Search results for "Number"

showing 10 items of 3939 documents

Towards a superformula for neutrinoless double beta decay

1998

A general Lorentz--invariant parameterization for the long-range part of the $0\nu\beta\beta$ decay rate is derived. Combined with the short range part this general parameterization in terms of effective $B-L$ violating couplings will allow it to extract the $0\nu\beta\beta$ limits on arbitrary lepton number violating theories. Several new nuclear matrix elements appear in the general formalism compared to the standard neutrino mass mechanism. Some of these new matrix elements have never been considered before and are calculated within pn-QRPA. Using these, limits on lepton number violating parameters are derived from experimental data on $^{76}$Ge.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLepton numberFormalism (philosophy of mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SuperformulaDouble beta decayHigh Energy Physics::ExperimentNeutrino
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Invisible Higgs boson decays in spontaneously broken R parity

2004

The Higgs boson may decay mainly to an invisible mode characterized by missing energy, instead of the Standard Model channels. This is a generic feature of many models where neutrino masses arise from the spontaneous breaking of ungauged lepton number at relatively low scales, such as spontaneously broken R-parity models. Taking these models as framework, we reanalyze this striking suggestion in view of the recent data on neutrino oscillations that indicate non-zero neutrino masses. We show that, despite the smallness of neutrino masses, the Higgs boson can decay mainly to the invisible Goldstone boson associated to the spontaneous breaking of lepton number. This requires a gauge singlet su…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetryLepton numbersymbols.namesakeHiggs fieldHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-paritysymbolsHiggs bosonHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationHiggs mechanism
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LHC phenomenology of the μνSSM

2009

The $\mu\nu$SSM has been proposed to solve simultaneously the $\mu$-problem of the MSSM and explain current neutrino data. The model breaks lepton number as well as R-parity. In this paper we study the phenomenology of this proposal concentrating on neutrino masses and the decay of the lightest supersymmetric particle (LSP). At first we investigate in detail the $\mu\nu$SSM with one generation of singlets, which can explain all neutrino data, once 1-loop corrections are taken into account. Then we study variations of the model with more singlets, which can generate all neutrino masses and mixings at tree-level. We calculate the decay properties of the lightest supersymmetric particle, assum…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciencesLightest Supersymmetric ParticleLepton number0103 physical sciencesNeutralinoVertex (curve)High Energy Physics::ExperimentNeutrino010306 general physicsPhenomenology (particle physics)Journal of High Energy Physics
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Short-range mechanisms of neutrinoless double beta decay at the LHC

2013

Lepton number violation (LNV) mediated by short- range operators can manifest itself in both neutrinoless double beta decay (0 nu beta beta) and in processes with same- sign dilepton final states at the LHC. We derive limits from existing LHC data at root s = 8 TeV and compare the discovery potential of the forthcoming root s = 14 TeV phase of the LHC with the sensitivity of current and future 0 nu beta beta decay experiments, assuming the short-range part of the 0 nu beta beta decay amplitude dominates. We focus on the first of two possible topologies triggered by one fermion and two bosons in the intermediate state. In all cases, except for the pure leptoquark mechanism, the LHC will be m…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica01 natural sciences7. Clean energyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesHigh Energy Physics::ExperimentLepton number010306 general physicsHumanitiesMajorana neutrinosPhysical Review D
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Multiplicity dependence of jet-like two-particle correlation structures in p–Pb collisions at sNN=5.02 TeV

2015

Two-particle angular correlations between unidentified charged trigger and associated particles are measured by the ALICE detector in p-Pb collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV. The transverse-momentum range 0.7<pT,assoc<pT,trig<5.0 GeV/c is examined, to include correlations induced by jets originating from low momentum-transfer scatterings (minijets). The correlations expressed as associated yield per trigger particle are obtained in the pseudorapidity range |η|<0.9. The near-side long-range pseudorapidity correlations observed in high-multiplicity p-Pb collisions are subtracted from both near-side short-range and away-side correlations in order to remove the no…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsScatteringBinary number01 natural sciencesUncorrelatedNuclear physicsCorrelationPseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentMultiplicity (chemistry)Nuclear Experiment010306 general physicsGlauberPhysics Letters B
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Natural fourth generation of leptons

2009

We consider implications of a fourth generation of leptons, allowing for the most general mass patterns for the fourth generation neutrino. We determine the constraints due to the precision electroweak measurements and outline the signatures to search for at the LHC experiments. As a concrete framework to apply these results we consider the minimal walking technicolor (MWTC) model where the matter content, regarding the electroweak quantum numbers, corresponds to a fourth generation.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorQuantum numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Fourth generationHigh Energy Physics::ExperimentNeutrinoLepton
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How to pin down theCPquantum numbers of a Higgs boson in itsτdecays at the LHC

2011

We investigate how the $CP$ quantum numbers of a neutral Higgs boson or spin-zero resonance $\ensuremath{\Phi}$, produced at the CERN Large Hadron Collider, can be determined in its $\ensuremath{\tau}$-pair decay mode $\ensuremath{\Phi}\ensuremath{\rightarrow}{\ensuremath{\tau}}^{\ensuremath{-}}{\ensuremath{\tau}}^{+}$. We use a method [S. Berge and W. Bernreuther, Phys. Lett. B 671, 470 (2009).] based on the distributions of two angles and apply it to the major 1-prong $\ensuremath{\tau}$ decays. We show for the resulting dilepton, lepton-pion, and two-pion final states that appropriate selection cuts significantly enhance the discriminating power of these observables. From our analysis we…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyElementary particleQuantum numberStandard ModelNuclear physicssymbols.namesakeGenerationHiggs bosonsymbolsCP violationHigh Energy Physics::ExperimentHiggs mechanismPhysical Review D
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2017

A measurement of the time-integrated CP asymmetry in the Cabibbo-suppressed decay D0→K−K+ is performed using pp collision data, corresponding to an integrated luminosity of 3fb−1, collected with the LHCb detector at centre-of-mass energies of 7 and 8 TeV. The flavour of the charm meson at production is determined from the charge of the pion in D∗+→D0π+ and D∗−→D0¯π− decays. The time-integrated CP asymmetry ACP(K−K+) is obtained assuming negligible CP violation in charm mixing and in Cabibbo-favoured D0→K−π+, D+→K−π+π+ and D+→K0¯π+ decays used as calibration channels. It is found to be ACP(K−K+)=(0.14±0.15(stat)±0.10(syst))%. A combination of this result with previous LHCb measurements yield…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMeson010308 nuclear & particles physicsmedia_common.quotation_subject01 natural sciencesAsymmetry3. Good healthLuminosityNuclear physicsPion0103 physical sciencesCP violationCharm (quantum number)010306 general physicsmedia_commonPhysics Letters B
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Doubly charmed exotic mesons: A gift of nature?

2011

Article history: We study doubly charmed exotic states by solving the scattering problem of two D mesons. Our results point to the existence of a stable isoscalar doubly charmed meson with quantum numbers (I) J P = (0)1 + . We perform a thorough comparison to the results obtained within the hyperspherical harmonic formalism. Such exotic states could be measured at LHC and RHIC. Their experimental observation would,

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMesonIsoscalarNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelHadronQuantum numberLippmann–Schwinger equationNuclear physicsHadron spectroscopyHigh Energy Physics::ExperimentNuclear ExperimentPhysics Letters B
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LHC dijet constraints on double beta decay

2015

13 pages.- 5 figures

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics beyond the Standard ModelScalar (mathematics)High Energy Physics::PhenomenologyFísicaFOS: Physical sciencesLepton numberNuclear physicsDiquarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayLepton numberHigh Energy Physics::ExperimentNeutrinoMajorana neutrinosBoson
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