĐłĐ°ĐœĐžĐ·Đ°Ń†ĐžĐŸĐœĐœŃ‹ĐŒ ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžŃĐŒ ĐœĐ° ĐżŃ€Đ”ĐŽĐżŃ€ĐžŃŃ‚ĐžĐž, Đ±Đ°Đ·ĐžŃ€ŃƒŃŽŃ‰ĐžĐčся ĐœĐ° ĐŸĐżŃ‚ĐžĐŒĐžĐ·Đ°Ń†ĐžĐŸĐœĐœĐŸĐč ĐŒĐŸĐŽĐ”Đ»Đž ĐČŃ‹Đ±ĐŸŃ€Đ° ĐŸĐżŃ‚ĐžĐŒĐ°Đ»ŃŒĐœŃ‹Ń… Ń€Đ”ŃˆĐ”ĐœĐžĐč. ĐžŃŃƒŃ‰Đ”ŃŃ‚ĐČĐ»Đ”ĐœĐ° праĐșтОчДсĐșая Đ°ĐżŃ€ĐŸĐ±Đ°Ń†ĐžŃ ĐżŃ€Đ”ĐŽĐ»ĐŸĐ¶Đ”ĐœĐœŃ‹Ń… ĐżĐŸĐŽŃ…ĐŸĐŽĐŸĐČ ĐœĐ° ĐŽĐ”ĐčстĐČŃƒŃŽŃ‰Đ”ĐŒ ĐżŃ€ĐŸĐŒŃ‹ŃˆĐ»Đ”ĐœĐœĐŸĐŒ ĐżŃ€Đ”ĐŽĐżŃ€ĐžŃŃ‚ĐžĐž Đž ŃŃ„ĐŸŃ€ĐŒŃƒĐ»ĐžŃ€ĐŸĐČĐ°ĐœŃ‹ пДрспДĐșтоĐČы ĐŽĐ°Đ»ŃŒĐœĐ”Đčшох ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč.The article is devoted to substantiating the approaches to minimizing the resistance of staff to organizational changes at an enterprise. It was revealed that existing scientific approaches do not allow formalizing the assessment of organizational resistance and minimizing the costs of preventing organizational resistance; they do not take into account such important factors as the authority of the members of the staff, objective benefits of a decision for the staff members and their inclination to adopt other people’s opinions. They do not allow assessing the staff members support for organizational change taking into account the information interaction between them. Based on the analysis of the shortcomings of existing approaches conceptual positions to minimizing the resistance of staff to organizational changes at enterprises were proposed, as part of which an approach was developed to assessing the level of support for organizational changes by the staff after the information interaction between the staff members, as well as an approach to managing the minimization of staff resistance to organizational changes at an enterprise based on the optimization model of optimal (in terms of cost and results) decisions. In terms of decision-making, the main task is the choice of optimal measures (interventions) that work through changing the objective benefits of the decisions and the initial level of support. A practical approbation of the proposed approaches at an existing industrial enterprise was carried out, and perspectives for further research were formulated. Prospects for further research are in the development of tools for minimizing organizational resistance and developing methods for assessing the characteristics of workers

    Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV

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    The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≄20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≀pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≀{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration

    Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector

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    The inclusive and dijet production cross-sections have been measured for jets containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The measurements use data corresponding to an integrated luminosity of 34 pb^-1. The b-jets are identified using either a lifetime-based method, where secondary decay vertices of b-hadrons in jets are reconstructed using information from the tracking detectors, or a muon-based method where the presence of a muon is used to identify semileptonic decays of b-hadrons inside jets. The inclusive b-jet cross-section is measured as a function of transverse momentum in the range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet cross-section is measured as a function of the dijet invariant mass in the range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets and the angular variable chi in two dijet mass regions. The results are compared with next-to-leading-order QCD predictions. Good agreement is observed between the measured cross-sections and the predictions obtained using POWHEG + Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet cross-section. However, it does not reproduce the measured inclusive cross-section well, particularly for central b-jets with large transverse momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final version published in European Physical Journal

    Single hadron response measurement and calorimeter jet energy scale uncertainty with the ATLAS detector at the LHC

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    The uncertainty on the calorimeter energy response to jets of particles is derived for the ATLAS experiment at the Large Hadron Collider (LHC). First, the calorimeter response to single isolated charged hadrons is measured and compared to the Monte Carlo simulation using proton-proton collisions at centre-of-mass energies of sqrt(s) = 900 GeV and 7 TeV collected during 2009 and 2010. Then, using the decay of K_s and Lambda particles, the calorimeter response to specific types of particles (positively and negatively charged pions, protons, and anti-protons) is measured and compared to the Monte Carlo predictions. Finally, the jet energy scale uncertainty is determined by propagating the response uncertainty for single charged and neutral particles to jets. The response uncertainty is 2-5% for central isolated hadrons and 1-3% for the final calorimeter jet energy scale.Comment: 24 pages plus author list (36 pages total), 23 figures, 1 table, submitted to European Physical Journal

    Search for displaced vertices arising from decays of new heavy particles in 7 TeV pp collisions at ATLAS

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    We present the results of a search for new, heavy particles that decay at a significant distance from their production point into a final state containing charged hadrons in association with a high-momentum muon. The search is conducted in a pp-collision data sample with a center-of-mass energy of 7 TeV and an integrated luminosity of 33 pb^-1 collected in 2010 by the ATLAS detector operating at the Large Hadron Collider. Production of such particles is expected in various scenarios of physics beyond the standard model. We observe no signal and place limits on the production cross-section of supersymmetric particles in an R-parity-violating scenario as a function of the neutralino lifetime. Limits are presented for different squark and neutralino masses, enabling extension of the limits to a variety of other models.Comment: 8 pages plus author list (20 pages total), 8 figures, 1 table, final version to appear in Physics Letters

    Measurement of the polarisation of W bosons produced with large transverse momentum in pp collisions at sqrt(s) = 7 TeV with the ATLAS experiment

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    This paper describes an analysis of the angular distribution of W->enu and W->munu decays, using data from pp collisions at sqrt(s) = 7 TeV recorded with the ATLAS detector at the LHC in 2010, corresponding to an integrated luminosity of about 35 pb^-1. Using the decay lepton transverse momentum and the missing transverse energy, the W decay angular distribution projected onto the transverse plane is obtained and analysed in terms of helicity fractions f0, fL and fR over two ranges of W transverse momentum (ptw): 35 < ptw < 50 GeV and ptw > 50 GeV. Good agreement is found with theoretical predictions. For ptw > 50 GeV, the values of f0 and fL-fR, averaged over charge and lepton flavour, are measured to be : f0 = 0.127 +/- 0.030 +/- 0.108 and fL-fR = 0.252 +/- 0.017 +/- 0.030, where the first uncertainties are statistical, and the second include all systematic effects.Comment: 19 pages plus author list (34 pages total), 9 figures, 11 tables, revised author list, matches European Journal of Physics C versio
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