Search results for "Neutral Current"

showing 10 items of 301 documents

Neutrino electron scattering and electroweak gauge structure: Future tests

1997

Low-energy high-resolution neutrino-electron scattering experiments may play an important role in testing the gauge structure of the electroweak interaction. We propose the use of radioactive neutrino sources (e.g. $^{51}$Cr) in underground experiments such as BOREXINO, HELLAZ and LAMA. As an illustration, we display the sensitivity of these detectors in testing the possible existence of extra neutral gauge bosons, both in the framework of E_6 models and of models with left-right symmetry.

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsNeutral currentPhysics::Instrumentation and DetectorsElectroweak interactionAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaTechnicolorAstrophysicsSymmetry (physics)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoBorexinoCharged current
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Probing neutrino magnetic moments at the Spallation Neutron Source facility

2015

24 pages.- 8 figures

PhysicsNuclear and High Energy PhysicsNeutral currentGauge theoryPhysics beyond the Standard ModelFOS: Physical sciencesFísicaContext (language use)Lepton numberElectromagnetic propertiesStandard ModelNuclear physicsMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lepton numberNeutrinoSpallation Neutron SourceMajorana neutrinos
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The axial isoscalar neutral current from inelastic electron-nuclear scattering

1978

Abstract Parity violating effects due to neutral currents in isoscalar 0+→1+ nuclear transitions induced by electron scattering are enhanced owing to the small isoscalar magnetic dipole strength. A polarization asymmetry of the order 10−4 is expected at q ∼ 100 MeV for the 12C transition to the 1+(T = 0) state at 12.71 MeV. It would allow to single out the (electron vector current) × (hardonic axial isoscalar current) quantum numbers and couplings of the neutral current interaction.

PhysicsNuclear and High Energy PhysicsNeutral currentIsoscalarmedia_common.quotation_subjectNuclear TheoryFísicaParity (physics)ElectronQuantum numberAsymmetryNuclear physicsElectron scatteringMagnetic dipolemedia_commonParticle Physics - Phenomenology
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Contact Interactions with Polarized Beams at HERA

1998

The discovery potential of the HERA collider, with and without polarized beams, for electron-quark contact interactions in neutral current scattering is reviewed. The measurement of spin asymmetries in the polarized case could give crucial information on the chiral structure of new interactions.

PhysicsNuclear and High Energy PhysicsNeutral currentScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesHERAlaw.inventionNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentColliderSpin-½
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Forward Compton scattering with weak neutral current: Constraints from sum rules

2015

We generalize forward real Compton amplitude to the case of the interference of the electromagnetic and weak neutral current, formulate a low-energy theorem, relate the new amplitudes to the interference structure functions and obtain a new set of sum rules. We address a possible new sum rule that relates the product of the axial charge and magnetic moment of the nucleon to the 0th moment of the structure function $g_5(\nu,0)$. We apply the GDH and the finite energy sum rule for constraining the dispersive $\gamma Z$-box correction to the proton's weak charge.

PhysicsNuclear and High Energy PhysicsNuclear TheoryNeutral currentCompton scatteringFOS: Physical sciencesDuality (optimization)Charge (physics)Interference (wave propagation)lcsh:QC1-999Nuclear Theory (nucl-th)Moment (mathematics)High Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Sum rule in quantum mechanicsNuclear Experiment (nucl-ex)NucleonNuclear Experimentlcsh:Physics
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Search for the rare decay Bs 0→μ+μ-

2010

We present the results of a search for the flavor changing neutral current decay B-s(0) -> mu(+)mu(-) using 6.1 fb(-1) of p (p) over bar collisions at root s = 1.96 TeV collected by the D0 experiment at the Fermilab Tevatron Collider. The observed number of B-s(0) candidates is consistent with background expectations. The resulting upper limit on the branching fraction is B(B-s(0) -> mu(+)mu(-)) < 5.1 x 10(-8) at the 95% C.L. This limit is a factor of 2.4 better than that of the previous DO analysis and the best limit to date. Published by Elsevier B.V.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionFlavor-changing neutral currentTevatronD0 experimentRare decays01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesCP violationB-quarksFermilab010306 general physicsColliderb-quarksBar (unit)
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Search forD0→γγand improved measurement of the branching fraction forD0→π0π0

2015

Using 2.92 fb(-1) of electron-positron annihilation data collected at root s = 3.773 GeV with the BESIII detector, we report the results of a search for the flavor-changing neutral current process D-0 -> gamma gamma using a double-tag technique. We find no signal and set an upper limit at 90% confidence level for the branching fraction of B(D-0 -> gamma gamma pi(0)pi(0)) = (8.24 +/- 0.21(stat) +/- 0.30(syst)) x 10(-4), the most precise measurement to date and consistent with the current world average.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationNeutral current010308 nuclear & particles physicsBranching fractionElectron–positron annihilation01 natural sciencesGamma gammaNuclear physics0103 physical sciencesPi010306 general physicsPhysical Review D
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General flavor blind minimal supersymmetric standard model andCPviolation

2001

We study the implications on flavor changing neutral current and $\mathrm{CP}$ violating processes in the context of supersymmetric theories without a new flavor structure (flavor blind supersymmetry). The low-energy parameters are determined by the running of the soft breaking terms from the grand unified scale with supersymmetric (SUSY) phases consistent with the electric dipole moment constraints. We find that the $\mathrm{CP}$ asymmetry in $\stackrel{\ensuremath{\rightarrow}}{b}s\ensuremath{\gamma}$ can reach large values potentially measurable at B factories, especially in the low $BR(\stackrel{\ensuremath{\rightarrow}}{b}s\ensuremath{\gamma})$ region, while the contributions to electr…

PhysicsNuclear and High Energy PhysicsParticle physicsAnomalous magnetic dipole moment010308 nuclear & particles physicsFlavor-changing neutral currentHigh Energy Physics::PhenomenologySupersymmetry01 natural sciencesElectric dipole momentChargino0103 physical sciencesGrand Unified TheoryCP violationHigh Energy Physics::Experiment010306 general physicsMinimal Supersymmetric Standard ModelPhysical Review D
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νd→μ−Δ++nreaction and axial vectorN−Δcoupling

1999

The reaction $\ensuremath{\nu}\stackrel{\ensuremath{\rightarrow}}{d}{\ensuremath{\mu}}^{\ensuremath{-}}{\ensuremath{\Delta}}^{++}n$ is studied in the region of low ${q}^{2}$ to investigate the effect of deuteron structure and width of the $\ensuremath{\Delta}$ resonance on the differential cross section. The results are used to extract the axial vector $N\ensuremath{-}\ensuremath{\Delta}$ coupling ${C}_{5}^{A}$ from the experimental data on this reaction. The possibility to determine this coupling from electroweak interaction experiments with high intensity electron accelerators is discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsDeuteriumNeutral currentElectroweak interactionResonanceElectronAtomic physicsCoupling (probability)PseudovectorCharged currentPhysical Review C
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Restricted flavor structure of soft SUSY breaking trilinear couplings

2000

We analyze the flavor structure of the trilinear couplings in the different theoretical models of SUSY breaking. We generically obtain A_{ij}= A^L_i + A^R_j in all the models examined. In fact, this is the rigorous form when SUSY breaking effects appear through the Kahler metric of chiral fields or through wave-function renormalization. Indeed, the low-energy phenomenological requirements from the absence of charge and color breaking minima and the measurements in flavor changing neutral current (FCNC) observables strongly favor this restricted form of the trilinear matrices. As a straightforward consequence, the number of unknown parameters associated with the trilinear couplings is decrea…

PhysicsNuclear and High Energy PhysicsParticle physicsFlavor-changing neutral currentHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyStructure (category theory)FOS: Physical sciencesCharge (physics)ObservableSupersymmetryMaxima and minimaRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Soft SUSY breakingHigh Energy Physics::Experiment
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