1,546 research outputs found

    The influence of probiotic on the biochemical status of young pigs

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    Abstract. Nowadays the fact of positive effects of new environmentally friendly and at the same time highly effective probiotic, antibacterial drugs on the body of young pigs attract particular attention of scientists. One of such drugs is sporobacterin. The aim of this study is to determine the influence of this drug on the physiological, morphological, and biochemical status of young pigs. The research was carried out on a pig farm «Ozerny» in the Republic of Tatarstan, Russia. The objects of the research were 75 one-day-old large white piglets, each weighing 1.1–1.2 kg. The young pigs were divided into three groups. Every day for 30 days the piglets of the first experimental group were given sporobacterin liquid at a dose of 0.2 ml/h, and a dose of 0.5 ml/h was administered to the second experimental group. The animals of the control group were on a basic diet. The study has shown that the administration of sporobacterin liquid at a dose of 0.2 and 0.5 ml/h induced high physiological activity. Morphological and biochemical blood composition in piglets of the experimental groups had improved by the age of 60 days. The total protein level in the serum of piglets increased by 8.95% and 8.98%; albumin, 6.13% and 7.37%; globulin, 10.79% and 11.43%; and gamma globulin, 27.74%, and 28.05%. The dose of 0.5 ml/h was more effective on average by 0.75%.</p

    Intraductal photodynamic therapy and its combination with intra-arterial chemoinfusion in the treatment of inoperable patients with Klatskin tumor

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    Background: A palliative or symptomatic treatment is indicated for 7080% of patients with Klatskins tumor because of the advanced lesion volume and the patients grave condition. Hepatic arterial infusion chemotherapy, chemoembolization, radioembolization are successfully used in the treatment of hepatocellular carcinoma and liver metastases. Aim: to estimate the immediate and long-term results of photodynamic therapy (PDT) and its combination with hepatic arterial infusion in inoperable patients with Klatskin tumors. Methods: Between 2010 and 2021, 83 palliative PDT sessions (from 1 to 8, average 2.4) were performed in 82 patients as a single treatment or in combination with hepatic arterial infusion. In all cases, percutaneous transhepatic biliary drainage was previously performed; no chemotherapy was applied. Two groups of 48 patients were stratified according to the ECOG status (23) and the numbers of PDT sessions (no more than two). The treatment group of the combination therapy consisted of 24 patients (13 male, 11 female) aged 38 to 85 (mean 63) years with the ECOG status of 24 (mean 2.4). This group received PDT with hepatic arterial infusion using a GemCis regimen. On average, 1.4 PDT sessions were performed, the treatment started on the 89th (27225) day after the biliary drainage. The hepatic arterial infusion was performed on the 2d3th day after the PDT. The control group received only PDT and consisted of 24 patients (13 male, 11 female) aged 51 to 83 (66 on average) years, with the ECOG status of 23 (mean 2.6). On average, 1.4 PDT sessions were performed, starting on the 106th (32405) day after the biliary drainage. Results: There were no serious adverse events associated with PDT in both groups. Toxic complications of hepatic arterial infusion were observed in 13 of 24 patients (54%): III grade hematological (54%) and gastrointestinal (69%); all were eliminated with medical therapy. Complications of the percutaneous transhepatic biliary drainage in three patients (hemobilia, n=2, and sepsis, n=1) were estimated as grade III by the CIRSE classification (2017) and successfully treated without surgery. In the combination treatment group, the overall mean survival and median survival were higher than those in the control group: 327.939.8 days (10.9 mo) versus 246.931.2 days (8.2 mo) and 275 days versus 244 days. However, these differences did not reach the statistical significance (p=0.12). Conclusions: PDT is a safe method of a palliative treatment of critically ill patients with Klatskin tumor (ECOG 23). PDT alone has limited clinical efficacy. A combination of PDT and hepatic arterial infusion does not cause serious complications and may increase the survival rates

    Measurements of the pp → ZZ production cross section and the Z → 4ℓ branching fraction, and constraints on anomalous triple gauge couplings at √s = 13 TeV

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    Four-lepton production in proton-proton collisions, pp -> (Z/gamma*)(Z/gamma*) -> 4l, where l = e or mu, is studied at a center-of-mass energy of 13 TeV with the CMS detector at the LHC. The data sample corresponds to an integrated luminosity of 35.9 fb(-1). The ZZ production cross section, sigma(pp -> ZZ) = 17.2 +/- 0.5 (stat) +/- 0.7 (syst) +/- 0.4 (theo) +/- 0.4 (lumi) pb, measured using events with two opposite-sign, same-flavor lepton pairs produced in the mass region 60 4l) = 4.83(-0.22)(+0.23) (stat)(-0.29)(+0.32) (syst) +/- 0.08 (theo) +/- 0.12(lumi) x 10(-6) for events with a four-lepton invariant mass in the range 80 4GeV for all opposite-sign, same-flavor lepton pairs. The results agree with standard model predictions. The invariant mass distribution of the four-lepton system is used to set limits on anomalous ZZZ and ZZ. couplings at 95% confidence level: -0.0012 < f(4)(Z) < 0.0010, -0.0010 < f(5)(Z) < 0.0013, -0.0012 < f(4)(gamma) < 0.0013, -0.0012 < f(5)(gamma) < 0.0013

    Bose-Einstein correlations of charged hadrons in proton-proton collisions at s\sqrt s = 13 TeV

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    Bose-Einstein correlations of charged hadrons are measured over a broad multiplicity range, from a few particles up to about 250 reconstructed charged hadrons in proton-proton collisions at s \sqrt{s} = 13 TeV. The results are based on data collected using the CMS detector at the LHC during runs with a special low-pileup configuration. Three analysis techniques with different degrees of dependence on simulations are used to remove the non-Bose-Einstein background from the correlation functions. All three methods give consistent results. The measured lengths of homogeneity are studied as functions of particle multiplicity as well as average pair transverse momentum and mass. The results are compared with data from both CMS and ATLAS at s \sqrt{s} = 7 TeV, as well as with theoretical predictions.[graphic not available: see fulltext]Bose-Einstein correlations of charged hadrons are measured over a broad multiplicity range, from a few particles up to about 250 reconstructed charged hadrons in proton-proton collisions at s=\sqrt{s} = 13 TeV. The results are based on data collected using the CMS detector at the LHC during runs with a special low-pileup configuration. Three analysis techniques with different degrees of dependence on simulations are used to remove the non-Bose-Einstein background from the correlation functions. All three methods give consistent results. The measured lengths of homogeneity are studied as functions of particle multiplicity as well as average pair transverse momentum and mass. The results are compared with data from both CMS and ATLAS at s=\sqrt{s} = 7 TeV, as well as with theoretical predictions

    Azimuthal separation in nearly back-to-back jet topologies in inclusive 2-and 3-jet events in pp collisions at root s=13TeV

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    A measurement for inclusive 2- and 3-jet events of the azimuthal correlation between the two jets with the largest transverse momenta, Delta phi(12), is presented. The measurement considers events where the two leading jets are nearly collinear ("back-to-back") in the transverse plane and is performed for several ranges of the leading jet transverse momentum. Proton-proton collision data collected with the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 fb(-1) are used. Predictions based on calculations using matrix elements at leading-order and next-to-leading-order accuracy in perturbative quantum chromodynamics supplemented with leading-log parton showers and hadronization are generally in agreement with themeasurements. Discrepancies between the measurement and theoretical predictions are as large as 15%, mainly in the region 177 degrees <Delta phi(12) <180 degrees. The 2- and 3-jet measurements are not simultaneously described by any of models.Peer reviewe

    Measurement of electroweak WZ boson production and search for new physics in WZ + two jets events in pp collisions at √s=13TeV

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    A measurement of WZ electroweak (EW) vector boson scattering is presented. The measurement is performed in the leptonic decay modes WZ→ℓνℓ′ℓ′, where ℓ,ℓ′=e,μ. The analysis is based on a data sample of proton-proton collisions at √s=13 TeV at the LHC collected with the CMS detector and corresponding to an integrated luminosity of 35.9 fb−1. The WZ plus two jet production cross section is measured in fiducial regions with enhanced contributions from EW production and found to be consistent with standard model predictions. The EW WZ production in association with two jets is measured with an observed (expected) significance of 2.2 (2.5) standard deviations. Constraints on charged Higgs boson production and on anomalous quartic gauge couplings in terms of dimension-eight effective field theory operators are also presented

    Measurement of the Splitting Function in &ITpp &ITand Pb-Pb Collisions at root&ITsNN&IT=5.02 TeV

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    Data from heavy ion collisions suggest that the evolution of a parton shower is modified by interactions with the color charges in the dense partonic medium created in these collisions, but it is not known where in the shower evolution the modifications occur. The momentum ratio of the two leading partons, resolved as subjets, provides information about the parton shower evolution. This substructure observable, known as the splitting function, reflects the process of a parton splitting into two other partons and has been measured for jets with transverse momentum between 140 and 500 GeV, in pp and PbPb collisions at a center-of-mass energy of 5.02 TeV per nucleon pair. In central PbPb collisions, the splitting function indicates a more unbalanced momentum ratio, compared to peripheral PbPb and pp collisions.. The measurements are compared to various predictions from event generators and analytical calculations.Peer reviewe

    Measurement of prompt open-charm production cross sections in proton-proton collisions at root s=13 TeV

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    The production cross sections for prompt open-charm mesons in proton-proton collisions at a center-of-mass energy of 13TeV are reported. The measurement is performed using a data sample collected by the CMS experiment corresponding to an integrated luminosity of 29 nb(-1). The differential production cross sections of the D*(+/-), D-+/-, and D-0 ((D) over bar (0)) mesons are presented in ranges of transverse momentum and pseudorapidity 4 < p(T) < 100 GeV and vertical bar eta vertical bar < 2.1, respectively. The results are compared to several theoretical calculations and to previous measurements.Peer reviewe

    Electroweak production of two jets in association with a Z boson in proton-proton collisions root s =13 TeV

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    A measurement of the electroweak (EW) production of two jets in association with a Z boson in proton-proton collisions at root s = 13 TeV is presented, based on data recorded in 2016 by the CMS experiment at the LHC corresponding to an integrated luminosity of 35.9 fb(-1). The measurement is performed in the lljj final state with l including electrons and muons, and the jets j corresponding to the quarks produced in the hard interaction. The measured cross section in a kinematic region defined by invariant masses m(ll) > 50 GeV, m(jj) > 120 GeV, and transverse momenta P-Tj > 25 GeV is sigma(EW) (lljj) = 534 +/- 20 (stat) fb (syst) fb, in agreement with leading-order standard model predictions. The final state is also used to perform a search for anomalous trilinear gauge couplings. No evidence is found and limits on anomalous trilinear gauge couplings associated with dimension-six operators are given in the framework of an effective field theory. The corresponding 95% confidence level intervals are -2.6 <cwww/Lambda(2) <2.6 TeV-2 and -8.4 <cw/Lambda(2) <10.1 TeV-2. The additional jet activity of events in a signal-enriched region is also studied, and the measurements are in agreement with predictions.Peer reviewe
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