Search results for "AYA"

showing 10 items of 358 documents

Measurements of |Vcb|, form factors and branching fractions in the decays → ℓ and → ℓ

1997

Two samples of exclusive semileptonic decays, 579 B0 -> D*+l-νl events and 261 B0 -> D+l-νl events, are selected from approximately 3.9 million hadronic Z decays collected by the ALEPH detector at LEP. From the reconstructed differential decay rate of each sample, the product of the hadronic form factor F(ω) at zero recoil of the D(*)+ meson and the CKM matrix element Vcb are measured to be FD*+ (1) Vcb = (31.9 +/- 1.8stat +/- 1.9syst) × 10-3,FD+ (1) Vcb = (27.8 +/- 6.8stat +/- 6.5syst) × 10-3. The ratio of the form factorsFD+ (1) and FD*+ (1) is measured to beFD+ (1)/FD*+ (1) = 0.87 +/- 0.22stat +/- 0.21syst. A value of Vcb is extracted from the two samples, using theoretical constraints o…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationHigh Energy Physics::PhenomenologyHadronCurvatureSpectral lineALEPH ExperimentRecoilHigh Energy Physics::ExperimentAtomic physicsALEPH experimentPhysics Letters B
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Minimal Flavour Violation and Multi-Higgs Models

2010

We propose an extension of the hypothesis of Minimal Flavour Violation (MFV) to general multi-Higgs models without the assumption of Natural Flavour Conservation (NFC) in the Higgs sector. We study in detail under what conditions the neutral Higgs couplings are only functions of V-CKM and propose a MFV expansion for the neutral Higgs couplings to fermions

PhysicsNuclear and High Energy PhysicsParticle physicsMinimal Flavour Violation010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesFCNCFermion01 natural sciencesHiggs sectorFlavour symmetriesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Multi-Higgs models0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsParticle Physics - Phenomenology
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Flavour constraints on multi-Higgs-doublet models: Yukawa alignment

2010

6 páginas, 3 figuras, 1 tabla.-- Talk given in the "Third Workshop on Theory, Phenomenology and Experiments in Heavy Flavour Physics" (Capri, 5-7 July 2010).

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral currentCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFermionAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonCP violationHigh Energy Physics::ExperimentPhenomenology (particle physics)
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The Proton Spectrum in Neutron Beta Decay: Latest Results with the aSPECT Spectrometer

2009

Abstract The purpose of the neutron decay spectrometer aSPECT is to determine the antineutrino electron angular correlation coefficient a with high precision. Latest measurements with aSPECT were performed during April/May 2008 at the Institut Laue-Langevin in Grenoble, France. In this paper we give a report on the experiment and the status of the ongoing data analysis.

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerProtonCabibbo–Kobayashi–Maskawa matrixSpectrum (functional analysis)ElectronBeta decayPhysics::GeophysicsNuclear physicsAngular correlationNeutronNuclear ExperimentNuclear Physics A
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Measurements of single top quark production cross sections and|Vtb|inpp¯collisions ats=1.96  TeV

2011

We present measurements of production cross sections of single top quarks in $\ppbar$ collisions at $\sqrt{s}=1.96\;\rm TeV$ in a data sample corresponding to an integrated luminosity of $5.4\;\rm fb^{-1}$ collected by the D0 detector at the Fermilab Tevatron Collider. We select events with an isolated electron or muon, an imbalance in transverse energy, and two, three, or four jets, with one or two of them containing a bottom hadron. We obtain an inclusive cross section of $\sigma({\ppbar}{\rargap}tb+X, tqb+X) = 3.43\pm^{0.73}_{0.74}\;\rm pb$ and use it to extract the CKM matrix element $0.79 < |V_{tb}| \leq 1$ at the 95% C.L. We also measure $\sigma({\ppbar}{\rargap}tb+X) = 0.68\pm^{0.38}…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHadronTevatron01 natural sciencesStandard ModelNuclear physics0103 physical sciencesProduction (computer science)010306 general physicsEnergy (signal processing)Physical Review D
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Measurement ofCPobservables inB±→DCPK±decays and constraints on the CKM angleγ

2010

Using the entire sample of 467×10^6 Υ(4S)→BB[overbar] decays collected with the BABAR detector at the PEP-II asymmetric-energy B factory at the SLAC National Accelerator Laboratory, we perform an analysis of B^± → DK^± decays, using decay modes in which the neutral D meson decays to either CP-eigenstates or non-CP-eigenstates. We measure the partial decay rate charge asymmetries for CP-even and CP-odd D final states to be A_(CP+) = 0.25±0.06±0.02 and A_(CP-) = -0.09±0.07±0.02, respectively, where the first error is the statistical and the second is the systematic uncertainty. The parameter A_(CP+) is different from zero with a significance of 3.6 standard deviations, constituting evidence f…

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarityMeson010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrix01 natural sciencesB-factoryNuclear physicsParticle decay0103 physical sciencesD mesonCP violationB meson010306 general physicsPhysical Review D
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Invariants and flavour in the general Two Higgs Doublet Model

2012

The flavour structure of the general Two Higgs Doublet Model (2HDM) is analysed and a detailed study of the parameter space is presented, showing that flavour mixing in the 2HDM can be parametrized by various unitary matrices which arise from the misalignment in flavour space between pairs of various Hermitian flavour matrices which can be constructed within the model. This is entirely analogous to the generation of the CKM matrix in the Standard Model (SM). We construct weak basis invariants which can give insight into the physical implications of any flavour model, written in an arbitrary weak basis (WB) in the context of 2HDM. We apply this technique to two special cases, models with MFV…

PhysicsNuclear and High Energy PhysicsParticle physicsfísica010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFlavourFOS: Physical sciencesUnitary matrixCP-violationParameter space01 natural sciencesHermitian matrixQuark mass matricesBaryogenesisHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)Two-Higgs-doublet modelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsParticle Physics - Phenomenology
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Polarization phenomena in Al/p-CdTe/Pt X-ray detectors

2013

Over the last decades, CdTe detectors are widely used for the development of room temperature X-ray and gamma ray spectrometers. Typically, high resolution CdTe detectors are fabricated with blocking contacts (indium, aluminum) ensuring low leakage currents and high electric field for optimum charge collection. As well known, time instability under bias voltage (termed as polarization) is the major drawback of CdTe diode detectors. Polarization phenomena cause a progressive degradation of the spectroscopic performance with time, due to hole trapping and detrapping from deep acceptors levels. In this work, we studied the polarization phenomenon on new Al/p-CdTe/Pt detectors, manufactured by …

PhysicsNuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryX-ray detectorchemistry.chemical_elementBiasingAcceptorCadmium telluride photovoltaicsSchottky CdTe detectorCondensed Matter::Materials SciencechemistryPolarizationElectric fieldActivation energyX-rayandgamma ray spectroscopyOptoelectronicsbusinessPolarization (electrochemistry)InstrumentationIndiumNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Measuring the proton spectrum in neutron decay - latest results with aSPECT

2008

The retardation spectrometer aSPECT was built to measure the shape of the proton spectrum in free neutron decay with high precision. This allows us to determine the antineutrino electron angular correlation coefficient a. We aim for a precision more than one order of magnitude better than the present best value, which is Delta_a /a = 5%. In a recent beam time performed at the Institut Laue-Langevin during April / May 2008 we reached a statistical accuracy of about 2% per 24 hours measurement time. Several systematic effects were investigated experimentally. We expect the total relative uncertainty to be well below 5%.

PhysicsNuclear and High Energy PhysicsSpectrometerProtonCabibbo–Kobayashi–Maskawa matrixFOS: Physical sciencesElectronMeasure (mathematics)Nuclear physicsNeutronNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationNuclear ExperimentOrder of magnitudeBeam (structure)
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Measurement of the t-channel single top-quark production cross section in pp collisions at s=7 TeV with the ATLAS detector

2012

We report a measurement of the cross section of single top-quark production in the t-channel using 1.04 fb -1 of pp collision data at s=7 TeV recorded with the ATLAS detector at the LHC. Selected e ...

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron ColliderChannel (digital image)Physics::Instrumentation and Detectors010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixAtlas detectorHigh Energy Physics::Phenomenology01 natural sciencesCross section (physics)medicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsPhysics Letters B
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