Search results for "physics beyond the standard model"

showing 10 items of 449 documents

Mixing asymmetries inBmeson systems, the D0 like-sign dimuon asymmetry, and generic new physics

2015

The measurement of a large like-sign dimuon asymmetry $A^b_{SL}$ by the D0 experiment at the Tevatron departs noticeably from Standard Model expectations and it may be interpreted as a hint of physics beyond the Standard Model contributing to $\Delta B\neq 0$ transitions. In this work we analyse how the natural suppression of $A^b_{SL}$ in the SM can be circumvented by New Physics. We consider generic Standard Model extensions where the charged current mixing matrix is enlarged with respect to the usual $3\times 3$ unitary Cabibbo-Kobayashi-Maskawa matrix, and show how, within this framework, a significant enhancement over Standard Model expectations for $A^b_{SL}$ is easily reachable throu…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard Modelmedia_common.quotation_subjectTevatronFísicaFOS: Physical sciencesAsymmetryHigh Energy Physics - Experiment3. Good healthStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)CP violationB mesonCharged currentMixing (physics)media_commonPhysical Review D
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Light vector mediators facing XENON1T data

2020

Recently the XENON1T collaboration has released new results on searches for new physics in low-energy electronic recoils. The data shows an excess over background in the low-energy tail, particularly pronounced at about $2-3$ keV. With an exposure of $0.65$ tonne-year, large detection efficiency and energy resolution, the detector is sensitive as well to solar neutrino backgrounds, with the most prominent contribution given by $pp$ neutrinos. We investigate whether such signal can be explained in terms of new neutrino interactions with leptons mediated by a light vector particle. We find that the excess is consistent with this interpretation for vector masses below $\lesssim 0.1$ MeV. The r…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsPhysics beyond the Standard ModelSolar neutrinoDetectorFOS: Physical sciencesParameter space01 natural scienceslcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Recoil0103 physical sciencesNeutrino010306 general physicslcsh:PhysicsBorexinoLeptonPhysics Letters
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Minimalistic Neutrino Mass Model

2000

We consider the simplest model which solves the solar and atmospheric neutrino puzzles, in the sense that it contains the smallest amount of beyond the Standard Model ingredients. The solar neutrino data is accounted for by Planck-mass effects while the atmospheric neutrino anomaly is due to the existence of a single right-handed neutrino at an intermediate mass scale between 10^9 GeV and 10^14 GeV. Even though the neutrino mixing angles are not exactly predicted, they can be naturally large, which agrees well with the current experimental situation. Furthermore, the amount of lepton asymmetry produced in the early universe by the decay of the right-handed neutrino is very predictive and ma…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoPhysics beyond the Standard Modelmedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAsymmetryUniverseHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoAnomaly (physics)BorexinoParticle Physics - PhenomenologyLeptonmedia_common
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Measurement of theCP-violation parameter ofB0mixing and decay withpp¯→μμXdata

2006

We measure the dimuon charge asymmetry A in p (p) over bar collisions at a center of mass energy root s=1960 GeV. The data was recorded with the D0 detector and corresponds to an integrated luminosity of approximately 1.0 fb(-1). Assuming that the asymmetry A is due to asymmetric B-0 (B) over bar (0) mixing and decay, we extract the CP-violation parameter of B-0 mixing and decay: ((epsilon B0))/(1+vertical bar epsilon B0 vertical bar 2)=(AB0)/(4)= -0.0023 +/- 0.0011(stat)+/- 0.0008(syst).A(B)(0) is the dimuon charge asymmetry from decays of B-0(B) over bar (0) pairs. The general case, with CP violation in both B-0 and B-s(0) systems, is also considered. Finally we obtain the forward-backwar…

PhysicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsmedia_common.quotation_subjectPhysics beyond the Standard Model01 natural sciencesAsymmetryNuclear physicsAntiproton0103 physical sciencesCP violationHigh Energy Physics::ExperimentInvariant massCenter of massNuclear Experiment010306 general physicsBar (unit)media_commonPhysical Review D
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One-loop effective lagrangian for an extension of the standard model with a heavy charged scalar singlet

1994

We study several problems related to the construction and the use of effective Lagrangians by considering an extension of the standard model that includes a heavy scalar singlet coupled to the leptonic doublet. Starting from the full renormalizable model, we build an effective field theory by integrating out the heavy scalar. A local effective Lagrangian (up to operators of dimension six) is obtained by expanding the one-loop effective action in inverse powers of the heavy mass. This is done by matching some Green functions calculated with both the full and the effective theories. Using this simple example we study the renormalization of effective Lagrangians in general and discuss how they…

PhysicsNuclear and High Energy PhysicsParticle physicsSpontaneous symmetry breakingPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyScalar (mathematics)Partícules (Física nuclear)RenormalizationStandard Model (mathematical formulation)Theoretical physicsEffective field theoryEffective actionPhenomenology (particle physics)Nuclear Physics B
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Sterile neutrinos with altered dispersion relations revisited

2020

In this paper we investigate neutrino oscillations with altered dispersion relations in the presence of sterile neutrinos. Modified dispersion relations represent an agnostic way to parameterize new physics. Models of this type have been suggested to explain global neutrino oscillation data, including deviations from the standard three-neutrino paradigm as observed by a few experiments. We show that, unfortunately, in this type of models new tensions arise turning them incompatible with global data.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrino010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - Experiment3. Good healthHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Dispersion relationBeyond Standard Model0103 physical scienceslcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physicsNeutrino oscillationJournal of High Energy Physics
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N_eff in low-scale seesaw models versus the lightest neutrino mass

2014

We evaluate the contribution to $N_{\rm eff}$ of the extra sterile states in low-scale Type I seesaw models (with three extra sterile states). We explore the full parameter space and find that at least two of the heavy states always reach thermalisation in the Early Universe, while the third one might not thermalise provided the lightest neutrino mass is below ${\mathcal O}(10^{-3}$eV). Constraints from cosmology therefore severely restrict the spectra of heavy states in the range 1eV- 100 MeV. The implications for neutrinoless double beta decay are also discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics beyond the Standard Modelmedia_common.quotation_subjectFOS: Physical sciencesFísicaUniverseNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryDouble beta decayMeasurements of neutrino speedNeutrinoNeutrino oscillationmedia_commonAstrophysics - Cosmology and Nongalactic Astrophysics
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Leptoquarks: Neutrino masses and related accelerator signals

2008

Leptoquark-Higgs interactions induce mixing between leptoquark (LQ) states with different chiralities once the electroweak symmetry is broken. In such LQ models Majorana neutrino masses are generated at 1-loop order. Here we calculate the neutrino mass matrix and explore the constraints on the parameter space enforced by the assumption that LQ-loops explain current neutrino oscillation data. LQs will be produced at the CERN LHC, if their masses are at or below the TeV scale. Since the fermionic decays of LQs are governed by the same Yukawa couplings, which are responsible for the nontrivial neutrino mass matrix, several decay branching ratios of LQ states can be predicted from measured neut…

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoGauge bosonMuonPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaNuclear physicsHiggs bosonHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLepton
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Flavor-changing Higgs boson decays into bottom and strange quarks in supersymmetric models

2015

In this work, we explore the flavor-changing decays ${H}_{i}\ensuremath{\rightarrow}bs$ in a general supersymmetric scenario. In these models the flavor-changing decays arise at loop level, but---because they originate from a dimension-four operator---they do not decouple and may provide a first sign of new physics for heavy masses beyond the reach of colliders. In the framework of the minimal supersymmetric extension of the Standard Model, we find that the largest branching ratio of the lightest Higgs (${H}_{1}$) is $\mathcal{O}(1{0}^{\ensuremath{-}6})$ after imposing present experimental constraints, while heavy Higgs states may still present branching ratios $\mathcal{O}(1{0}^{\ensuremat…

PhysicsNuclear and High Energy PhysicsParticle physicsStrange quarkLarge Hadron ColliderBranching fractionPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicalaw.inventionHiggs fieldlawHiggs bosonHigh Energy Physics::ExperimentColliderMinimal Supersymmetric Standard ModelPhysical Review D
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Amplitude analysis ofB0→K+π−π0and evidence of directCPviolation inB→K*πdecays

2011

We analyze the decay B0-->K+ pi- pi0 with a sample of 454 million B Bbar events collected by the BaBar detector at the PEP-II asymmetric-energy B factory at SLAC, and extract the complex amplitudes of seven interfering resonances over the Dalitz plot. These results are combined with amplitudes measured in B0-->K_S pi+ pi- decays to construct isospin amplitudes from B0-->K* pi and B0-->rho K decays. We measure the phase of the isospin amplitude Phi_3/2, useful in constraining the CKM unitarity triangle angle gamma and evaluate a CP rate asymmetry sum rule sensitive to the presence of new physics operators. We measure direct CP violation in B0-->K*+ pi- decays at the level of 3 sigma when mea…

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelElectron–positron annihilationDalitz plot01 natural sciencesB-factoryNuclear physicsParticle decayIsospin0103 physical sciencesCP violation010306 general physicsPhysical Review D
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