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ATLAS measured the centrality dependence of the dijet yield using 165 nb^{-1} of p+Pb data collected at sqrt[s_{NN}]=8.16 TeV in 2016. The event centrality, which reflects the p+Pb impact parameter, is characterized by the total transverse energy registered in the Pb-going side of the forward calorimeter. The central-to-peripheral ratio of the scaled dijet yields, R_{CP}, is evaluated, and the results are presented as a function of variables that reflect the kinematics of the initial hard parton scattering process. The R_{CP} shows a scaling with the Bjorken x of the parton originating from the proton, x_{p}, while no such trend is observed as a function of x_{Pb}. This analysis provides unique input to understanding the role of small proton spatial configurations in p+Pb collisions by covering parton momentum fractions from the valence region down to x_{p}â¼10^{-3} and x_{Pb}â¼4×10^{-4}.
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Searches for new resonances are performed using an unsupervised anomaly-detection technique. Events with at least one electron or muon are selected from 140 fb^{-1} of pp collisions at sqrt[s]=13 TeV recorded by ATLAS at the Large Hadron Collider. The approach involves training an autoencoder on data, and subsequently defining anomalous regions based on the reconstruction loss of the decoder. Studies focus on nine invariant mass spectra that contain pairs of objects consisting of one light jet or b jet and either one lepton (e,µ), photon, or second light jet or b jet in the anomalous regions. No significant deviations from the background hypotheses are observed. Limits on contributions from generic Gaussian signals with various widths of the resonance mass are obtained for nine invariant masses in the anomalous regions.
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Statistical combinations of searches for charginos and neutralinos using various decay channels are performed using 139 fb^{-1} of pp collision data at sqrt[s]=13 TeV with the ATLAS detector at the Large Hadron Collider. Searches targeting pure-wino chargino pair production, pure-wino chargino-neutralino production, or Higgsino production decaying via standard model W, Z, or h bosons are combined to extend the mass reach to the produced supersymmetric particles by 30-100 GeV. The depth of the sensitivity of the original searches is also improved by the combinations, lowering the 95% C.L. cross-section upper limits by 15%-40%.
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A combination of searches for a new resonance decaying into a Higgs boson pair is presented, using up to 139 fb^{-1} of pp collision data at sqrt[s]=13 TeV recorded with the ATLAS detector at the LHC. The combination includes searches performed in three decay channels: bb[over ¯]bb[over ¯], bb[over ¯]τ^{+}τ^{-}, and bb[over ¯]γγ. No excess above the expected Standard Model background is observed and upper limits are set at the 95% confidence level on the production cross section of Higgs boson pairs originating from the decay of a narrow scalar resonance with mass in the range 251 GeV-5 TeV. The observed (expected) limits are in the range 0.96-600 fb (1.2-390 fb). The limits are interpreted in the type-I two-Higgs-doublet model and the minimal supersymmetric standard model, and constrain parameter space not previously excluded by other searches.
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Higgsinos with masses near the electroweak scale can solve the hierarchy problem and provide a dark matter candidate, while detecting them at the LHC remains challenging if their mass splitting is O(1 GeV). This Letter presents a novel search for nearly mass-degenerate Higgsinos in events with an energetic jet, missing transverse momentum, and a low-momentum track with a significant transverse impact parameter using 140 fb^{-1} of proton-proton collision data at sqrt[s]=13 TeV collected by the ATLAS experiment. For the first time since LEP, a range of mass splittings between the lightest charged and neutral Higgsinos from 0.3 to 0.9 GeV is excluded at 95% confidence level, with a maximum reach of approximately 170 GeV in the Higgsino mass.
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Angular correlations between heavy quarks provide a unique probe of the quark-gluon plasma created in ultrarelativistic heavy-ion collisions. Results are presented of a measurement of the azimuthal angle correlations between muons originating from semileptonic decays of heavy quarks produced in 5.02 TeV Pb+Pb and pp collisions at the LHC. The muons are measured with transverse momenta and pseudorapidities satisfying p_{T}^{µ}>4 GeV and |η^{µ}|<2.4, respectively. The distributions of azimuthal angle separation ΔÏ for muon pairs having pseudorapidity separation |Δη|>0.8, are measured in different Pb+Pb centrality intervals and compared to the same distribution measured in pp collisions at the same center-of-mass energy. Results are presented separately for muon pairs with opposite-sign charges, same-sign charges, and all pairs. A clear peak is observed in all ΔÏ distributions at ΔÏâ¼π, consistent with the parent heavy-quark pairs being produced via hard-scattering processes. The widths of that peak, characterized using Cauchy-Lorentz fits to the ΔÏ distributions, are found to not vary significantly as a function of Pb+Pb collision centrality and are similar for pp and Pb+Pb collisions. This observation will provide important constraints on theoretical descriptions of heavy-quark interactions with the quark-gluon plasma.
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This Letter reports the observation of WZγ production and a measurement of its cross section using 140.1±1.2 fb^{-1} of proton-proton collision data recorded at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The WZγ production cross section, with both the W and Z bosons decaying leptonically, ppâWZγââ^{'}^{±}νâ^{+}â^{-}γ (â^{(^{'})}=e, µ), is measured in a fiducial phase-space region defined such that the leptons and the photon have high transverse momentum and the photon is isolated. The cross section is found to be 2.01±0.30(stat)±0.16(syst) fb. The corresponding standard model predicted cross section calculated at next-to-leading order in perturbative quantum chromodynamics and at leading order in the electroweak coupling constant is 1.50±0.06 fb. The observed significance of the WZγ signal is 6.3σ, compared with an expected significance of 5.0σ.
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This Letter presents the first study of Higgs boson production in association with a vector boson (V=W or Z) in the fully hadronic qqbb final state using data recorded by the ATLAS detector at the LHC in proton-proton collisions at sqrt[s]=13 TeV and corresponding to an integrated luminosity of 137 fb^{-1}. The vector bosons and Higgs bosons are each reconstructed as large-radius jets and tagged using jet substructure techniques. Dedicated tagging algorithms exploiting b-tagging properties are used to identify jets consistent with Higgs bosons decaying into bb[over ¯]. Dominant backgrounds from multijet production are determined directly from the data, and a likelihood fit to the jet mass distribution of Higgs boson candidates is used to extract the number of signal events. The VH production cross section is measured inclusively and differentially in several ranges of Higgs boson transverse momentum: 250-450, 450-650, and greater than 650 GeV. The inclusive signal yield relative to the standard model expectation is observed to be µ=1.4_{-0.9}^{+1.0} and the corresponding cross section is 3.1±1.3(stat)_{-1.4}^{+1.8}(syst) pb.
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A search is made for potential ccc[over ¯]c[over ¯] tetraquarks decaying into a pair of charmonium states in the four muon final state using proton-proton collision data at sqrt[s]=13 TeV, corresponding to an integrated luminosity of 140 fb^{-1} recorded by the ATLAS experiment at LHC. Two decay channels, J/ψ+J/ψâ4µ and J/ψ+ψ(2S)â4µ, are studied. Backgrounds are estimated based on a hybrid approach involving Monte Carlo simulations and data-driven methods. Statistically significant excesses with respect to backgrounds dominated by the single parton scattering are seen in the di-J/ψ channel consistent with a narrow resonance at 6.9 GeV and a broader structure at lower mass. A statistically significant excess is also seen in the J/ψ+ψ(2S) channel. The fitted masses and decay widths of the structures are reported.
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A key open question in the study of multiparticle production in high-energy pp collisions is the relationship between the "ridge"-i.e., the observed azimuthal correlations between particles in the underlying event that extend over all rapidities-and hard or semihard scattering processes. In particular, it is not known whether jets or their soft fragments are correlated with particles in the underlying event. To address this question, two-particle correlations are measured in pp collisions at sqrt[s]=13 TeV using data collected by the ATLAS experiment at the LHC, with an integrated luminosity of 15.8 pb^{-1}, in two different configurations. In the first case, charged particles associated with jets are excluded from the correlation analysis, while in the second case, correlations are measured between particles within jets and charged particles from the underlying event. Second-order flow coefficients, v_{2}, are presented as a function of event multiplicity and transverse momentum. These measurements show that excluding particles associated with jets does not affect the measured correlations. Moreover, particles associated with jets do not exhibit any significant azimuthal correlations with the underlying event, ruling out hard processes contributing to the ridge.
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A measurement of the mass of the Higgs boson combining the HâZZ^{*}â4â and Hâγγ decay channels is presented. The result is based on 140 fb^{-1} of proton-proton collision data collected by the ATLAS detector during LHC run 2 at a center-of-mass energy of 13 TeV combined with the run 1 ATLAS mass measurement, performed at center-of-mass energies of 7 and 8 TeV, yielding a Higgs boson mass of 125.11±0.09(stat)±0.06(syst)=125.11±0.11 GeV. This corresponds to a 0.09% precision achieved on this fundamental parameter of the Standard Model of particle physics.
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A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the standard model Z boson is presented, using 139 fb^{-1} of sqrt[s]=13 TeV proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the standard model photon and the dark photon, α_{D}ϵ^{2}, in the dark photon mass range of [5, 40] GeV except for the Ï mass window [8.8, 11.1] GeV. This search explores new parameter space not previously excluded by other experiments.
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Human urinary DNase I was inactivated by monoiodoacetate and monobromoacetate. The inactivation was greater at pH 7.2 than at 6.0 and proceeded in the presence of Ca2+. Amino acid analysis of monobromoacetate-inactivated human urinary DNase I indicated that one histidine residue per mole of the enzyme reacted with monobromoacetate. Diethylpyrocarbonate also inactivated the enzyme, which was protected by DNA in the presence of Mg2+. However, oligonucleotides did not prevent the inactivation even in the presence of Mg2+. Hydroxylamine almost completely restored the activity of the inactivated enzyme by DEP. One histidine residue per mole of the enzyme was calculated to be modified, as shown by the difference spectra of DEP-inactivated enzyme. This histidine residue seems to react with the substrate. These results provide evidence that human urinary DNase I possesses one essential histidine residue at the active site.
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Desoxirribonucleasas/orina , Histidina/química , Acetatos/química , Sitios de Unión , Desoxirribonucleasas/química , Desoxirribonucleasas/metabolismo , Dietil Pirocarbonato/química , Humanos , Yodoacetatos/química , Espectrofotometría UltravioletaRESUMEN
Sickle red blood cells (RBCs) have been shown to have an increase in total nicotinamide adenine dinucleotide (NAD) content by an as-yet-unknown mechanism. Because glutamine is an essential precursor in NAD biosynthesis, we have examined the rates of active RBC glutamine transport and glutamine transport kinetics with Michaelis-Menten constant (K[m]) and maximum velocity (V[max]) in RBCs from patients with sickle cell disease, patients with high reticulocyte counts, and normal volunteers. In addition, plasma and RBC levels of glutamine and glutamate in the three groups were analyzed. The rate of active glutamate transport in sickle RBCs increased threefold over that in high-reticulocyte RBCs and increased 15-fold over that in normal RBCs. Glutamine transport K(m) in sickle RBCs was decreased fivefold in comparison with that in the high-reticulocyte group and that in normal control subjects. Glutamine transport V(max) for sickle RBCs was twofold and eightfold higher in comparison with those in the high-reticulocyte RBCs and normal control RBCs, respectively. Finally, the level of RBC glutamate (a byproduct of glutamine in NAD synthesis) in the sickle group was significantly increased in comparison with that in the high-reticulocyte group, whereas the RBC glutamine level was not. The higher glutamate level in sickle cells may suggest a higher glutamine turnover in these cells. These data suggest that sickle RBCs have an increased glutamine availability and affinity that may facilitate the increase in total NAD in sickle RBCs.
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Anemia de Células Falciformes/metabolismo , Eritrocitos/metabolismo , Glutamina/metabolismo , Transporte Biológico Activo , Ácido Glutámico/metabolismo , Humanos , Cinética , NAD/metabolismoRESUMEN
Previously, we demonstrated that there is an increased utilization of glutamine by intact sickle red blood cells (RBC) in conjunction with nicotinamide adenine dinucleotide (NAD) metabolism in vitro. In this report, we describe the in vivo effect of L-glutamine supplementation on total NAD, nicotinamide adenine dinucleotide reduced (NADH), and NAD redox potential of sickle RBC. Seven adult sickle cell anemia patients participated in this study. The exclusion criteria were pregnancy, previous or current use of hydroxyurea, and transfusion within 3 months of initiation of the study. After proper consent, L-glutamine was started at a dose of 30 g/day administered orally. Fasting blood samples were drawn at baseline and after 4 weeks of therapy by routine phlebotomy for evaluation of RBC total NAD and NADH levels. We found significant changes in both the NADH level and NAD redox potential (ratio of NADH to NAD+ + NADH). NAD redox potential increased from 47.2 +/- 3.7% to 62.1 +/- 11.8% (P < 0.01). The NADH level increased from 47.5 +/- 6.3 to 72.1 +/- 15.1 nmol/ml RBC (P < 0.01). The total NAD level demonstrated an upward trend (from 101.2 +/- 16 to 116.4 +/- 14.7 nmol/ml RBC) but this was not statistically significant. Our data show that oral L-glutamine can significantly increase the NAD redox potential and NADH level in sickle RBC. These changes may decrease oxidative susceptibility of sickle RBC and result in clinical benefit.
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Anemia de Células Falciformes/tratamiento farmacológico , Suplementos Dietéticos , Eritrocitos/efectos de los fármacos , Glutamina/uso terapéutico , NAD/sangre , Administración Oral , Adulto , Humanos , Persona de Mediana Edad , Oxidación-Reducción , Proyectos Piloto , Resultado del TratamientoRESUMEN
Desferrioxamine (DFO) is an important iron-chelating agent. It has also been thought of as an agent with anti-oxidant potential as it chelates ferric iron in various parts of the body. However, there is evidence suggesting that it may paradoxically affect red blood cells (RBCs) by inducing intracellular oxidant stress. Recently we observed that incubation of RBCs with DFO decreases NAD redox potential in normal RBC. To further understand the mechanism of DFO's interaction with RBC, we conducted a study to determine the effect of extracellular DFO upon RBC's redox status. We examined NAD redox potential in intact RBC (N = 7) incubated with DFO conjugated to starch. RBCs were incubated with 4 mM DFO for 3(1/2) hr and with 6 mM DFO for 2 and 3(1/2) hr. Significant decreases in NAD redox potential were observed after the incubations. With 4 mM DFO at the 3 (1/2) hr time point the mean decrease was 12.37% +/- 9.96% (P < 0.0085). With 6 mM DFO, the mean decreases were 18.54% +/- 9.79% (P < 0.0013) and 19.16% +/- 8.78% (P < 0.0006) for the 2 and 3 (1/2) hr incubations, respectively. DFO by itself is very poorly permeable to RBC. Conjugation with starch further ensured impermeability of DFO. The data presented here confirm the oxidant effect of DFO on RBC. The data also demonstrate that the effect of DFO on RBC's NAD redox potential originates extracellularly.