1000 resultados para 8-69
Resumo:
[Excerpt] The purine core is a privileged scaffold in medicinal chemistry and the biological relevance of purine derivatives makes them attractive targets in the preparation of combinatorial libraries.1,2 In particular, there is a great interest in the synthesis of 8-substituted purines due to their important potential as antiviral and anticancer agents.3 Reports on 8-aminopurines are limited and general methods to obtain these purine derivatives are still needed.4 Cyclic amines and hydrazines are key structural motifs in various bioactive agents.5 Here we report a novel, efficient and inexpensive method for the synthesis of 6,8-diaminopurines 4 incorporating cycloalkylamino substituents at N3position of the purine ring. (...)
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[Excerpt] Purine nucleobases are fundamental biochemicals in living organisms. They have been a valuable inspiration for drug design once they play several key roles in the cell.1 To the best of our knowledge, reported routes to 8-aminopurines are still scarce due to the difficulty in introducing amino groups in this position of the purine ring. Here we report a novel, inexpensive and facile synthetic method to generate N3,N6-disubstituted-6,8-diaminopurines. In our research group, a number of substituted purines have been obtained from a common imidazole precursor, the 5-amino-4-cyanoformimidoyl imidazole 1. Recently, a comprehensive study on the reactivity of imidazoles 1 with nucleophiles under acidic conditions led us to develop experimental methods to incorporate primary amines into the cyanoformimidoyl group.2 (...)
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Os frutos do açaizeiro (Euterpe precatoria Mart.) procedentes de diferentes ecossistemas amazônicos foram processados para a obtenção de suco. O produto foi avaliado quanto à composição centesimal (umidade, cinzas, lipídeos, proteína, glicídios e fibra alimentar), minerais, ácidos graxos e antocianinas. Os frutos foram comparados quanto ao peso, constatando-se uma variação significativa de 1,1 a 2,0 g entre eles. Com relação ao suco, verificou-se baixa concentração de proteína e alto teor de energia devido, principalmente, à presença de lipídeos cuja concentração variou de 4,24 a 9,74%. Dentre os minerais, o potássio foi o mais abundante com teores na faixa de 73,78 a 376,69 mg 100 g-¹ (do suco), seguido do cálcio (15,99 a 57,85 mg 100g-¹). O ferro foi encontrado em concentrações minoritárias, na ordem de 0,43 a 1,2 mg 100g-¹. Com relação aos ingredientes funcionais, o suco de açaí apresentou concentrações importantes de fibra alimentar (2,37 a 7,8%), e antocianinas, variando de 128,4 mg 100 g-¹ , nos frutos de coloração verde, procedentes de Parintins, até 868,9 mg 100 g-¹ nas amostras de Manaquiri (base seca). Na fração lipídica, destacou-se ainda a presença do ácido graxo oleico (18:1), com porcentagem média de 68,2% no total de ácidos graxos, seguido do ácido palmítico (16:0) com 17,5%. Tais resultados reforçam o potencial do açaí como fonte de energia, lipídeos, fibra alimentar, antocianinas, ácido graxo monoinsaturado e minerais. O presente estudo irá contribuir para a ampliação da tabela de composição química de alimentos e, consequentemente, auxiliar nos programas de melhoramento genético, mercado e inclusão social.
Resumo:
A search for flavour-changing neutral current decays of a top quark to an uptype quark (q = u, c) and the Standard Model Higgs boson, where the Higgs boson decays to bb¯¯, is presented. The analysis searches for top quark pair events in which one top quark decays to Wb, with the W boson decaying leptonically, and the other top quark decays to Hq. The search is based on pp collisions at s√=8 TeV recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider and uses an integrated luminosity of 20.3 fb−1. Data are analysed in the lepton-plus-jets final state, characterised by an isolated electron or muon and at least four jets. The search exploits the high multiplicity of b-quark jets characteristic of signal events, and employs a likelihood discriminant that uses the kinematic differences between the signal and the background, which is dominated by tt¯→WbWb decays. No significant excess of events above the background expectation is found, and observed (expected) 95% CL upper limits of 0.56% (0.42%) and 0.61% (0.64%) are derived for the t → Hc and t → Hu branching ratios respectively. The combination of this search with other ATLAS searches in the H → γγ and H → WW *, ττ decay modes significantly improves the sensitivity, yielding observed (expected) 95% CL upper limits on the t → Hc and t → Hu branching ratios of 0.46% (0.25%) and 0.45% (0.29%) respectively. The corresponding combined observed (expected) upper limits on the |λ tcH | and |λ tuH | couplings are 0.13 (0.10) and 0.13 (0.10) respectively. These are the most restrictive direct bounds on tqH interactions measured so far.
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An analysis is presented of events containing jets including at least one b-tagged jet, sizeable missing transverse momentum, and at least two leptons including a pair of the same electric charge, with the scalar sum of the jet and lepton transverse momenta being large. A data sample with an integrated luminosity of 20.3 fb−1 of pp collisions at s√=8 TeV recorded by the ATLAS detector at the Large Hadron Collider is used. Standard Model processes rarely produce these final states, but there are several models of physics beyond the Standard Model that predict an enhanced rate of production of such events; the ones considered here are production of vector-like quarks, enhanced four-top-quark production, pair production of chiral b′-quarks, and production of two positively charged top quarks. Eleven signal regions are defined; subsets of these regions are combined when searching for each class of models. In the three signal regions primarily sensitive to positively charged top quark pair production, the data yield is consistent with the background expectation. There are more data events than expected from background in the set of eight signal regions defined for searching for vector-like quarks and chiral b′-quarks, but the significance of the discrepancy is less than two standard deviations. The discrepancy reaches 2.5 standard deviations in the set of five signal regions defined for searching for four-top-quark production. The results are used to set 95% CL limits on various models.
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The production cross sections of top-quark pairs in association with massive vector bosons have been measured using data from pp collisions at s√=8 TeV. The dataset corresponds to an integrated luminosity of 20.3 fb−1 collected by the ATLAS detector in 2012 at the LHC. Final states with two, three or four leptons are considered. A fit to the data considering the tt¯W and tt¯Z processes simultaneously yields a significance of 5.0σ (4.2σ) over the background-only hypothesis for tt¯W (tt¯Z) production. The measured cross sections are σtt¯W=369+100−91 fb and σtt¯Z=176+58−52 fb. The background-only hypothesis with neither tt¯W nor tt¯Z production is excluded at 7.1σ. All measurements are consistent with next-to-leading-order calculations for the tt¯W and tt¯Z processes.
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A search for new particles that decay into top quark pairs is reported. The search is performed with the ATLAS experiment at the LHC using an integrated luminosity of 20.3 fb−1 of proton-proton collision data collected at a centre-of-mass energy of s√=8 TeV. The lepton-plus-jets final state is used, where the top pair decays to W+bW−b¯¯, with one W boson decaying leptonically and the other hadronically. The invariant mass spectrum of top quark pairs is examined for local excesses or deficits that are inconsistent with the Standard Model predictions. No evidence for a top quark pair resonance is found, and 95% confidence-level limits on the production rate are determined for massive states in benchmark models. The upper limits on the cross-section times branching ratio of a narrow Z′ boson decaying to top pairs range from 4.2 pb to 0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A narrow leptophobic topcolour Z′ boson with mass below 1.8 TeV is excluded. Upper limits are set on the cross-section times branching ratio for a broad colour-octet resonance with Γ/m = 15% decaying to tt¯. These range from 4.8 pb to 0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein excitation of the gluon in a Randall-Sundrum model is excluded for masses below 2.2 TeV.
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A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the s√=8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis. Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models. In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions.
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The distribution and orientation of energy inside jets is predicted to be an experimental handle on colour connections between the hard--scatter quarks and gluons initiating the jets. This Letter presents a measurement of the distribution of one such variable, the jet pull angle. The pull angle is measured for jets produced in tt¯ events with one W boson decaying leptonically and the other decaying to jets using 20.3 fb−1 of data recorded with the ATLAS detector at a centre--of--mass energy of s√=8 TeV at the LHC. The jet pull angle distribution is corrected for detector resolution and acceptance effects and is compared to various models.
Resumo:
Many extensions of the Standard Model predict the existence of charged heavy long-lived particles, such as R-hadrons or charginos. These particles, if produced at the Large Hadron Collider, should be moving non-relativistically and are therefore identifiable through the measurement of an anomalously large specific energy loss in the ATLAS pixel detector. Measuring heavy long-lived particles through their track parameters in the vicinity of the interaction vertex provides sensitivity to metastable particles with lifetimes from 0.6 ns to 30 ns. A search for such particles with the ATLAS detector at the Large Hadron Collider is presented, based on a data sample corresponding to an integrated luminosity of 18.4 fb−1 of pp collisions at s√ = 8 TeV. No significant deviation from the Standard Model background expectation is observed, and lifetime-dependent upper limits on R-hadrons and chargino production are set. Gluino R-hadrons with 10 ns lifetime and masses up to 1185 GeV are excluded at 95% confidence level, and so are charginos with 15 ns lifetime and masses up to 482 GeV.
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A search is presented for photonic signatures motivated by generalised models of gauge-mediated supersymmetry breaking. This search makes use of 20.3 fb−1 of proton-proton collision data at s√=8 TeV recorded by the ATLAS detector at the LHC, and explores models dominated by both strong and electroweak production of supersymmetric partner states. Four experimental signatures incorporating an isolated photon and significant missing transverse momentum are explored. These signatures include events with an additional photon, lepton, b-quark jet, or jet activity not associated with any specific underlying quark flavor. No significant excess of events is observed above the Standard Model prediction and model-dependent 95% confidence-level exclusion limits are set.
Resumo:
Searches for both resonant and non-resonant Higgs boson pair production are performed in the hh→bbττ,γγWW∗ final states using 20.3 fb−1 of pp collision data at a center-of-mass energy of 8 TeV recorded with the ATLAS detector at the Large Hadron Collider. No evidence of their production is observed and 95% confidence level upper limits on the production cross sections are set. These results are then combined with the published results of the hh→γγbb,bbbb analyses. An upper limit of 0.69 (0.47) pb on the non-resonant Standard Model like hh production is observed (expected), corresponding to 70 (48) times of the SM gg→hh cross section. For production via narrow resonances, cross section limits of hh production from a heavy Higgs boson decay are set as a function of the heavy Higgs boson mass. The observed (expected) limits range from 2.1 (1.1) pb at 260 GeV to 0.011 (0.018) pb at 1000 GeV. These results are interpreted in the context of two simplified scenarios of the Minimal Supersymmetric Standard Model.
Resumo:
Results of a search for new phenomena in events with large missing transverse momentum and a Higgs boson decaying to two photons are reported. Data from proton--proton collisions at a center-of-mass energy of 8 TeV and corresponding to an integrated luminosity of 20.3 fb−1 have been collected with the ATLAS detector at the LHC. The observed data are well described by the expected Standard Model backgrounds. Upper limits on the cross section of events with large missing transverse momentum and a Higgs boson candidate are also placed. Exclusion limits are presented for models of physics beyond the Standard Model featuring dark-matter candidates.
Resumo:
OBJETIVO: Identificar prevalência e fatores associados aos sintomas de transtornos alimentares entre escolares. MÉTODOS: Estudo transversal envolvendo 365 escolares, de 7 a 14 anos de idade, do ensino fundamental de Salvador/BA. Aplicou-se nos escolares < 12 anos o Teste de Comportamentos Alimentares e Imagem Corporal e, naqueles > 13 anos de idade, o Teste de Atitudes Alimentares-26, o Teste de Investigação Bulímica de Edinburgh e o Teste de Imagem Corporal. O Child Behavior Checklist foi aplicado para todos os escolares. Coletaram-se dados antropométricos e alimentares, sobre estilo de vida, demográficos, socioeconômicos e puberais. Na análise estatística utilizou-se regressão de Poisson. RESULTADOS: Sintomas de transtornos alimentares estavam presentes em 23% dos escolares. Idade (RP: 1,25; IC95%: 1,11-1,40), insatisfação com imagem corporal (RP: 4,23; IC95%: 2,53-7,08), problema de comportamento de internalização (RP: 1,78; IC95%: 1,11-2,85), substituição das refeições por consumo de balas (RP: 2,14; IC95%: 1,24-3,69), maior consumo de frutas e outros vegetais (RP: 2,49; IC95%: 1,55-3,99) e escolaridade materna de 5ª a 8ª série (RP: 1,95; IC95%: 1,06-3,58) associaram-se ao aumento da ocorrência dos sintomas de transtornos alimentares. CONCLUSÃO: Observou-se alta prevalência de sintomas de transtornos alimentares entre os escolares; fatores sociodemográficos e comportamentais estavam associados ao evento.
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OBJETIVO: Descrever a associação entre depressão durante a gestação e os efeitos no recém-nascido (baixo peso ao nascer e prematuridade). MÉTODOS: Foi realizado um estudo de coorte, com 100 gestantes atendidas entre março e setembro de 2011 em uma unidade de atenção básica de saúde de Nova Iguaçu. As gestantes responderam sobre características sociodemográficas, condições médicas/obstétricas, eventos estressantes e apoio social. A depressão foi avaliada por meio do Composite International Diagnostic Interview (CIDI). Após o período do pós-parto, as mães responderam às questões sobre baixo peso e prematuridade ao nascer. RESULTADOS: A prevalência da depressão na gravidez foi de 18% (IC95%: 12,2-23,8). Fatores associados com desfecho neonatal foram depressão gestacional (OR: 6,60 IC: 1,51-28,91) e uso de álcool (OR: 8,75 IC: 1,10-69,71). CONCLUSÃO: As implicações do presente estudo para a prática enfatizam a necessidade de triagem para depressão durante a gestação.