Search results for "Fermi"

showing 10 items of 1388 documents

Charge asymmetry in hadroproduction of heavy quarks

1998

A sizeable difference in the differential production cross section of top and antitop quarks, respectively, is predicted for hadronically produced heavy quarks. It is of order $\alpha_s$ and arises from the interference between charge odd and even amplitudes respectively. For the TEVATRON it amounts to approximately 5-10% in the region where the cross section is large and could therefore be measured in the next round of experiments. At the LHC the asymmetry can be studied by selecting appropriately chosen kinematical regions.

QuarkPhysicsParticle physicsLarge Hadron Collidermedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronFísicaGeneral Physics and AstronomyOrder (ring theory)FOS: Physical sciencesCharge (physics)AsymmetryNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Production (computer science)High Energy Physics::ExperimentFermilabmedia_common
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The effect of hyperfine mixing in electromagnetic and semileptonic decays of doubly heavy baryons

2010

We consider the role played by hyperfine mixing in electromagnetic and semileptonic decays of doubly heavy baryons, which give rise to large corrections to the decay widths in both cases.

QuarkPhysicsParticle physicsNuclear TheoryHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleFermionBaryonNuclear Theory (nucl-th)Particle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear ExperimentHyperfine structureMixing (physics)
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Sensitivity to charged scalars in B → D(*)τν and B → τν decays

2013

We analyze the recent experimental evidence for an excess of $\tau$-lepton production in several exclusive semileptonic $B$-meson decays in the context of two-Higgs-doublet models. These decay modes are sensitive to the exchange of charged scalars and constrain strongly their Yukawa interactions. While the usual Type-II scenario cannot accommodate the recent BaBar data, this is possible within more general models in which the charged-scalar couplings to up-type quarks are not as suppressed. Both the $B\to D^{(*)}\tau\nu_\tau$ and the $B\to\tau\nu_\tau$ data can be fitted within the framework of the Aligned Two-Higgs-Doublet Model, but the resulting parameter ranges are in conflict with the …

QuarkPhysicsParticle physicsNuclear and High Energy PhysicsB-Physics; Beyond Standard Model; High Energy Physics - Phenomenology; High Energy Physics - Phenomenology; High Energy Physics - Experiment; Nuclear and High Energy PhysicsPhysics beyond the Standard ModelB-PhysicsHigh Energy Physics::PhenomenologyScalar (mathematics)Yukawa potentialContext (language use)FermionHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyBeyond Standard ModelHigh Energy Physics::ExperimentProduction (computer science)Charm (quantum number)
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Flavour geometry and effective Yukawa couplings in the MSSM

2010

We present a new geometric approach to the flavour decomposition of an arbitrary soft supersymmetry-breaking sector in the MSSM. Our approach is based on the geometry that results from the quark and lepton Yukawa couplings, and enables us to derive the necessary and sufficient conditions for a linearly-independent basis of matrices related to the completeness of the internal [SU(3) circle times U(1)](5) flavour space. In a second step, we calculate the effective Yukawa couplings that are enhanced at large values of tan beta for general soft supersymmetry-breaking mass parameters. We highlight the contributions due to non-universal terms in the flavour decompositions of the sfermion mass mat…

QuarkPhysicsParticle physicsNuclear and High Energy PhysicsBasis (linear algebra)010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaGeometrySpace (mathematics)01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Sfermion0103 physical sciencesHigh Energy Physics::ExperimentBoundary value problem010306 general physicsLeptonParticle Physics - Phenomenology
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Improved measurements of electroweak parameters from Z decays into fermion pairs

1992

The properties of the Z resonance are measured on the basis of 190000 Z decays into fermion pairs collected with the ALEPH detector at LEP. Assuming lepton universality, M(Z) = (91.182 +/- 0.009exp +/- 0.020L;P) GeV, GAMMA(Z) = (2484 +/- 17) MeV, sigma(had)0 = (41.44 +/- 0.36) nb, and GAMMA(had)/GAMMA(ll) = 21.00 +/- 0.20. The corresponding number of light neutrino species is 2.97 +/- 0.07. The forward-backward asymmetry in leptonic decays is used to determine the ratio of vector to axial-vector coupling constants of leptons: g(V)2(M(Z)2)/g(A)2(M(Z)2) = 0.0072 +/- 0.0027. Combining these results with ALEPH results on quark charge and bbBAR asymmetries, and tau-polarization, sin2 theta(W)(M(…

QuarkPhysicsParticle physicsPhysics and Astronomy (miscellaneous)Electron–positron annihilationHigh Energy Physics::PhenomenologyElectroweak interactionElementary particleWeinberg angleFermionALEPH detectorNuclear physicsHigh Energy Physics::ExperimentNeutrinoEngineering (miscellaneous)Particle Physics - ExperimentLepton
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Measurement ofW-Boson Polarization in Top-Quark Decay inpp¯Collisions ats=1.96  TeV

2010

We report measurements of the polarization of W bosons from top-quark decays using 2.7 fb(-1) of p (p) over bar collisions collected by the CDF II detector. Assuming a top-quark mass of 175 GeV/c(2), three measurements are performed. A simultaneous measurement of the fraction of longitudinal (f(0)) and right-handed (f(0)) W bosons yields the model- independent results f(0) =0. 88 +/- 0.11(stat) +/- 0.06(syst) and f(+) = 0.15 +/- 0.07(stat) +/- 0.06(syst) with a correlation coefficient of -0.59. A measurement of f(0) [f(+)] constraining f(+) [f(0)] to its standard model value of 0.0 [0.7] yields f(0) 0.70 + 0.07(stat) +/- 0.04(syst) [f(+) - 0.01 +/- 0.02(stat) +/- 0.05(syst)]. All these resu…

QuarkPhysicsParticle physicsTop quark010308 nuclear & particles physicsGeneral Physics and AstronomyElementary particleFermion01 natural sciencesHelicityNuclear physicsPair production0103 physical sciencesGrand Unified Theory010306 general physicsBosonPhysical Review Letters
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Search for 3- and 4-body decays of the scalar top quark in pp- collisions at root s = 1.8 TeV

2004

Abstract We have searched for the signature of 3- and 4-body decays of pair-produced scalar top quarks (stop) in the inclusive final state containing an electron, a muon, and significant missing transverse energy using a sample of p p events corresponding to 108.3 pb−1 of data collected with the DO detector at Fermilab. The search is done in the framework of the minimal supersymmetric standard model assuming that the neutralino ( χ 0 1 ) is the lightest supersymmetric particle and is stable. No evidence for a signal is found and we derive cross-section upper limits as a function of stop (t) and neutralino masses in different decay scenarios leading to the blν χ 0 1 final state.

QuarkPhysicsParticle physicsTop quarkNuclear and High Energy PhysicsMuon010308 nuclear & particles physicsScalar (mathematics)High Energy Physics::Phenomenology01 natural sciencesLightest Supersymmetric ParticleNuclear physics0103 physical sciencesNeutralinoHigh Energy Physics::ExperimentFermilab010306 general physicsMinimal Supersymmetric Standard ModelPhysics Letters B
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BK from the lattice with Wilson quarks

2004

We report our results for the bag-parameter BK obtained from the quenched simulations on the lattice with Wilson fermions at three values of the lattice spacing. We implemented the method by which no subtraction of the mixing with other four-fermion dS=2 operators is needed. Our final result, in terms of the renormalisation group invariant bag-parameter, is BK = 0.96 +/- 0.10.

QuarkPhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciences[PHYS.HLAT] Physics [physics]/High Energy Physics - Lattice [hep-lat]Fermion01 natural sciencesHigh Energy Physics - LatticeLattice constantLattice (order)0103 physical sciences010306 general physicsEngineering (miscellaneous)Mathematical physics
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Nonperturbative renormalization and O(a) -improvement of the nonsinglet vector current with Nf=2+1 Wilson fermions and tree-level Symanzik improved g…

2019

In calculating hadronic contributions to precision observables for tests of the Standard Model in lattice QCD, the electromagnetic current plays a central role. Using a Wilson action with $\mathrm{O}(a)$ improvement in QCD with ${N}_{\mathrm{f}}$ flavors, a counterterm must be added to the vector current in order for its on-shell matrix elements to be $\mathrm{O}(a)$ improved. In addition, the local vector current, which has support on one lattice site, must be renormalized. At $\mathrm{O}(a)$, the breaking of the $\mathrm{SU}({N}_{\mathrm{f}})$ symmetry by the quark mass matrix leads to a mixing between the local currents of different quark flavors. We present a nonperturbative calculation…

QuarkPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryLattice QCDFermionMass matrix01 natural sciencesRenormalizationLattice (order)0103 physical sciences010306 general physicsMathematical physicsPhysical Review D
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A solution to the strong CP problem transforming the theta angle to the KM CP-violating phase

2010

It is shown that in the scheme with a rotating fermion mass matrix (i.e. one with a scale-dependent orientation in generation space) suggested earlier for explaining fermion mixing and mass hierarchy, the theta angle term in the QCD action of topological origin can be eliminated by chiral transformations, while giving still nonzero masses to all quarks. Instead, the effects of such transformations get transmitted by the rotation to the CKM matrix as the KM phase giving, for theta of order unity, a Jarlskog invariant typically of order 10(-5), as experimentally observed. Strong and weak CP violations appear then as just two facets of the same phenomenon.

QuarkPhysicsQuantum chromodynamicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstronomy and AstrophysicsFermionAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)CP violationStrong CP problemInvariant (mathematics)Mixing (physics)
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