Production of [Formula: see text] and [Formula: see text] in proton-proton collisions at [Formula: see text] 7 TeV.

The production of the strange and double-strange baryon resonances ([Formula: see text], [Formula: see text]) has been measured at mid-rapidity ([Formula: see text][Formula: see text]) in proton-proton collisions at [Formula: see text] [Formula: see text] 7 TeV with the ALICE detector at the LHC. Transverse momentum spectra for inelastic collisions are compared to QCD-inspired models, which in general underpredict the data. A search for the [Formula: see text] pentaquark, decaying in the [Formula: see text] channel, has been carried out but no evidence is seen.

Measurement of prompt D-meson production in p-Pb collisions at √(s(NN))=5.02 TeV.

The p_{T}-differential production cross sections of the prompt charmed mesons D^{0}, D^{+}, D^{*+}, and D_{s}^{+} and their charge conjugate in the rapidity interval -0.96

Exclusive J/ψ photoproduction off protons in ultraperipheral p-Pb collisions at √(s(NN))=5.02 TeV.

We present the first measurement at the LHC of exclusive J/ψ photoproduction off protons, in ultraperipheral proton-lead collisions at sqrt[s_{NN}]=5.02 TeV. Events are selected with a dimuon pair produced either in the rapidity interval, in the laboratory frame, 2.5

Measurement of Galectin-3 with the ARCHITECT assay: Clinical validity and cost-effectiveness in patients with heart failure.

OBJECTIVES: Galectin-3 (Gal-3) testing is emerging as a valuable tool for the prognosis of heart failure (HF). Our objectives were to determine the clinical validity and cost-effectiveness of the recently developed ARCHITECT Gal-3 automated immunoassay. DESIGN AND METHODS: Gal-3 levels were measured in HF patients with reduced left ventricular ejection fraction with the ARCHITECT i2000SR Gal-3 assay as well as with the reference Gal-3 ELISA assay. The relationship between Gal-3 levels determined with the automated assay and HF severity as well as its predictive value for long-term cardiovascular death were evaluated. The impact of Gal-3 testing on the diagnostic related group (DRG) based reimbursement was also estimated. RESULTS: Gal-3 levels measured with the ARCHITECT assay were related to the severity of HF based on New York Heart Association functional classes (p<0.001) and were also significantly and positively correlated to BNP concentrations (r=0.35, p<0.001). Gal-3 values higher than 19.2 ng/mL were predictive of long-term cardiovascular death in patients with systolic HF and also provided incremental prognostic information to BNP testing. In addition, Gal-3 testing was estimated to save DRG in comparison to standard of care. CONCLUSIONS: Our results demonstrated the clinical validity of the ARCHITECT Gal-3 automated immunoassay for the risk stratification of HF patients. The automation of Gal-3 testing was also cost-effective and might help to preserve hospital budget.

Measurement of quarkonium production at forward rapidity in [Formula: see text] collisions at [Formula: see text]TeV.

The inclusive production cross sections at forward rapidity of [Formula: see text], [Formula: see text], [Formula: see text](1S) and [Formula: see text](2S) are measured in [Formula: see text] collisions at [Formula: see text] with the ALICE detector at the LHC. The analysis is based on a data sample corresponding to an integrated luminosity of 1.35 pb[Formula: see text]. Quarkonia are reconstructed in the dimuon-decay channel and the signal yields are evaluated by fitting the [Formula: see text] invariant mass distributions. The differential production cross sections are measured as a function of the transverse momentum [Formula: see text] and rapidity [Formula: see text], over the ranges [Formula: see text] GeV/c for [Formula: see text], [Formula: see text] GeV/c for all other resonances and for [Formula: see text]. The measured cross sections integrated over [Formula: see text] and [Formula: see text], and assuming unpolarized quarkonia, are: [Formula: see text] [Formula: see text]b, [Formula: see text] [Formula: see text]b, [Formula: see text] nb and [Formula: see text] nb, where the first uncertainty is statistical and the second one is systematic. The results are compared to measurements performed by other LHC experiments and to theoretical models.

Galectin-3 testing: validity of a novel automated assay in heart failure patients with reduced ejection fraction.

Circulating levels of galectin-3 (Gal-3), a marker of cardiac fibrosis and remodeling, contribute to the risk stratification of patients with heart failure (HF). The aim of our study was to determine the analytical validity and clinical validity of a novel automated Gal-3 assay in HF patients with reduced ejection fraction. We showed an excellent agreement between the VIDAS® Gal-3 automated assay and the ELISA reference method (r=0.90, p<0.001) and a mean difference of -1.3 ng/mL was observed on the Bland and Altman plot. Gal-3 levels measured with the VIDAS® assay were significantly related to NYHA functional classes (p<0.001) and mean Gal-3 levels were 13.8 ng/mL in NYHA II patients, 17.7 ng/mL in NYHA III and 19.6 ng/mL in NYHA IV. Furthermore, our results showed that Gal-3 levels measured with the VIDAS® assay were not only predictive of long-term cardiovascular death in patients with systolic HF but have also provided added value to natriuretic peptide testing in multimarker strategies. Therefore, our data are also supporting the clinical validity of the Gal-3 automated assay.

K(S)0 and Λ production in Pb-Pb collisions at √(s(NN))=2.76 TeV.

The ALICE measurement of K(S)(0) and Λ production at midrapidity in Pb-Pb collisions at √(s(NN))=2.76 TeV is presented. The transverse momentum (p(T)) spectra are shown for several collision centrality intervals and in the p(T) range from 0.4 GeV/c (0.6 GeV/c for Λ) to 12 GeV/c. The p(T) dependence of the Λ/K(S)(0) ratios exhibits maxima in the vicinity of 3 GeV/c, and the positions of the maxima shift towards higher p(T) with increasing collision centrality. The magnitude of these maxima increases by almost a factor of three between most peripheral and most central Pb-Pb collisions. This baryon excess at intermediate p(T) is not observed in pp interactions at √s=0.9 TeV and at √s=7 TeV. Qualitatively, the baryon enhancement in heavy-ion collisions is expected from radial flow. However, the measured p(T) spectra above 2 GeV/c progressively decouple from hydrodynamical-model calculations. For higher values of p(T), models that incorporate the influence of the medium on the fragmentation and hadronization processes describe qualitatively the p(T) dependence of the Λ/K(S)(0) ratio.

J/ψ elliptic flow in Pb-Pb collisions at √(s(NN))=2.76 TeV.

We report on the first measurement of inclusive J/ψ elliptic flow v2 in heavy-ion collisions at the LHC. The measurement is performed with the ALICE detector in Pb-Pb collisions at √(s(NN))=2.76 TeV in the rapidity range 2.5

What is the phenotype of patients with gastrointestinal intolerance to metformin?

BACKGROUND: A substantial minority of type 2 diabetes mellitus (T2DM) patients treated with metformin develop severe gastrointestinal (GI) symptoms leading to drug discontinuation, depriving them of the potentially cardioprotective pleiotropic effects of this first-line oral agent. At present, it is unclear whether treating diabetes without being able to ever use metformin alters cardiovascular outcomes. PATIENTS AND METHODS: From a population of 773 consecutive T2DM outpatients, the cardiometabolic phenotypes of 83 patients who discontinued metformin due to GI intolerance (Met-Intol cases) were compared with those of 332 age- and gender-matched metformin-tolerant (Met-Tol) controls, amounting to a case: control ratio of 1:4. RESULTS: Mean age (SD) was 70 (13) (male:female: 46:54). Metformin intolerance was associated with a reduced prevalence of macroangiopathy (P=0.0486), mainly due to a lower prevalence of CAD (-34%; P=0.0374). Met-Intol cases more often belonged to blood group A and subgroup A Rh+, with 50% and 66% relative increases (P=0.0039 and P=0.0005), respectively. There were twice as many non-right-handers among the Met-Intol (18% vs. 9%; P=0.0262), and this group also had significantly higher serum ferritin and LDL cholesterol levels. Statins/fibrates were used by 66%/19% of Met-Tol vs. 48%/18% of Met-Intol (P=0.0051 for statins). On the other hand, there were no differences between groups as regards smoking, diabetes duration, HbA1c, BMI, blood pressure, waist size, fat mass, visceral fat, liver steatosis, the metabolic syndrome, eGFR, albuminuria, erectile dysfunction and microangiopathy. CONCLUSION: Intolerance to metformin represents an unforeseen phenotype in T2DM patients characterized by a low rate of ischaemic heart disease, left-handedness, ABO group imbalance and an iron load.

Transverse momentum distribution and nuclear modification factor of charged particles in p+Pb collisions at sqrt[s(NN)] = 5.02 TeV.

The transverse momentum (p(T)) distribution of primary charged particles is measured in minimum bias (non-single-diffractive) p+Pb collisions at sqrt[s(NN)]=5.02 TeV with the ALICE detector at the LHC. The p(T) spectra measured near central rapidity in the range 0.5

Charge separation relative to the reaction plane in Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV.

Measurements of charge-dependent azimuthal correlations with the ALICE detector at the LHC are reported for Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV. Two- and three-particle charge-dependent azimuthal correlations in the pseudorapidity range |η| < 0.8 are presented as a function of the collision centrality, particle separation in pseudorapidity, and transverse momentum. A clear signal compatible with a charge-dependent separation relative to the reaction plane is observed, which shows little or no collision energy dependence when compared to measurements at RHIC energies. This provides a new insight for understanding the nature of the charge-dependent azimuthal correlations observed at RHIC and LHC energies.

Pseudorapidity density of charged particles in p+Pb collisions at √(s(NN))=5.02 TeV.

The charged-particle pseudorapidity density measured over four units of pseudorapidity in nonsingle-diffractive p+Pb collisions at a center-of-mass energy per nucleon pair √(s(NN))=5.02 TeV is presented. The average value at midrapidity is measured to be 16.81±0.71 (syst), which corresponds to 2.14±0.17 (syst) per participating nucleon, calculated with the Glauber model. This is 16% lower than in nonsingle-diffractive pp collisions interpolated to the same collision energy and 84% higher than in d+Au collisions at s√(s(NN))=0.2 TeV. The measured pseudorapidity density in p+Pb collisions is compared to model predictions and provides new constraints on the description of particle production in high-energy nuclear collisions.

Comparison between intact and bioactive parathyroid hormone assays in patients with severe heart failure.

OBJECTIVES: Parathyroid hormone (PTH) is a major systemic calcium-regulating hormone. Recent evidence has suggested that measurement of PTH might provide complementary information for the diagnosis and risk stratification of patients with heart failure (HF). The aim of our study was to compare intact and bioactive PTH assays in patients with severe heart failure. DESIGN AND METHODS: The following measurements were carried out in blood samples from 73 patients with severe heart failure: bioactive PTH (1-84) assay, intact PTH assay, non-PTH (1-84), 25-hydroxyvitamin D, B-type natriuretic peptide (BNP), N-terminal proBNP (Nt-proBNP), Galectin-3 and high sensitive troponin T (hsTnT). RESULTS: The correlation between intact and bioactive PTH assays was very high in HF patients. However, the bioactive PTH concentrations were lower than those measured with the intact assay. Intact and bioactive PTH as well as non-PTH (1-84) was significantly and positively correlated to BNP, Nt-proBNP, and galectin-3 but not to hsTnT. The strongest relationships with these cardiac biomarkers and with cardiovascular death were observed with the bioactive PTH assay. CONCLUSIONS: The PTH concentrations obtained with intact and bioactive assays are not comparable in patients with severe HF. The specificity of PTH assays might therefore impact on the potential diagnosis and prognosis values of PTH testing in patients with heart failure.

Charmonium and e+e- pair photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at [Formula: see text].

The ALICE Collaboration at the LHC has measured the J/ψ and ψ' photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at [Formula: see text]. The charmonium is identified via its leptonic decay for events where the hadronic activity is required to be minimal. The analysis is based on an event sample corresponding to an integrated luminosity of about 23 µb-1. The cross section for coherent and incoherent J/ψ production in the rapidity interval -0.9

Energy dependence of the transverse momentum distributions of charged particles in pp collisions measured by ALICE.

Differential cross sections of charged particles in inelastic pp collisions as a function of pT have been measured at [Formula: see text] at the LHC. The pT spectra are compared to NLO-pQCD calculations. Though the differential cross section for an individual [Formula: see text] cannot be described by NLO-pQCD, the relative increase of cross section with [Formula: see text] is in agreement with NLO-pQCD. Based on these measurements and observations, procedures are discussed to construct pp reference spectra at [Formula: see text] up to pT=50 GeV/c as required for the calculation of the nuclear modification factor in nucleus-nucleus and proton-nucleus collisions.

Measurement of inelastic, single- and double-diffraction cross sections in proton-proton collisions at the LHC with ALICE.

Measurements of cross sections of inelastic and diffractive processes in proton-proton collisions at LHC energies were carried out with the ALICE detector. The fractions of diffractive processes in inelastic collisions were determined from a study of gaps in charged particle pseudorapidity distributions: for single diffraction (diffractive mass MX <200 GeV/c2) [Formula: see text], and [Formula: see text], respectively at centre-of-mass energies [Formula: see text]; for double diffraction (for a pseudorapidity gap Δη>3) σDD/σINEL=0.11±0.03,0.12±0.05, and [Formula: see text], respectively at [Formula: see text]. To measure the inelastic cross section, beam properties were determined with van der Meer scans, and, using a simulation of diffraction adjusted to data, the following values were obtained: [Formula: see text] mb at [Formula: see text] and [Formula: see text] at [Formula: see text]. The single- and double-diffractive cross sections were calculated combining relative rates of diffraction with inelastic cross sections. The results are compared to previous measurements at proton-antiproton and proton-proton colliders at lower energies, to measurements by other experiments at the LHC, and to theoretical models.

Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV.

The directed flow of charged particles at midrapidity is measured in Pb-Pb collisions at √(s(NN))=2.76 TeV relative to the collision symmetry plane defined by the spectator nucleons. A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found at the highest RHIC energy is observed. This suggests a smaller longitudinal tilt of the initial system and disfavors the strong fireball rotation predicted for the LHC energies. The rapidity-even directed flow component is measured for the first time with spectators and found to be independent of pseudorapidity with a sign change at transverse momenta p(T) between 1.2 and 1.7 GeV/c. Combined with the observation of a vanishing rapidity-even p(T) shift along the spectator deflection this is strong evidence for dipolelike initial density fluctuations in the overlap zone of the nuclei. Similar trends in the rapidity-even directed flow and the estimate from two-particle correlations at midrapidity, which is larger by about a factor of 40, indicate a weak correlation between fluctuating participant and spectator symmetry planes. These observations open new possibilities for investigation of the initial conditions in heavy-ion collisions with spectator nucleons.

D meson elliptic flow in noncentral Pb-Pb collisions at sqrt[sNN]=2.76 Tev.

Azimuthally anisotropic distributions of D0, D+, and D*+ mesons were studied in the central rapidity region (|y|<0.8) in Pb-Pb collisions at a center-of-mass energy sqrt[sNN]=2.76 TeV per nucleon-nucleon collision, with the ALICE detector at the LHC. The second Fourier coefficient v2 (commonly denoted elliptic flow) was measured in the centrality class 30%-50% as a function of the D meson transverse momentum pT, in the range 2-16 GeV/c. The measured v2 of D mesons is comparable in magnitude to that of light-flavor hadrons. It is positive in the range 2

Net-charge fluctuations in Pb-Pb collisions at sqrt[sNN]=2.76 TeV.

We report the first measurement of the net-charge fluctuations in Pb-Pb collisions at sqrt[sNN]=2.76 TeV, measured with the ALICE detector at the CERN Large Hadron Collider. The dynamical fluctuations per unit entropy are observed to decrease when going from peripheral to central collisions. An additional reduction in the amount of fluctuations is seen in comparison to the results from lower energies. We examine the dependence of fluctuations on the pseudorapidity interval, which may account for the dilution of fluctuations during the evolution of the system. We find that the fluctuations at the LHC are smaller compared to the measurements at the BNL Relativistic Heavy Ion Collider, and as such, closer to what has been theoretically predicted for the formation of a quark-gluon plasma.