Metabolism and toxicity of two new benzodiazepine-type antileishmanial agents in hepatocytes and macrophages

With increasing reports of resistance of Leishmania to antimonials (Thakur et al., 2004) and other traditional antileishmanial drugs, the need for the discovery of new antileishmanial agents is rising. In an attempt to find new antileishmanial agents, two new benzodiazepine (BNZ) analogues (7-chloro-4-(cyclohexylmethyl)-1-methyl-3,4-dihydro-1H-1,4-benodiazepine-2,5-dione (BNZ-1) and 4-(cyclohexylmethyl)-1-methyl-3,4-dihydro-1H-1,4-benzodiazepine-2,5-dione (BNZ-2)) were synthesised, and found to be effective against leishmaniasis in mice. This study investigates the metabolism of these two drugs together with the prototype BNZ, flurazepam (FZP), using rat hepatocytes, and investigates their interaction with glutathione in macrophages. Hepatocytes (>80% viability by Trypan Blue exclusion isolated by liver perfusion with collagenase) were prepared from male Sprague-Dawley rats (200-250 g). Drugs (100 μM) were incubated with 2 × 106 viable cells/ml in Krebs-Hepes buffer, pH 7.4, in rotating round bottomed flasks under an atmosphere of 95% O2/5% CO2, at 37 °C for 3 h, and timed samples taken for metabolite measurement. Samples were extracted twice with ethyl acetate at pH 10, the combined organic phases evaporated to dryness and stored at −20 °C until analysis. Metabolites were separated by HPLC using an ACE C18 column (50 mm × 3.0 mm i.d., 5 μm packing), and a solvent gradient consisting of 0.1% formic acid: acetonitrile (starting composition 95:5%, and composition after 25 min 65:35% for FZP and 70:30% for both BNZ 1 and 2). Flow rate was 0.5 ml/min, and detection was at 230 nm. Identification of the metabolites was by mass spectrometry with both positive and negative ion electronspray ionization. The effects of 24 h exposure to the compounds (100 μM) was investigated in the macrophage cell line J774.1 in terms of reduced glutathione content (GSH) and the activity of glutathione reductase (GR). There was no evidence of significant cytotoxicity with any of the compounds at the concentration used. FZP (m/z 388) was metabolised by dealkylation of the two N-1 ethyl substituents (m/z 360 and m/z 332), followed by hydroxylation on the BNZ ring. There was no evidence for either N- or O-glucuronidation of the resulting metabolites. BNZ-1 (m/z 321) was metabolised by N-demethylation (m/z 307) followed by hydroxylation (m/z 323), mono- and di-hydroxylation of the parent (m/z 337 and m/z 353) and by glucuronidation of the mono-hydroxylated metabolite (m/z 513). BNZ-2 (m/z 287) was transformed by N-demethylation (m/z 273) and hydroxylation of the parent (m/z 303), with the latter further metabolised by O-glucuronidation (m/z 479). In addition, the hydroxylated N-demethylated product (m/z 289) was also formed. Macrophages did not produce detectable metabolism of any of the drugs. All the drugs depleted macrophage GSH significantly (p < 0.05 by ANOVA followed by Dunnett's test) with BNZ-1 and BNZ-2 causing greater depletion than FZP (40.6 ± 4.0 and 45.8 ± 8.4, respectively, compared with 55.5 ± 4.9 nmol/mg protein with FZP, n = 3). Control macrophage GSH was 74.1 ± 6.6 nmol/mg protein. The depletion in GSH was not due to inhibition of GR: only FZP caused a significant decrease in macrophage GR activity (28.0 ± 5.9 compared with 42.1 ± 8.0 nmol/ml/min in control cells, p < 0.05 by ANOVA followed by Dunnett's test, n = 3). The marked depletion of macrophage GSH indicates a potential toxic interaction in mammalian cells. The new BNZ analogues were rapidly metabolised by hepatocytes, producing N-dealkylated and multiple hydroxylated phase I metabolites, followed by glucuronidation. This rapid metabolism may limit the therapeutic effect of BNZ 1 and 2 if their metabolites are inactive against leishmaniasis and suggest the need to optimise these lead structures further to obtain compounds with reduced rates and extent of metabolism

Measurement of the View the tt production cross-section using eμ events with b-tagged jets in pp collisions at √s = 13 TeV with the ATLAS detector

This paper describes a measurement of the inclusive top quark pair production cross-section (σtt¯) with a data sample of 3.2 fb−1 of proton–proton collisions at a centre-of-mass energy of √s = 13 TeV, collected in 2015 by the ATLAS detector at the LHC. This measurement uses events with an opposite-charge electron–muon pair in the final state. Jets containing b-quarks are tagged using an algorithm based on track impact parameters and reconstructed secondary vertices. The numbers of events with exactly one and exactly two b-tagged jets are counted and used to determine simultaneously σtt¯ and the efficiency to reconstruct and b-tag a jet from a top quark decay, thereby minimising the associated systematic uncertainties. The cross-section is measured to be: σtt¯ = 818 ± 8 (stat) ± 27 (syst) ± 19 (lumi) ± 12 (beam) pb, where the four uncertainties arise from data statistics, experimental and theoretical systematic effects, the integrated luminosity and the LHC beam energy, giving a total relative uncertainty of 4.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. A fiducial measurement corresponding to the experimental acceptance of the leptons is also presented

Search for strong gravity in multijet final states produced in pp collisions at √s=13 TeV using the ATLAS detector at the LHC

A search is conducted for new physics in multijet final states using 3.6 inverse femtobarns of data from proton-proton collisions at √s = 13TeV taken at the CERN Large Hadron Collider with the ATLAS detector. Events are selected containing at least three jets with scalar sum of jet transverse momenta (HT) greater than 1TeV. No excess is seen at large HT and limits are presented on new physics: models which produce final states containing at least three jets and having cross sections larger than 1.6 fb with HT > 5.8 TeV are excluded. Limits are also given in terms of new physics models of strong gravity that hypothesize additional space-time dimensions

Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at sqrt [ s ] = 13TeV

A search for physics beyond the Standard Model, in final states with at least one high transverse momentum charged lepton (electron or muon) and two additional high transverse momentum leptons or jets, is performed using 3.2 fb−1 of proton–proton collision data recorded by the ATLAS detector at the Large Hadron Collider in 2015 at √s = 13 TeV. The upper end of the distribution of the scalar sum of the transverse momenta of leptons and jets is sensitive to the production of high-mass objects. No excess of events beyond Standard Model predictions is observed. Exclusion limits are set for models of microscopic black holes with two to six extra dimensions

Measurement of the correlation between flow harmonics of different order in lead-lead collisions at √sNN = 2.76 TeV with the ATLAS detector

Correlations between the elliptic or triangular flow coefficients vm (m=2 or 3) and other flow harmonics vn (n=2 to 5) are measured using √sNN=2.76 TeV Pb+Pb collision data collected in 2010 by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 7 μb−1. The vm−vn correlations are measured in midrapidity as a function of centrality, and, for events within the same centrality interval, as a function of event ellipticity or triangularity defined in a forward rapidity region. For events within the same centrality interval, v3 is found to be anticorrelated with v2 and this anticorrelation is consistent with similar anticorrelations between the corresponding eccentricities, ε2 and ε3. However, it is observed that v4 increases strongly with v2, and v5 increases strongly with both v2 and v3. The trend and strength of the vm−vn correlations for n=4 and 5 are found to disagree with εm−εn correlations predicted by initial-geometry models. Instead, these correlations are found to be consistent with the combined effects of a linear contribution to vn and a nonlinear term that is a function of v22 or of v2v3, as predicted by hydrodynamic models. A simple two-component fit is used to separate these two contributions. The extracted linear and nonlinear contributions to v4 and v5 are found to be consistent with previously measured event-plane correlations

The performance of the jet trigger for the ATLAS detector during 2011 data taking

The performance of the jet trigger for the ATLAS detector at the LHC during the 2011 data taking period is described. During 2011 the LHC provided proton–proton collisions with a centre-of-mass energy of 7 TeV and heavy ion collisions with a 2.76 TeV per nucleon–nucleon collision energy. The ATLAS trigger is a three level system designed to reduce the rate of events from the 40 MHz nominal maximum bunch crossing rate to the approximate 400 Hz which can be written to offline storage. The ATLAS jet trigger is the primary means for the online selection of events containing jets. Events are accepted by the trigger if they contain one or more jets above some transverse energy threshold. During 2011 data taking the jet trigger was fully efficient for jets with transverse energy above 25 GeV for triggers seeded randomly at Level 1. For triggers which require a jet to be identified at each of the three trigger levels, full efficiency is reached for offline jets with transverse energy above 60 GeV. Jets reconstructed in the final trigger level and corresponding to offline jets with transverse energy greater than 60 GeV, are reconstructed with a resolution in transverse energy with respect to offline jets, of better than 4 % in the central region and better than 2.5 % in the forward direction

Search for dark matter produced in association with a hadronically decaying vector boson in pp collisions at sqrt (s) = 13 TeV with the ATLAS detector

A search is presented for dark matter produced in association with a hadronically decaying W or Z boson using 3.2 fb−1 of pp collisions at View the MathML sources=13 TeV recorded by the ATLAS detector at the Large Hadron Collider. Events with a hadronic jet compatible with a W or Z boson and with large missing transverse momentum are analysed. The data are consistent with the Standard Model predictions and are interpreted in terms of both an effective field theory and a simplified model containing dark matter

Measurement of the cross section for isolated-photon plus jet production in pp collisions at √s=13 TeV using the ATLAS detector

The dynamics of isolated-photon production in association with a jet in proton–proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 fb−1. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti- algorithm with radius parameter and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon–jet invariant mass and the scattering angle in the photon–jet centre-of-mass system. Tree-level plus parton-shower predictions from Sherpa and Pythia as well as next-to-leading-order QCD predictions from Jetphox and Sherpa are compared to the measurements

Search for vectorlike B quarks in events with one isolated lepton, missing transverse momentum, and jets at √s = 8 TeV with the ATLAS detector

A search has been performed for pair production of heavy vectorlike down-type (B) quarks. The analysis explores the lepton-plus-jets final state, characterized by events with one isolated charged lepton (electron or muon), significant missing transverse momentum, and multiple jets. One or more jets are required to be tagged as arising from b quarks, and at least one pair of jets must be tagged as arising from the hadronic decay of an electroweak boson. The analysis uses the full data sample of pp collisions recorded in 2012 by the ATLAS detector at the LHC, operating at a center-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 20.3 fb −1 . No significant excess of events is observed above the expected background. Limits are set on vectorlike B production, as a function of the B branching ratios, assuming the allowable decay modes are B → Wt/Zb/Hb. In the chiral limit with a branching ratio of 100% for the decay B → Wt, the observed (expected) 95% C.L. lower limit on the vectorlike B mass is 810 GeV (760 GeV). In the case where the vectorlike B quark has branching ratio values corresponding to those of an SU(2) singlet state, the observed (expected) 95% C.L. lower limit on the vectorlike B mass is 640 GeV (505 GeV). The same analysis, when used to investigate pair production of a colored, charge 5/3 exotic fermion T 5/3 , with subsequent decay T 5/3 → Wt, sets an observed (expected) 95% C.L. lower limit on the T 5/3 mass of 840 GeV (780 GeV)