Next to leading order eta production at hadron colliders

Inclusive eta production at hadron colliders is considered,based on evaluation of eta fragmentation functions at next to leading order. Absolute predictions at LHC and SSC are presented, including the ratio $\eta/\pi^0$, together with the estimate of the theoretical uncertainty, as a possible neutral background to the $H\to \gamma\gamma$ detection.Comment: 8 pages, latex, FNT/T-93/13,14 figures avilable upon reques

Homocysteine induces cell death in H9C2 cardiomyocytes through the generation of peroxynitrite

Homocysteine (HCY) is toxic on blood vessels, but a potential direct toxicity of HCY on the heart is unknown. We addressed this issue by exposing H9C2 cardiomyocytes to HCY (0.1-5 mM) for up to 6h. At these concentrations, HCY reduced cell viability, induced necrosis and apoptosis and triggered the cleavage of caspase-3 and poly(ADP-ribose) polymerase (PARP). This was associated with the intracellular generation of the potent oxidant peroxynitrite. Removing peroxynitrite by the decomposition catalyst FeTPPS considerably reduced LDH release, DNA fragmentation, cleavage of caspase-3 and PARP, and restored normal cell morphology. In additional experiments performed in primary rat ventricular cardiomyocytes, HCY (1 mM, 6h) activated the phosphorylation of the MAP kinases ERK and JNK, two essential stress signaling kinases regulating myocardial apoptosis, hypertrophy and remodeling. These results provide the first demonstration that HCY kills cardiomyocytes through the generation of peroxynitrite and can activate key signaling cascades in the myocardium

Peroxynitrite is a potent inhibitor of NF-{kappa}B activation triggered by inflammatory stimuli in cardiac and endothelial cell lines.

Peroxynitrite is a potent oxidant and nitrating species proposed as a direct effector of myocardial damage in numerous cardiac pathologies. Whether peroxynitrite also acts indirectly, by modulating cell signal transduction in the myocardium, has not been investigated. Therefore, we examined a possible role for peroxynitrite on the activation of NF-kappaB, a crucial pro-inflammatory transcription factor, in cultured H9C2 cardiomyocytes. H9C2 cells were stimulated with tumor necrosis factor-alpha or lipopolysaccharide following a brief (20-min) exposure to peroxynitrite. NF-kappaB activation (phosphorylation and degradation of its inhibitor IkappaBalpha, nuclear translocation of NF-kappaB p65, and NF-kappaB DNA binding) triggered by lipopolysaccharide or tumor necrosis factor-alpha was abrogated by peroxynitrite. Peroxynitrite also inhibited NF-kappaB in two human endothelial cell lines activated with tumor necrosis factor-alpha or interleukin-1beta. These effects were related to oxidative but not nitrative chemistry and were still being observed while nitration was suppressed by epicatechin. The mechanism of NF-kappaB inhibition by peroxynitrite was a complete blockade of phosphorylation and activation of the upstream kinase IkappaB kinase (IKK) beta, required for canonical, pro-inflammatory NF-kappaB activation. At the same time, peroxynitrite activated phosphorylation of NF-kappaB-inducing kinase and IKKalpha, considered as part of an alternative, noncanonical NF-kappaB activation pathway. Suppression of IKKbeta-dependent NF-kappaB activation translated into a marked inhibition of the transcription of NF-kappaB-dependent genes by peroxynitrite. Thus, peroxynitrite has a dual effect on NF-kappaB, inhibiting canonical IKKbeta-dependent NF-kappaB activation while activating NF-kappaB-inducing kinase and IKKalpha phosphorylation, which suggests its involvement in an alternative pathway of NF-kappaB activation. These findings offer new perspectives for the understanding of the relationships between redox stress and inflammation

QCD results from the Fermilab Tevatron p¯p Collider

Several selected quantum chromodynamics (QCD) measurements performed at the Fermilab Tevatron by the CDF and D0 Collaborations, using proton-antiproton collisions at a centre-of-mass energy of √s = 1.96TeV are reviewed. We will summarize the status of inclusive jet and dijet production crosssection measurements, which can be used to extract a precise value of the strong coupling constant and to search for physics beyond the Standard Model. We will then review results from the inclusive photon production cross-section measurement, as well as the associated production of photon with a light or heavy flavors jet. Finally we will describe various measurements concerning the production of vector bosons and jets

Proceedings of the Workshop on Monte Carlo's, Physics and Simulations at the LHC PART II

These proceedings collect the presentations given at the first three meetings of the INFN "Workshop on Monte Carlo's, Physics and Simulations at the LHC", held at the Frascati National Laboratories in 2006. The first part of these proceedings contains pedagogical introductions to several basic topics of both theoretical and experimental high pT LHC physics. The second part collects more specialised presentations.Comment: 157 pages, 136 figures; contribution by M. Grazzini has been adde

Measurement of the ttbar Production Cross Section in ppbar Collisions at sqrt(s) = 1.96 TeV

We present a measurement of the top quark pair production cross section in ppbar collisions at sqrt(s)=1.96 TeV using 318 pb^{-1} of data collected with the Collider Detector at Fermilab. We select ttbar decays into the final states e nu + jets and mu nu + jets, in which at least one b quark from the t-quark decays is identified using a secondary vertex-finding algorithm. Assuming a top quark mass of 178 GeV/c^2, we measure a cross section of 8.7 +-0.9 (stat) +1.1-0.9 (syst) pb. We also report the first observation of ttbar with significance greater than 5 sigma in the subsample in which both b quarks are identified, corresponding to a cross section of 10.1 +1.6-1.4(stat)+2.0-1.3 (syst) pb.Comment: Accepted for publication in Physics Review Letters, 7 page

Search for the Supersymmetric Partner of the Top-Quark in ppˉp \bar{p} Collisions at s=1.8TeV\sqrt{s} = 1.8 {\rm TeV}

We report on a search for the supersymmetric partner of the top quark (stop) produced in $t \bar{t}$ events using $110 {\rm pb}^{-1}$ of $p \bar{p}$ collisions at $\sqrt{s} = 1.8 {\rm TeV}$ recorded with the Collider Detector at Fermilab. In the case of a light stop squark, the decay of the top quark into stop plus the lightest supersymmetric particle (LSP) could have a significant branching ratio. The observed events are consistent with Standard Model $t \bar{t}$ production and decay. Hence, we set limits on the branching ratio of the top quark decaying into stop plus LSP, excluding branching ratios above 45% for a LSP mass up to 40 {\rm GeV/c}$^{2}$.Comment: 11 pages, 4 figure