0000000000210550

AUTHOR

Gabriela Barenboim

showing 94 related works from this author

NEUTRINO SPECTRUM IN NONSUPERSYMMETRIC SO(10)

1996

We present a predictive scheme for fermion masses and mixings inspired by nonsupersymmetric SO(10) in which the hierarchy problem is resolved without fine tuning the Yukawa couplings. This calls for a nonminimal Higgs sector which we exploit in deriving the expressions for the mass matrices. To keep the predictivity of the model under control we limit the structure of the mass matrices by imposing U(1) symmetries. A very predictive neutrino spectrum is then obtained.

PhysicsNuclear and High Energy PhysicsFine-tuningParticle physicsHigh Energy Physics::PhenomenologyYukawa potentialGeneral Physics and AstronomyAstronomy and AstrophysicsHierarchy problemFermionHiggs sectorLimit (mathematics)NeutrinoSO(10)Modern Physics Letters A
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Impact of CP-violation on neutrino lepton number asymmetries revisited

2017

We revisit the effect of the (Dirac) CP-violating phase on neutrino lepton number asymmetries in both mass- and flavor-basis. We found that, even if there are sizable effects on muon- and tau-neutrino asymmetries, the effect on the asymmetry of electron-neutrinos is at most similar to the upper bound set by BBN for initial neutrino degeneracy parameters smaller than order unity. We also found that, for the asymmetries in mass-basis, the changes caused by CP-violation is of sub-\% level which is unlikely to be accesible neither in the current nor in the forthcoming experiments.

Particle physicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics::Instrumentation and Detectorsmedia_common.quotation_subjectFOS: Physical sciences01 natural sciencesAsymmetryNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationmedia_commonPhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLepton numberlcsh:QC1-999Massless particleHigh Energy Physics - PhenomenologyCP violationHigh Energy Physics::ExperimentNeutrinolcsh:PhysicsLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Structure formation during an early period of matter domination

2014

In this work we show that modifying the thermal history of the Universe by including an early period of matter domination can lead to the formation of astronomical objects. However, the survival of these objects can only be possible if the dominating matter decays to a daughter particle which is not only almost degenerate with the parent particle but also has an open annihilation channel. This requirement translates in an upper bound for the coupling of such a channel and makes the early structure formation viable.

PhysicsAstronomical ObjectsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Structure formation010308 nuclear & particles physicsDegenerate energy levelsFOS: Physical sciencesFísicaAstrophysics16. Peace & justice01 natural sciencesUpper and lower boundsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesParticle010303 astronomy & astrophysicsPeriod (music)Astrophysics - Cosmology and Nongalactic AstrophysicsJournal of High Energy Physics
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Tree-level flavor-changing neutral currents in theBsystem: FromCPasymmetries to rare decays

2001

corresponding to 0.59 ≤ sin(2�) ≤ 0.82, which is cer- tainly outside the 1� Babar range but not outside the world average. This potential discrepancy is at the ori- gin of several papers (6) studying the implications of a small aJ/ in the search of new physics. In this paper, we analyze the implications of this situ- ation for a realistic model, obtained with the only addi- tion of an isosinglet down vector-like quark (7) to the SM spectrum. This model naturally arises, for instance, as the low-energy limit of an E6 grand unified theory. At a more phenomenological level, models with isosinglet quarks provide the simplest self-consistent framework to study deviations of 3 ×3 unitarity of the…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelGrand Unified TheoryB mesonQuarkoniumStandard ModelPhysical Review D
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Flavor violation in supersymmetric SU(5) GUT at large tan beta

2001

We study flavor violation in the general SUSY SU(5) GUT assuming all the third generation Yukawa couplings to be due to the renormalizable physics above GUT scale. At large tan beta, as suggested by Yukawa unification in SU(5), sizable flavor violation in the left (right) slepton (down squark) sector can be induced in nonminimal models due to renormalization effects of down type Yukawa couplings between GUT and Planck scales, in addition to the flavor violation in the right slepton sector. The new flavor physics contribution to K-(K) over bar, B-(B) over bar mixing is small but might be of phenomenological interest in the case of b --> s gamma. The sign of the latter contribution is the sam…

PhysicsNuclear and High Energy PhysicsParticle physicsBranching fractionHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFísicaElementary particleSupersymmetryRenormalizationCharginoHigh Energy Physics::ExperimentLepton
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Spontaneous breakdown of CP in left right symmetric models

1997

We show that it is possible to obtain spontaneous CP violation in the minimal SU(2)L × SU(2)R × U(1)B -L, i.e. in a left right symmetric model containing a bidoublet and two triplets in the scalar sector. For this to be a natural scenario, the non-diagonal quartic couplings between the two scalar triplets and the bidoublet play a fundamental role. We analyze the corresponding Higgs spectrum, the suppression of FCNC’s and the manifestation of the spontaneous CP phase in the electric dipole moment of the electron.

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)Spontaneous symmetry breakingScalar (mathematics)High Energy Physics::PhenomenologySymmetric modelFísicaElectronElectric dipole momentQuartic functionHiggs bosonCP violation
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The (relative) size does not matter in inflation

2015

We show that a tiny correction to the inflaton potential can make critical changes in the inflationary observables for some types of inflation models.

High Energy Physics - PhenomenologyCosmology and Nongalactic Astrophysics (astro-ph.CO)High Energy Physics - Phenomenology (hep-ph)FOS: Physical sciencesAstrophysics - Cosmology and Nongalactic Astrophysics
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CPT Violating Decoherence and LSND: a possible window to Planck scale Physics

2004

Decoherence has the potential to explain all existing neutrino data including LSND results, without enlarging the neutrino sector. This particular form of CPT violation can preserve the equality of masses and mixing angles between particle and antiparticle sectors, and still provide seizable differences in the oscillation patterns. A simplified minimal model of decoherence is sufficient to explain the existing neutrino data quite neatly, while making dramatic predictions for the upcoming experiments. Some comments on the order of the decoherence parameters in connection with theoretically expected values from some models of quantum-gravity are given. In particular, the quantum gravity decoh…

PhysicsNuclear and High Energy PhysicsParticle physicsAntiparticleQuantum decoherenceOscillationHigh Energy Physics::PhenomenologyFOS: Physical sciencesMinimal modelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dark energyQuantum gravityHigh Energy Physics::ExperimentNeutrinoMixing (physics)
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Light neutrino masses from gravitational condensation: the Schwinger-Dyson approach

2019

In this work we demonstrate that non-zero neutrino masses can be generated from gravitational interactions. We solve the Schwinger-Dyson equations to find a non-trivial vacuum thereby determining the scale of the neutrino condensate and the number of new particle degrees of freedom required for gravitationally induced dynamical chiral symmetry breaking. We show for minimal beyond the Standard Model particle content, the scale of the condensation occurs close to the Planck scale.

High Energy Physics - TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)FOS: Physical sciences
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Light charged Higgs at the beginning of the LHC era

2008

The terascale will be explored with the start of the LHC. One of the most fundamental questions which we expect to be answered is the root of electroweak symmetry breaking and whether the Higgs mechanism is realized in nature or not. In this context we pose the question if existing experimental data still allow for a light non-minimal Higgs sector. We tackle this question first in the context of the two Higgs doublet model and then we concentrate in two supersymmetric models, the constrained MSSM and the MSSM with non-universal Higgs masses. In both supersymmetric scearios, light pseudoscalar and light charged-Higgs bosons are still viable provided tan beta is large. In this regime, we emph…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHiggs physicsContext (language use)Higgs sectorHiggs physics; Supersymmetry phenomenology; Nuclear and High Energy PhysicsSupersymmetry phenomenologyTwo-Higgs-doublet modelsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonsymbolsHigh Energy Physics::ExperimentHiggs mechanismBoson
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Improved tau-lepton tools for Higgs boson hunting

2014

In this work, we use the results from Higgs searches in the $\gamma\gamma$ and $\tau\tau$ decay channels at LHC and indirect bounds as BR$(B \to X_s \gamma)$ to constrain the parameter space of a generic MSSM Higgs sector. In particular, we include the latest CMS results that look for additional Higgs states with masses up to 1 TeV. We show that the $\tau \tau$ channel is the best and most accurate weapon in the hunt for new Higgs states beyond the Standard Model. We obtain that present experimental results rule out additional neutral Higgs bosons in a generic MSSM below 300 GeV for any value of $\tan \beta$ and, for instance, values of $\tan \beta$ above 30 are only possible for Higgs mass…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaParameter space01 natural sciencesHiggs sectormedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesHiggs bosonmedicineHigh Energy Physics::Experiment010306 general physicsBoson
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Colliders as a simultaneous probe of supersymmetric dark matter and Terascale cosmology

2006

Terascale supersymmetry has the potential to provide a natural explanation of the dominant dark matter component of the standard lambda-CDM cosmology. However once we impose the constraints on minimal supersymmetry parameters from current particle physics data, a satisfactory dark matter abundance is no longer prima facie natural. This Neutralino Tuning Problem could be a hint of nonstandard cosmology during and/or after the Terascale era. To quantify this possibility, we introduce an alternative cosmological benchmark based upon a simple model of quintessential inflation. This benchmark has no free parameters, so for a given supersymmetry model it allows an unambiguous prediction of the da…

PhysicsInflation (cosmology)Nuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderAstrophysics (astro-ph)Dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetryAstrophysics::Cosmology and Extragalactic AstrophysicsParameter spaceAstrophysicsCMB cold spotCosmologyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Neutralino
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Peccei–Quinn field for inflation, baryogenesis, dark matter, and much more

2016

We propose a scenario of brane cosmology in which the Peccei-Quinn field plays the role of the inflaton and solves simultaneously many cosmological and phenomenological issues such as the generation of a heavy Majorana mass for the right-handed neutrinos needed for seesaw mechanism, MSSM $\mu$-parameter, the right amount of baryon number asymmetry and dark matter relic density at the present universe, together with an axion solution to the strong CP problem without the domain wall obstacle. Interestingly, the scales of the soft SUSY-breaking mass parameter and that of the breaking of $U(1)_{\rm PQ}$ symmetry are lower bounded at $\mathcal{O}(10) {\mathrm TeV}$ and $\mathcal{O}(10^{11}) {\ma…

PhysicsInflation (cosmology)Particle physicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsInflaton01 natural scienceslcsh:QC1-999BaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBrane cosmologyStrong CP problemHigh Energy Physics::Experiment010306 general physicsAxionlcsh:PhysicsAstrophysics - Cosmology and Nongalactic AstrophysicsPhysics Letters B
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Inflation might be caused by the right

2009

15 pages, 4 figures.-- ISI article identifier: 000265600800102.-- ArXiv pre-print avaible at: http://arxiv.org/abs/0811.2998

Inflation (cosmology)PhysicsNuclear and High Energy PhysicsParticle physicsBeyond Standard ModelAstrophysics (astro-ph)FOS: Physical sciencesElementary particleFermionInflatonAstrophysicsMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Neutrino PhysicsNeutrinoScalar fieldComputer Science::DatabasesLeptonCosmology of Theories beyond the SM
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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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Diagnostic Potential of Cosmic-Neutrino Absorption Spectroscopy

2004

Annihilation of extremely energetic cosmic neutrinos on the relic-neutrino background can give rise to absorption lines at energies corresponding to formation of the electroweak gauge boson $Z^{0}$. The positions of the absorption dips are set by the masses of the relic neutrinos. Suitably intense sources of extremely energetic ($10^{21}$ -- $10^{25}$-eV) cosmic neutrinos might therefore enable the determination of the absolute neutrino masses and the flavor composition of the mass eigenstates. Several factors--other than neutrino mass and composition--distort the absorption lines, however. We analyze the influence of the time-evolution of the relic-neutrino density and the consequences of …

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsCosmologiaPhysics::Instrumentation and Detectorsmedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaDark matterAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysicsPartícules (Física nuclear)UniverseCosmic neutrino backgroundHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedInvariant massHigh Energy Physics::ExperimentAbsorption (logic)Neutrinomedia_common
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Unduland universe: expansion with alternating eras of acceleration and deceleration

2005

If the equation of state for 'dark energy' varies periodically, the expansion of the Universe may have undergone alternating eras of acceleration and deceleration. We examine a specific form that survives existing observational tests, does not single out the present state of the Universe as exceptional, and suggests a future much like the matter-dominated past: a smooth expansion without a final inflationary epoch.

PhysicsNuclear and High Energy PhysicsCosmologiaSteady State theoryBig RipAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsParticle horizonMetric expansion of spaceDe Sitter universeDark energyInflationary epochScale factor (cosmology)
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Combining LSND and Atmospheric Anomalies in a Three-Neutrino Picture

2001

We investigate the three-neutrino mixing scheme for solving the atmospheric and LSND anomalies. We find the region in the parameter space that provides a good fit to the LSND and the SK atmospheric data, taking into account the CHOOZ constraint. We demonstrate that the goodness of this fit is comparable to that of the conventional fit to the solar and atmospheric data. Large values of the LSND angle are favoured and $\sin^2(2\theta_{\rm LSND})$ can be as high as 0.1. This can have important effects on the atmospheric electron neutrino ratios as well as on down-going multi-GeV muon neutrino ratios. We examine the possibility of distinguishing this scheme from the conventional one at the long…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsFísicaFOS: Physical sciencesParameter spaceCHOOZNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Muon neutrinoHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationElectron neutrinoMixing (physics)Particle Physics - Phenomenology
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(Standard model) universe dominated by the right matter

2009

14 pages, 3 figures. References on late time enthropy release included, several points clarified. PACS numbers: 14.60.Pq, 98.80.Cq. ArXiv pre-print available at http://arxiv.org/abs/0806.4389

AstrofísicaPhysicsNuclear and High Energy PhysicsParticle physicsGrand-Unified-TheoryDark-MatterHigh Energy Physics::PhenomenologyElectroweak interactionDark matterBaryogenesisFísicaAstrophysics::Cosmology and Extragalactic AstrophysicsTime Entropy ProductionBaryogenesisBaryon asymmetryDecaying ParticlesConstraintsHigh Energy Physics::ExperimentGravitinoNeutrinoNeutrino MassNeutrino oscillationPhenomenology (particle physics)Inflationary UniversePhysical Review D
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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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Direct neutralino searches in the NMSSM with gravitino LSP in the degenerate scenario

2011

In the present work a two-component dark matter model is studied adopting the degenerate scenario in the R-parity conserving NMSSM. The gravitino LSP and the neutralino NLSP are extremely degenerate in mass, avoiding the BBN bounds and obtaining a high reheating temperature for thermal leptogenesis. In this model both gravitino (absolutely stable) and neutralino (quasi-stable) contribute to dark matter, and direct detection searches for neutralino are discussed. Points that survive all the constraints correspond to a singlino-like neutralino.

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Degenerate energy levelsDark matterFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)LeptogenesisNeutralinoGravitinoAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of High Energy Physics
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Neutrinos, DUNE and the world best bound on CPT invariance

2017

CPT symmetry, the combination of Charge Conjugation, Parity and Time reversal, is a cornerstone of our model building strategy and therefore the repercussions of its potential violation will severely threaten the most extended tool we currently use to describe physics, i.e. local relativistic quantum fields. However, limits on its conservation from the Kaon system look indeed imposing. In this work we will show that neutrino oscillation experiments can improve this limit by several orders of magnitude and therefore are an ideal tool to explore the foundations of our approach to Nature. Strictly speaking testing CPT violation would require an explicit model for how CPT is broken and its effe…

Nuclear and High Energy PhysicsParticle physicsCPT symmetryFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationQuantumPhysics010308 nuclear & particles physicsOscillationHigh Energy Physics::PhenomenologyParity (physics)Observablelcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoModel buildinglcsh:Physics
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IS ALR SUGGESTING A LEFT–RIGHT SYMMETRIC SOLUTION?

1996

The implications of the recent measurement of the left–right asymmetry ALR by the SLD collaboration for the left–right symmetric theory are examined. We show that it is possible to arrange for a large, negative value of S, without serious side effects for other observables within this model. We also consider a restricted model with specified Higgs structure, where limits on MZ2 can be obtained.

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectStructure (category theory)General Physics and AstronomyAstronomy and AstrophysicsObservableAsymmetryNuclear physicsHiggs bosonSymmetric solutionValue (mathematics)media_commonModern Physics Letters A
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Lepton number asymmetries and the lower bound on the reheating temperature

2017

We show that the reheating temperature of a matter-domination era in the early universe can be pushed down to the neutrino decoupling temperature at around $2 \ {\rm MeV}$ if the reheating takes place through non-hadronic decays of the dominant matter and neutrino-antineutrino asymmetries are still large enough, $|L| \gtrsim \mathcal{O}(10^{-2})$ (depending on the neutrino flavor) at the end of reheating.

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsmedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and AstrophysicsNeutrino decouplingAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesLepton numberUpper and lower boundsUniverseGeneral Relativity and Quantum Cosmology0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010303 astronomy & astrophysicsmedia_commonAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of Cosmology and Astroparticle Physics
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A full picture of large lepton number asymmetries of the Universe

2017

A large lepton number asymmetry of (0.1−1) at present Universe might not only be allowed but also necessary for consistency among cosmological data. We show that, if a sizeable lepton number asymmetry were produced before the electroweak phase transition, the requirement for not producing too much baryon number asymmetry through sphalerons processes, forces the high scale lepton number asymmetry to be larger than about 03. Therefore a mild entropy release causing (10-100) suppression of pre-existing particle density should take place, when the background temperature of the Universe is around T = (10−2-102) GeV for a large but experimentally consistent asymmetry to be present today. We also …

PhysicsParticle physics010308 nuclear & particles physicsEntropy productionmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyElectroweak interactionAstronomy and Astrophysics01 natural sciencesLepton numberAsymmetryUniverse0103 physical sciencesHigh Energy Physics::ExperimentBaryon number010303 astronomy & astrophysicsEntropy (arrow of time)Vacuum expectation valuemedia_commonJournal of Cosmology and Astroparticle Physics
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Symmetry meets AI

2021

We explore whether Neural Networks (NNs) can {\it discover} the presence of symmetries as they learn to perform a task. For this, we train hundreds of NNs on a {\it decoy task} based on well-controlled Physics templates, where no information on symmetry is provided. We use the output from the last hidden layer of all these NNs, projected to fewer dimensions, as the input for a symmetry classification task, and show that information on symmetry had indeed been identified by the original NN without guidance. As an interdisciplinary application of this procedure, we identify the presence and level of symmetry in artistic paintings from different styles such as those of Picasso, Pollock and Van…

FOS: Computer and information sciencesComputer Science - Machine Learning0303 health sciencesTheoretical computer scienceArtificial neural networkComputer Vision and Pattern Recognition (cs.CV)PhysicsQC1-999Computer Science - Computer Vision and Pattern RecognitionFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesMachine Learning (cs.LG)Task (project management)High Energy Physics - Phenomenology03 medical and health sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spacePICASSOHidden layerSymmetry (geometry)010306 general physics030304 developmental biologySciPost Physics
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Cosmology and CPT violating neutrinos

2017

The combination Charge Conjugation-Parity-Time Reversal(CPT) is a fundamental symmetry in our current understanding of nature. As such, testing CPT violation is a strongly motivated path to explore new physics. In this paper we study CPT violation in the neutrino sector, giving for the first time a bound, for a fundamental particle, in the CPT violating particle-antiparticle gravitational mass difference. We argue that cosmology is nowadays the only data sensitive to CPT violation for the neutrino-antineutrino mass splitting and we use the latest data release from Planck combined with the current Baryonic-Acoustic-Oscillation measurement to perform a full cosmological analysis. To show the …

Particle physicsPhysics::General PhysicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelFOS: Physical sciencesElementary particlelcsh:Astrophysics7. Clean energy01 natural sciencesCosmologyGravitationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. RadioactivityPlanck010306 general physics010303 astronomy & astrophysicsEngineering (miscellaneous)PhysicsHigh Energy Physics::PhenomenologyCharge (physics)Symmetry (physics)High Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentNeutrino
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On large lepton number asymmetries of the Universe

2017

A large lepton number asymmetry of $\mathcal{O}(0.1-1)$ at present universe might not only be allowed but also necessary for consistency among cosmological data. We show that, if a sizeable lepton number asymmetry were produced before the electroweak phase transition, the requirement for not producing too much baryon number asymmetry through sphalerons processes, forces the high scale lepton number asymmetry to be larger than about $30$. Therefore a mild entropy release causing $\mathcal{O}(10-100)$ suppression of pre-existing particle density should take place, when the background temperature of the universe is around $T = \mathcal{O}(10^{-2} - 10^2) {\rm GeV}$ for a large but experimental…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::Experiment
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CPasymmetries inBsdecays and spontaneousCPviolation

1999

We study the possible effects of new physics in $\mathrm{CP}$ asymmetries in two-body ${B}_{s}$ decays in left-right models with spontaneous $\mathrm{CP}$ violation. Considering the contributions of new $\mathrm{CP}$ phases to the ${B}_{s}$ mixing as well as to the penguin-dominated decay amplitudes we show that, with the present constraints, large deviations from the standard model predictions in $\mathrm{CP}$ asymmetries are allowed in both cases. The detection of new physics can be achieved by measuring nonzero asymmetries which are predicted to vanish in the standard model or by comparing two measurements which are predicted to be equal in the standard model. In particular, we show that…

PhysicsNuclear and High Energy PhysicsParticle physicsAmplitudePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionCP violationHigh Energy Physics::ExperimentLarge deviations theoryMixing (physics)Standard ModelPhysical Review D
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Transplanckian masses in inflation

2016

AbstractWe explore the possibility that the transplanckian field values needed to accommodate the experimental results in minimally coupled single-field inflation models are only due to our insistence of imposing a minimal coupling of the inflaton field to gravity. A simple conformal transformation can bring the field values below the Planck mass without changing the physics at the expense of having a richer gravitational sector. Transplanckian field values may be the signal that we are (miss)interpreting phenomena due to gravity as being originated exclusively in the scalar sector.

PhysicsMinimal couplingInflation (cosmology)Nuclear and High Energy PhysicsGravity (chemistry)Field (physics)010308 nuclear & particles physicsScalar (mathematics)Planck massInflaton01 natural sciencesGravitationTheoretical physicsGeneral Relativity and Quantum CosmologyClassical mechanics0103 physical sciences010306 general physicsNuclear and Particle Physics Proceedings
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Constraints on inflation with an extended neutrino sector

2019

Constraints on inflationary models typically assume only the standard models of cosmology and particle physics. By extending the neutrino sector to include a new interaction with a light scalar mediator (mφ∼MeV), it is possible to relax these constraints, in particular via opening up regions of the parameter space of the spectral index ns. These new interactions can be probed at IceCube via interactions of astrophysical neutrinos with the cosmic neutrino background for nearly all of the relevant parameter space.

PhysicsParticle physicsSpectral index010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaScalar (mathematics)Parameter space01 natural sciencesCosmologyCosmic neutrino background0103 physical sciencesNeutrino010306 general physics
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Neutrino mixing and masses from long baseline and atmospheric oscillation experiments

1998

We argue that regardless of the outcome of future Long Baseline experiments, additional information will be needed to unambiguously decide among the different scenarios of neutrino mixing. We use, for this purpose, a simple test of underground data: an asymmetry between downward and upward going events. Such an asymmetry, in which matter effects can be crucial, tests electron and muon neutrino data separately and can be compared with the theoretical prediction without relying on any simulation program.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsOscillationmedia_common.quotation_subjectFísicaFOS: Physical sciencesElectronAsymmetryOutcome (probability)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentMuon neutrinoNeutrinoBaseline (configuration management)Mixing (physics)media_commonPhysics Letters B
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Footprints of a left-right symmetric model in a muon collider

2000

Abstract The double charged Higgs bosons, Δ ±± , are one of the benchmarks of left-right symmetric models. We discuss their production and demonstrate that even for small values of the Δ ++ l − l − coupling, they would produce observable signals at muon colliders.

PhysicsCouplingNuclear and High Energy PhysicsParticle physicsMuonPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologySymmetric modelObservableNuclear physicsMuon colliderHiggs bosonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentBosonPhysics Letters B
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Eviction of a 125 GeV “heavy”-Higgs from the MSSM

2013

We prove that the present experimental constraints are already enough to rule out the possibility of the similar to 125 GeV Higgs found at LHC being the second lightest Higgs in a general MSSM context, even with explicit CP violation in the Higgs potential. Contrary to previous studies, we are able to eliminate this possibility analytically, using simple expressions for a relatively small number of observables. We show that the present LHC constraints on the diphoton signal strength, tau tau production through Higgs and BR(B -> X-s gamma) are enough to preclude the possibility of H-2 being the observed Higgs with m(H) similar or equal to 125 GeV within an MSSM context, without leaving room …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHiggs PhysicsSupersymmetric Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableContext (language use)Resonance (particle physics)Partícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Signal strengthBeyond Standard ModelHiggs bosonCP violationHigh Energy Physics::Experiment
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Prospects for constraining the shape of non-Gaussianity with the scale-dependent bias

2012

We consider whether the non-Gaussian scale-dependent halo bias can be used not only to constrain the local form of non-Gaussianity but also to distinguish among different shapes. In particular, we ask whether it can constrain the behavior of the primordial three-point function in the squeezed limit where one of the momenta is much smaller than the other two. This is potentially interesting since the observation of a three-point function with a squeezed limit that does not go like the local nor equilateral templates would be a signal of non-trivial dynamics during inflation. To this end we use the quasi-single field inflation model of Chen and Wang as a representative two-parameter model, wh…

Inflation (cosmology)PhysicsAstrofísicaCosmology and Nongalactic Astrophysics (astro-ph.CO)Cosmologia010308 nuclear & particles physicsFísicaFOS: Physical sciencesAstronomy and AstrophysicsFunction (mathematics)Astrophysics::Cosmology and Extragalactic AstrophysicsAstrophysics01 natural sciencesCosmologyNon-Gaussianity0103 physical sciencesHalo effectDark energyRange (statistics)Limit (mathematics)Statistical physics010303 astronomy & astrophysicsBispectrumAstrophysics - Cosmology and Nongalactic Astrophysics
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Slinky inflation

2005

We present a new approach to quintessential inflation, in which both dark energy and inflation are explained by the evolution of a single scalar field. We start from a simple scalar potential with both oscillatory and exponential behavior. We employ the conventional reheating mechanism of new inflation, in which the scalar decays to light fermions with a decay width that is proportional to the scalar mass. Because our scalar mass is proportional to the Hubble rate, this gives adequate reheating at early times while shutting off at late times to preserve quintessence and satisfy nucleosynthesis constraints. We discuss a simple model which solves the horizon, flatness, and "why now" problems.…

Inflation (cosmology)PhysicsNuclear and High Energy PhysicsCosmic microwave backgroundScalar (mathematics)Astrophysics (astro-ph)FOS: Physical sciencesFísicaScalar potentialAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsTheoretical physicsHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)NucleosynthesisDark energyScalar fieldQuintessence
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Neutrino oscillation probabilities through the looking glass

2019

In this paper we review different expansions for neutrino oscillation probabilities in matter in the context of long-baseline neutrino experiments. We examine the accuracy and computational efficiency of different exact and approximate expressions. We find that many of the expressions used in the literature are not precise enough for the next generation of long-baseline experiments, but several of them are while maintaining comparable simplicity. The results of this paper can be used as guidance to both phenomenologists and experimentalists when implementing the various oscillation expressions into their analysis tools.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsOscillationmedia_common.quotation_subjectFOS: Physical sciencesContext (language use)01 natural scienceslcsh:QC1-999Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesSimplicityAnalysis toolsNeutrino010306 general physicsNeutrino oscillationlcsh:Physicsmedia_common
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Eternal hilltop inflation

2016

We consider eternal inflation in hilltop-type inflation models, favored by current data, in which the scalar field in inflation rolls off of a local maximum of the potential. Unlike chaotic or plateau-type inflation models, in hilltop inflation the region of field space which supports eternal inflation is finite, and the expansion rate $H_{EI}$ during eternal inflation is almost exactly the same as the expansion rate $H_*$ during slow roll inflation. Therefore, in any given Hubble volume, there is a finite and calculable expectation value for the lifetime of the "eternal" inflation phase, during which quantum flucutations dominate over classical field evolution. We show that despite this, i…

PhysicsInflationCosmology and Nongalactic Astrophysics (astro-ph.CO)Slow rollSpacetime010308 nuclear & particles physicsmedia_common.quotation_subjectSpace timeKeynesian economicsFOS: Physical sciencesAstronomy and AstrophysicsExpectation valueAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesGeneral Relativity and Quantum CosmologyHubble volume0103 physical sciences010306 general physicsEternal inflationScalar fieldmedia_commonAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of Cosmology and Astroparticle Physics
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Left-handed neutrino disappearance probe of neutrino mass and character

1996

We explore the sensitivity to a non vanishing neutrino mass offered by dynamical observables, i.e., branching ratios and polarizations. The longitudinal polarization in the C.M. frame decreases by a 4% for $D^+ \rightarrow \tau^+ \nu_\tau$ and $m_{\nu_\tau}=24$ MeV. Taking advantage of the fact that the polarization is a Lorentz variant quantity, we study the polarization effects in a boosted frame. By means of a neutrino beam, produced by a high velocity boosted parent able to flip the neutrino helicity, we find that an enhanced left-handed neutrino deficit, induced by a Wigner rotation, appears.

Left handedPhysicsParticle physicsLorentz transformationHigh Energy Physics::PhenomenologyWigner rotationFOS: Physical sciencesFísicaGeneral Physics and AstronomyObservableNeutrino beamPolarization (waves)HelicityNuclear physicssymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentNeutrino
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Constraints on doubly charged Higgs interactions at linear collider

1996

Production of a single doubly charged Higgs boson $Delta^{--}$ in polarized $e^+e^-$ and $e^+\gamma$ collision modes of the linear collider have been investigated. The mass range of $Delta^{--}$ to be probed extends up to the collision energy. The diagonal lepton number violating Yukawa coupling $h_{ee}$ will be tested at least three orders of magnitude more strictly than in present experiments.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaCoupling (probability)01 natural sciencesLepton number3. Good healthlaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)law0103 physical sciencesHiggs bosonProduction (computer science)High Energy Physics::Experiment010306 general physicsColliderEnergy (signal processing)
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Inflation meets neutrinos

2019

Constraints on inflationary models typically assume only the standard models of cosmology and particle physics. By extending the neutrino sector to include a new interaction with a light scalar mediator ($m_{\phi}\sim$MeV), it is possible to relax these constraints, in particular via opening up regions of the parameter space of the spectral index $n_s$. These new interactions can be probed at IceCube via interactions of astrophysical neutrinos with the Cosmic Neutrino Background for nearly all of the relevant parameter space.

High Energy Astrophysical Phenomena (astro-ph.HE)High Energy Physics - PhenomenologyCosmology and Nongalactic Astrophysics (astro-ph.CO)High Energy Physics - Phenomenology (hep-ph)Physics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysics - High Energy Astrophysical PhenomenaAstrophysics - Cosmology and Nongalactic Astrophysics
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CPAsymmetries inB0Decays in the Left-Right Model

1998

We study time dependent CP asymmetries in B^0_{d,s} decays in the left-right model with spontaneous breakdown of CP. Due to the new contributions to B^0-\bar B^0 mixing the CP asymmetries can be substantially modified. Moreover, there can be significant new contributions to the $B$-meson decay amplitudes from the magnetic penguins. Most promising for detection of the new physics in the planned $B$ factories is that the CP asymmetries in the decays B--> J/\psi K_S and B--> \phi K_S which are supposed to be equal in the standard model can differ significantly in this class of models independently of the results in the measurements of B--> X_s \gamma.

PhysicsParticle physicsAmplitudePhysics beyond the Standard ModelSpontaneous symmetry breakingGeneral Physics and AstronomyCP violationHigh Energy Physics::ExperimentAtomic physicsMixing (physics)Standard ModelB-factoryBar (unit)Physical Review Letters
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How to relax the cosmological neutrino mass bound

2019

We study the impact of non-standard momentum distributions of cosmic neutrinos on the anisotropy spectrum of the cosmic microwave background and the matter power spectrum of the large scale structure. We show that the neutrino distribution has almost no unique observable imprint, as it is almost entirely degenerate with the effective number of neutrino flavours, $N_{\mathrm{eff}}$, and the neutrino mass, $m_{\nu}$. Performing a Markov chain Monte Carlo analysis with current cosmological data, we demonstrate that the neutrino mass bound heavily depends on the assumed momentum distribution of relic neutrinos. The message of this work is simple and has to our knowledge not been pointed out cle…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)cosmological neutrinosPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaCosmic microwave backgroundFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysicscosmological parameters from LSS01 natural sciencesCosmologyMomentumsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)cosmological0103 physical sciencesPhysicsCOSMIC cancer database010308 nuclear & particles physicsMatter power spectrumHigh Energy Physics::Phenomenologycosmological parameters from CMBRAstronomy and AstrophysicsObservableMarkov chain Monte Carloneutrino masses from cosmologyHigh Energy Physics - Phenomenologyparameters from CMBRsymbolsHigh Energy Physics::ExperimentNeutrinoAstrophysics - Cosmology and Nongalactic Astrophysics
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Sterile Neutrinos, Black Hole Vacuum and Holographic Principle

2021

We construct an effective field theory (EFT) model that describes matter field interactions with Schwarzschild mini-black-holes (SBH's), treated as a scalar field, $B_0(x)$. Fermion interactions with SBH's require a random complex spurion field, $\theta_{ij}$, which we interpret as the EFT description of "holographic information," which is correlated with the SBH as a composite system. We consider Hawking's virtual black hole vacuum (VBH) as a Higgs phase, $\langle B_0 \rangle =V$. Integrating sterile neutrino loops, the field $\theta_{ij}$ is promoted to a dynamical field, necessarily developing a tachyonic instability and acquiring a VEV of order the Planck scale. For $N$ sterile neutrino…

High Energy Physics - TheorySterile neutrinoParticle physicsPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:AstrophysicsGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466Effective field theorylcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsVirtual black holeEngineering (miscellaneous)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)Higgs phaseBlack holeHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)lcsh:QC770-798Scalar fieldSchwarzschild radius
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Invisible neutrino decay in precision cosmology

2021

We revisit the topic of invisible neutrino decay in the precision cosmological context, via a first-principles approach to understanding the cosmic microwave background and large-scale structure phenomenology of such a non-standard physics scenario. Assuming an effective Lagrangian in which a heavier standard-model neutrino $\nu_H$ couples to a lighter one $\nu_l$ and a massless scalar particle $\phi$ via a Yukawa interaction, we derive from first principles the complete set of Boltzmann equations, at both the spatially homogeneous and the first-order inhomogeneous levels, for the phase space densities of $\nu_H$, $\nu_l$, and $\phi$ in the presence of the relevant decay and inverse decay p…

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsCosmic microwave backgroundFOS: Physical sciencesAstronomy and AstrophysicsScalar bosonYukawa interaction01 natural sciencesCosmologyMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Phase space0103 physical sciencesHigh Energy Physics::ExperimentNeutrinoPhenomenology (particle physics)Astrophysics - Cosmology and Nongalactic AstrophysicsJournal of Cosmology and Astroparticle Physics
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MINOS and CPT violating neutrinos

2009

We review the status of CPT violation in the neutrino sector. Apart from LSND, current data favors three flavors of light stable neutrinos and antineutrinos, with both halves of the spectrum having one smaller mass splitting and one larger mass splitting. Oscillation data for the smaller splitting are consistent with CPT. For the larger splitting, current data favor an antineutrino mass-squared splitting that is an order of magnitude larger than the corresponding neutrino splitting, with the corresponding mixing angle less than maximal. This CPT-violating spectrum is driven by recent results from MINOS, but is consistent with other experiments if we ignore LSND. We describe an analysis tech…

AstrofísicaQuarkPhysicsNuclear and High Energy PhysicsParticle physicsMuonCPT symmetryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesWeinberg angleNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)MINOSHigh Energy Physics::ExperimentNeutrinoNeutrinosCPT violationNeutrino oscillationLepton
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CPT and CP, an entangled couple

2020

Even though it is undoubtedly very appealing to interpret the latest T2K results as evidence of CP violation, this claim assumes CPT conservation in the neutrino sector to an extent that has not been tested yet. As we will show, T2K results are not robust against a CPT-violating explanation. On the contrary, a CPT-violating CP-conserving scenario is in perfect agreement with current neutrino oscillation data. Therefore, to elucidate whether T2K results imply CP or CPT violation is of utter importance. We show that, even after combining with data from NO$\nu$A and from reactor experiments, no claims about CP violation can be made. Finally, we update the bounds on CPT violation in the neutrin…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationBeyond Standard Model0103 physical scienceslcsh:QC770-798CP violationNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino010306 general physicsNeutrino oscillationJournal of High Energy Physics
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Spontaneous CP violation and the B0 system

1998

We investigate effects of spontaneous breakdown of CP in $B^0_{d,s}-\overline{B^0}_{d,s}$ systems in left-right symmetric models. Assuming that the left-right contribution to the $B^0-\overline{B^0}$ matrix element $M_{12}$ can be at most equal to the standard model one we obtain a new lower bound, $M_H\gsim 12$ TeV, on the flavour changing Higgs boson mass. Most importantly, the convention independent parameter $Re(\overline{\epsilon}_B),$ which measures the amount of $\Delta B=2$ CP violation, can be enhanced by a factor of four or more for $B^0_d$ and almost by two orders of magnitude for $B^0_s$ systems when compared with the Standard Model predictions. Therefore, interesting possibilit…

PhysicsNuclear and High Energy PhysicsParticle physicsIndependent parameterHiggs bosonFísicaCP violationMatrix elementUpper and lower boundsOrder of magnitudeStandard ModelNuclear Physics B
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Spiral Inflation

2015

We propose a novel scenario of primordial inflation in which the inflaton goes through a spiral motion starting from around the top of a symmetry breaking potential. We show that, even though inflation takes place for a field value much smaller than Planck scale, it is possible to obtain relatively large tensor to scalar ratio ($r \sim 0.1$) without fine tuning. The inflationary observables perfectly match Planck data.

PhysicsInflation (cosmology)Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Field (physics)Scalar (mathematics)FOS: Physical sciencesFísicaObservableAstrophysics::Cosmology and Extragalactic AstrophysicsInflatonlcsh:QC1-999High Energy Physics - PhenomenologyTheoretical physicssymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)symbolsTensorSymmetry breakingPlancklcsh:PhysicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Neutrino Coannihilation on Dark-Matter Relics?

2006

High-energy neutrinos may resonate with relic background neutralinos to form short-lived sneutrinos. In some circumstances, the decay chain that leads back to the lightest supersymmetric particle would yield few-GeV gamma rays or charged-particle signals. Although resonant coannihilation would occur at an appreciable rate in our galaxy, the signal in any foreseeable detector is unobservably small.

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)Dark matterHigh Energy Physics::PhenomenologyGamma rayFOS: Physical sciencesAstrophysicsAstrophysicsLightest Supersymmetric ParticleGalaxyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentDecay chainNeutrinoResonance effect
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Decoherent neutrino mixing, dark energy, and matter-antimatter asymmetry

2004

A CPT violating decoherence scenario can easily account for all the experimental evidence in the neutrino sector including LSND. In this work it is argued that this framework can also accommodate the Dark Energy content of the Universe, as well as the observed matter-antimatter asymmetry.

High Energy Physics - TheoryPhysics::General PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsCPT symmetrymedia_common.quotation_subjectFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyCosmologyNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Neutrino oscillationComputer Science::Databasesmedia_commonPhysicsHigh Energy Physics::PhenomenologyFísicaUniverseHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Neutrino detectorAntimatterDark energyHigh Energy Physics::ExperimentNeutrinoPhysical Review D
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Minimal noncanonical cosmologies

2006

We demonstrate how much it is possible to deviate from the standard cosmological paradigm of inflation-assisted LambdaCDM, keeping within current observational constraints, and without adding to or modifying any theoretical assumptions. We show that within a minimal framework there are many new possibilities, some of them wildly different from the standard picture. We present three illustrative examples of new models, described phenomenologically by a noncanonical scalar field coupled to radiation and matter. These models have interesting implications for inflation, quintessence, reheating, electroweak baryogenesis, and the relic densities of WIMPs and other exotics.

Inflation (cosmology)PhysicsNuclear and High Energy PhysicsElectroweak interactionAstrophysics (astro-ph)FOS: Physical sciencesFísicaAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsBaryogenesisTheoretical physicsGeneral Relativity and Quantum CosmologyScalar fieldQuintessence
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Electroweak precision data and right-handed gauge bosons

1998

The implication of recent electroweak precision data for left-right symmetric models is examined. We establish a lower bound on the charged and neutral right-handed gauge bosons independent of the right-handed neutrino mass and of any restrictions or implied symmetries on the right KM matrix.

PhysicsGauge bosonParticle physicsPhysics and Astronomy (miscellaneous)Right handedCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyElectroweak interactionTechnicolorUpper and lower boundsQuantum electrodynamicsHomogeneous spaceNeutrinoEngineering (miscellaneous)The European Physical Journal C
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The dark(er) side of inflation

2006

We present a new approach to quintessential inflation, in which both dark energy and inflation are explained by the evolution of a single scalar field. We start from a simple scalar potential with both oscillatory and exponential behavior.We employ the conventional reheating mechanism of new inflation, in which the scalar decays to light fermions with a decay width that is proportional to the scalar mass. Because our scalar mass is proportional to the Hubble rate, this gives adequate reheating at early times while shutting off at late times to preserve quintessence and satisfy nucleosynthesis constraints.

High Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics
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Gravitational waves from first order phase transitions as a probe of an early matter domination era and its inverse problem

2016

We investigate the gravitational wave background from a first order phase transition in a matter-dominated universe, and show that it has a unique feature from which important information about the properties of the phase transition and thermal history of the universe can be easily extracted. Also, we discuss the inverse problem of such a gravitational wave background in view of the degeneracy among macroscopic parameters governing the signal.

PhysicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Gravitational-wave observatory010308 nuclear & particles physicsGravitational waveSpeed of gravityFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Gravitational acceleration01 natural scienceslcsh:QC1-999General Relativity and Quantum CosmologyGravitational energyGravitational wave backgroundHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Classical mechanicsGravitational field0103 physical sciences010306 general physicslcsh:PhysicsAstrophysics - Cosmology and Nongalactic AstrophysicsGravitational redshiftPhysics Letters
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On the tensor-to-scalar ratio in large single-field inflation models

2015

We show that generically the tensor-to-scalar ratio in large single-field inflation scenarios is bounded to be larger than $\mathcal{O}(10^{-3})$ for the spectral index in the range favored by observations.

General Relativity and Quantum CosmologyHigh Energy Physics - PhenomenologyCosmology and Nongalactic Astrophysics (astro-ph.CO)High Energy Physics - Phenomenology (hep-ph)FOS: Physical sciencesAstrophysics - Cosmology and Nongalactic Astrophysics
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Observational Constraints on Undulant Cosmologies

2005

In an undulant universe, cosmic expansion is characterized by alternating periods of acceleration and deceleration. We examine cosmologies in which the dark-energy equation of state varies periodically with the number of e-foldings of the scale factor of the universe, and use observations to constrain the frequency of oscillation. We find a tension between a forceful response to the cosmic coincidence problem and the standard treatment of structure formation.

PhysicsCOSMIC cancer databaseStructure formationOscillationEquation of state (cosmology)media_common.quotation_subjectAstrophysics (astro-ph)FOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsUniverseMetric expansion of spaceAccelerationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Scale factor (cosmology)media_common
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Baryogenesis from a right-handed neutrino condensate

2010

We show that the baryon asymmetry of the Universe can be generated by a strongly coupled right handed neutrino condensate which also drives inflation. The resulting model has only a small number of parameters, which completely determine not only the baryon asymmetry of the Universe and the mass of the right handed neutrino but also the inflationary phase. This feature allows us to make predictions that will be tested by current and planned experiments. As compared to the usual approach our dynamical framework is both economical and predictive.

PhysicsInflation (cosmology)Strongly coupledNuclear and High Energy PhysicsParticle physicsRight handedHigh Energy Physics::PhenomenologyPhase (waves)FOS: Physical sciencesFísicaAstrophysics::Cosmology and Extragalactic AstrophysicsBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryHigh Energy Physics::ExperimentNeutrinoJournal of High Energy Physics
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Tau neutrinos from muon storage rings

2000

Charged tau leptons emerging in a long baseline experiment with a muon storage ring and a far-away detector will positively establish neutrino oscillations. We study the conversion of $\nu_\mu$ ($\bar{\nu}_\mu$) and of $\bar{\nu}_e$ ($\nu_e$) to $\nu_\tau$ or $\bar{\nu}_\tau$ for neutrinos from a 20 GeV muon storage ring, within the strong mixing scheme and on the basis of the squared mass differences which are compatible with all reported neutrino anomalies, including the LSND data. In contrast to other solutions which ignore the Los Alamos anomaly, we find charged tau production rates which should be measurable in a realistic set up. As a consequence, determining the complete mass spectru…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Mass spectrumProduction (computer science)High Energy Physics::ExperimentNeutrinoAnomaly (physics)Neutrino oscillationStorage ringLepton
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Electroweak baryogenesis window in non standard cosmologies

2012

In this work we show that the new bounds on the Higgs mass are more than difficult to reconcile with the strong constraints on the physical parameters of the Standard Model and the Minimal Supersymmetric Standard Model imposed by the preservation of the baryon asymmetry. This bound can be weakened by assuming a nonstandard cosmology at the time of the electroweak phase transition, reverting back to standard cosmology by BBN time. Two explicit examples are an early period of matter dominated expansion due to a heavy right handed neutrino (see-saw scale), or a nonstandard braneworld expansion.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesCosmologyStandard ModelBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryHiggs bosonNeutrinoMinimal Supersymmetric Standard ModelJournal of High Energy Physics
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Spontaneous CP violation in the left-right model and the kaon system

1996

A left-right model with spontaneous $CP$ breakdown, consistent with the particle physics phenomenology, is presented. Constraints on free parameters of the model: mass of the new right handed gauge boson $M_2$ and ratio $r$ of the two vacuum expectation values of the bidoublet, are found from the measurement of $\epsilon$ in the kaon system. For most of the parameter space, $M_2$ is restricted to be below 10 TeV. Higher masses can be achieved only by fine tuning of Kobayashi-Maskawa matrix elements, quark masses, $r$ and the phase $\alpha$ which is the unique source of $CP$-violation in the model. Large number of combinations of signs of quark masses, which are observables of the model, are…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsFine-tuningGauge bosonHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableParameter spaceHigh Energy Physics - PhenomenologyMatrix (mathematics)High Energy Physics - Phenomenology (hep-ph)CP violationFree parameterNuclear Physics B
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The dark side of curvature

2009

Geometrical tests such as the combination of the Hubble parameter H(z) and the angular diameter distance d(A)(z) can, in principle, break the degeneracy between the dark energy equation of state parameter w(z), and the spatial curvature Omega(k) in a direct, model-independent way. In practice, constraints on these quantities achievable from realistic experiments, such as those to be provided by Baryon Acoustic Oscillation (BAO) galaxy surveys in combination with CMB data, can resolve the cosmic confusion between the dark energy equation of state parameter and curvature only statistically and within a parameterized model for w(z). Combining measurements of both H(z) and d(A)(z) up to suffici…

Equation of stateCosmology and Nongalactic Astrophysics (astro-ph.CO)Cosmic microwave backgroundFOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsCurvature01 natural sciencessymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesDark energy experiments010303 astronomy & astrophysicsPhysics010308 nuclear & particles physicsAngular diameter distanceAstronomy and AstrophysicsRedshiftCosmological parameters from CMBRHigh Energy Physics - PhenomenologysymbolsDark energyBaryon acoustic-oscillationsBaryon acoustic oscillationsHubble's lawAstrophysics - Cosmology and Nongalactic Astrophysics
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Composite states of two right-handed neutrinos

2016

In this work, we develop a model for Higgs-like composites based on two generations of right-handed neutrinos that condense. We analyze the spontaneous symmetry breaking of the theory with two explicit breakings, setting the different scales of the model and obtaining massive bosons as a result. Finally, we calculate the gravitational wave imprint left by the phase transition associated with the symmetry breaking of a generic potential dictated by the symmetries of the composites.

PhysicsPhase transitionParticle physics010308 nuclear & particles physicsSpontaneous symmetry breaking01 natural sciencesSupersymmetry breakingChirality (physics)Explicit symmetry breakingHiggs field0103 physical sciencesSymmetry breaking010306 general physicsChiral symmetry breakingPhysical Review D
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Resurrection of large lepton number asymmetries from neutrino flavor oscillations

2016

We numerically solve the evolution equations of neutrino three-flavor density matrices, and show that, even if neutrino oscillations mix neutrino flavors, large lepton number asymmetries are still allowed in certain limits by Big Bang Nucleosynthesis (BBN).

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLepton numberNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesis0103 physical sciencesMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationFlavorAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Neutrinos: Fast & Curious

2016

The Standard Model has been effective way beyond expectations in foreseeing the result of almost all the experimental tests done up so far. In it, neutrinos are massless. Nonetheless, in recent years we have collected solid proofs indicating little but non zero masses for the neutrinos (when contrasted with those of the charged leptons). These masses permit neutrinos to change their flavor and oscillate, indeed a unique treat. In these lectures, I discuss the properties and the amazing potential of neutrinos in and beyond the Standard Model.

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::ExperimentParticle Physics - Phenomenology
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METing SUSY on the Z peak

2016

Recently the ATLAS experiment announced a 3 $\sigma$ excess at the Z-peak consisting of 29 pairs of leptons together with two or more jets, $E_T^{\rm miss}> 225$ GeV and $H_T \geq 600$ GeV, to be compared with $10.6 \pm 3.2$ expected lepton pairs in the Standard Model. No excess outside the Z-peak was observed. By trying to explain this signal with SUSY we find that only relatively light gluinos, $m_{\tilde g} \lesssim 1.2$ TeV, together with a heavy neutralino NLSP of $m_{\tilde \chi} \gtrsim 400$ GeV decaying predominantly to Z-boson plus a light gravitino, such that nearly every gluino produces at least one Z-boson in its decay chain, could reproduce the excess. We construct an explicit …

PhysicsParticle physicsGluinoLarge Hadron ColliderPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetry01 natural sciencesStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutralinoGravitinoProduction (computer science)High Energy Physics::Experiment010306 general physicsEngineering (miscellaneous)Lepton
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Constraints on theWRmass andCPviolation in left-right models

1997

We update the constraints on the right-handed W{sub R} gauge boson mass, mixing angle {zeta} with the left-handed W{sub L} gauge boson, and other parameters in general left-right symmetric models with different mechanisms of CP violation. Constraints mostly independent of any assumption on the quark sector are obtained from a reanalysis of muon decay data. The best {chi}{sup 2} fit of the data gives g{sub R}/g{sub L}=0.94{plus_minus}0.09 for the ratio of right to left gauge couplings, with M{sub W{sub R}}{ge}485 GeV and {vert_bar}{zeta}{vert_bar}{le}0.0327. Fixing g{sub L}=g{sub R} (in particular for manifestly left-right symmetric models), we obtain M{sub W{sub R}}{approx_gt}549 GeV and {v…

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsMuonMesonHadronCP violationElementary particleStandard ModelBosonPhysical Review D
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CP violating lepton asymmetries in left-right models

1998

Lepton charge asymmetries can be used as an alternative means of searching for new physics. They are interesting because they are small in the Standard Model and therefore, necessarily evidence new physics. In this work we explore the use of lepton asymmetries as a probe of the flavour structure of the left-right symmetric model with spontaneous CP violation. We find that new physics may enhance the magnitude of $a_{SL}$ up to the precent level within the appropiate parameter space.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFlavourStructure (category theory)FOS: Physical sciencesFísicaCharge (physics)Parameter spaceHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::ExperimentLeptonPhysics Letters B
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Only three flavours

1998

Abstract It is shown that it is possible to account for all the experimental indications for neutrino oscillations with just three flavours. In particular we suggest that the atmospheric neutrino anomaly and the LSND result can be explained by the same mass difference and mixing. Possible implications and future test of the resulting mass and mixing pattern are given.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics::ExperimentAtmospheric neutrinoAnomaly (physics)Neutrino oscillationMixing (physics)
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New- vs. chaotic- inflations

2015

We show that "spiralized" models of new-inflation can be experimentally identified mostly by their positive spectral running in direct contrast with most chaotic-inflation models which have negative runnings typically in the range of $\mathcal{O}(10^{-4}-10^{-3})$.

PhysicsHigh Energy Physics - PhenomenologyMathematical model010308 nuclear & particles physics0103 physical sciencesChaoticContrast (statistics)Astronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsStatistical physics010306 general physics01 natural sciencesAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of Cosmology and Astroparticle Physics
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Quintessence, inflation and baryogenesis from a single pseudo-Nambu-Goldstone boson

2007

15 pages, 3 figures.-- ISI Article Identifier: 000250759700079.-- ArXiv pre-print available at: http://arxiv.org/abs/0707.3999

Nuclear and High Energy PhysicsParticle physicsProton decayCosmic microwave backgroundGenerationFOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicssymbols.namesakePlanckBosonPhysicsHigh Energy Physics::PhenomenologyAstrophysics (astro-ph)BaryogenesisFísicaCosmology of Theories beyond the SMWater Cherenkov DetectorBaryogenesisGoldstone bosonLeptogenesissymbolsDark energyHigh Energy Physics::ExperimentQuintessence
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Slow roll in simple non-canonical inflation

2007

17 pages, 4 figures.-- ISI Article Identifier: 000245945000008.-- ArXiv pre-print available at: http://arxiv.org/abs/astro-ph/0701343

High Energy Physics - TheoryAstrofísicaField (physics)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Kinetic termAstrophysicsAstrophysicsCurvature01 natural sciencesPower lawGeneral Relativity and Quantum CosmologyCosmological perturbation theory0103 physical sciencesStatistical physics010306 general physicsInflation (cosmology)PhysicsBasis (linear algebra)Slow roll010308 nuclear & particles physicsAstrophysics (astro-ph)HorizonSpectral densityFísicaAstronomy and AstrophysicsHigh Energy Physics - Theory (hep-th)K-inflationFlatnessPhysics of the early universe
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Self-accelerating solutions of scalar-tensor gravity

2007

Scalar-tensor gravity is the simplest and best understood modification of general relativity, consisting of a real scalar field coupled directly to the Ricci scalar curvature. Models of this type have self-accelerating solutions. In an example inspired by string dilaton couplings, scalar-tensor gravity coupled to ordinary matter exhibits a de Sitter type expansion, even in the presence of a {\it negative} cosmological constant whose magnitude exceeds that of the matter density. This unusual behavior does not require phantoms, ghosts or other exotic sources. More generally, we show that any expansion history can be interpreted as arising partly or entirely from scalar-tensor gravity. To dist…

PhysicsAstrofísicaGeneral relativityAstrophysics (astro-ph)FOS: Physical sciencesFísicaAstronomy and AstrophysicsCosmological constantAstrophysicsAstrophysicsGravitationTheoretical physicsHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)De Sitter universeDark energyDilatonScalar fieldQuintessence
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How sensitive to FCNC can $B^0$ CP asymmetries be?

1998

We show that the study of CP asymmetries in neutral B-meson decays provides a very sensitive probe of flavour-changing neutral currents (FCNC). We introduce two new angles, $\alpha_{SM}$ and $\beta_{SM}$, whose main feature is that they can be readily obtained from the measurement of the CP asymmetries $a_{J/\psi K_s}$, $a_{\pi^+ \pi^-}$ and the ratio $R_u \equiv|V_{ud}V_{ub}^*|/|V_{cd}V_{cb}^*|$, providing a quantitative test of the presence of new physics in a model-independent way. Assuming that new physics is due to the presence of an isosinglet down-type quark, we indicate how to reconstruct the unitarity quadrangles and point out that the measurements of the above asymmetries, within …

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityPhysics beyond the Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentParticle Physics - Phenomenology
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Flavor versus mass eigenstates in neutrino asymmetries: implications for cosmology

2017

We show that, if they exist, lepton number asymmetries ($L_\alpha$) of neutrino flavors should be distinguished from the ones ($L_i$) of mass eigenstates, since Big Bang Nucleosynthesis (BBN) bounds on the flavor eigenstates cannot be directly applied to the mass eigenstates. Similarly, Cosmic Microwave Background (CMB) constraints on mass eigenstates do not directly constrain flavor asymmetries. Due to the difference of mass and flavor eigenstates, the cosmological constraint on the asymmetries of neutrino flavors can be much stronger than conventional expectation, but not uniquely determined unless at least the asymmetry of the heaviest neutrino is well constrained. Cosmological constrain…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics and Astronomy (miscellaneous)media_common.quotation_subjectHigh Energy Physics::LatticeCosmic microwave backgroundCosmic background radiationFOS: Physical scienceslcsh:AstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesAsymmetryCosmologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesislcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Eigenvalues and eigenvectorsmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLepton numberHigh Energy Physics - Phenomenologylcsh:QC770-798High Energy Physics::ExperimentNeutrinoAstrophysics - Cosmology and Nongalactic Astrophysics
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Non-decoupling of Heavy Neutrinos and Lepton Flavour Violation

1995

We consider a class of models predicting new heavy neutral fermionic states, whose mixing with the light neutrinos can be naturally significant and produce observable effects below the threshold for their production. We update the indirect limits on the flavour non-diagonal mixing parameters that can be derived from unitarity, and show that significant rates are in general expected for one-loop-induced rare processes due to the exchange of virtual heavy neutrinos, involving the violation of the muon and electron lepton numbers. In particular, the amplitudes for $\mu$--$e$ conversion in nuclei and for $\mu\to ee^+e^-$ show a non-decoupling quadratic dependence on the heavy neutrino mass $M$,…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonUnitarityHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesObservableDecoupling (cosmology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoElectroweak scaleMixing (physics)Particle Physics - PhenomenologyLepton
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Phantom Dirac-Born-Infeld dark energy

2017

Motivated by the apparent discrepancy between Cosmic Microwave Background measurements of the Hubble constant and measurements from Type-Ia supernovae, we construct a model for Dark Energy with equation of state $w = p / ��< -1$, violating the Null Energy Condition. Naive canonical models of so-called "Phantom" Dark Energy require a negative scalar kinetic term, resulting in a Hamiltonian unbounded from below and associated vacuum instability. We construct a scalar field model for Dark Energy with $w < -1$, which nonetheless has a Hamiltonian bounded from below in the comoving reference frame, {\it i.e.} in the rest frame of the fluid. We demonstrate that the solution is a cosmologica…

PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsKinetic termRest frame01 natural sciencesGeneral Relativity and Quantum Cosmologysymbols.namesake0103 physical sciencesAttractorsymbolsEnergy conditionDark energyHamiltonian (quantum mechanics)010303 astronomy & astrophysicsScalar fieldAstrophysics - Cosmology and Nongalactic AstrophysicsMathematical physicsHubble's lawPhysical Review D
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CP Violation with Three Oscillating Neutrino Flavours

2000

We explore the prospects of observing leptonic CP violation in a neutrino factory in the context of a scenario with three strongly oscillating neutrinos able to account for the solar, the atmospheric and the LSND results. We address also the problems related with the fake asymmetries induced by the experimental device and by the presence of matter.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesContext (language use)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationNeutrino FactoryHigh Energy Physics::ExperimentNeutrino
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Implications of an axino LSP for naturalness

2014

Both the naturalness of the electroweak symmetry breaking and the resolution of the strong CP problem may require a small Higgsino mass $\mu$ generated by a realization of the DFSZ axion model. Assuming the axino is the lightest supersymmetric particle, we study its implications on $\mu$ and the axion scale. Copiously produced light Higgsinos at collider (effectively only neutral NLSP pairs) eventually decay to axinos leaving prompt multi-leptons or displaced vertices which are being looked for at the LHC. We use latest LHC7+8 results to derive current limits on $\mu$ and the axion scale. Various Higgsino-axino phenomenology is illustrated by comparing with a standard case without lightest …

PhysicsNuclear and High Energy PhysicsParticle physicsAxinoPhysics beyond the Standard ModelElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLightest Supersymmetric ParticleHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Strong CP problemHigh Energy Physics::ExperimentHiggsinoPhenomenology (particle physics)Axion
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Coleman-Weinberg inflation in light of Planck

2014

We revisit a single field inflationary model based on Coleman-Weinberg potentials. We show that in small field Coleman-Weinberg inflation, the observed amplitude of perturbations needs an extremely small quartic coupling of the inflaton, which might be a signature of radiative origin. However, the spectral index obtained in a standard cosmological scenario turns out to be outside the 2 sigma region of the Planck data. When a non-standard cosmological framework is invoked, such as brane-world cosmology in the Randall-Sundrum model, the spectral index can be made consistent with Planck data within 1 sigma, courtesy of the modification in the evolution of the Hubble parameter in such a scheme.…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Electroweak interactionFOS: Physical sciencesFísicaAstrophysics::Cosmology and Extragalactic AstrophysicsInflatonCosmologyHigh Energy Physics - Phenomenologysymbols.namesakeTheoretical physicsGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Randall–Sundrum modelQuantum electrodynamicsQuartic functionsymbolsSymmetry breakingPlanckAstrophysics - Cosmology and Nongalactic AstrophysicsHubble's law
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Spiral Inflation with Coleman-Weinberg Potential

2015

We apply the idea of spiral inflation to Coleman-Weinberg potential, and show that inflation matching well observations is allowed for a symmetry-breaking scale ranging from an intermediate scale to GUT scale even if the quartic coupling $\lambda$ is of $\mathcal{O}(0.1)$. The tensor-to-scalar ratio can be of $\mathcal{O}(0.01)$ in case of GUT scale symmetry-breaking.

PhysicsInflation (cosmology)Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Scale (ratio)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsLambdaCoupling (probability)01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsQuartic function0103 physical sciencesColeman–Weinberg potentialGrand Unified TheorySymmetry breaking010306 general physicsMathematical physicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Neutrino Masses and Lepton Flavour Violation in Thick Brane Scenarios

2001

We address the issue of lepton flavour violation and neutrino masses in the ``fat-brane'' paradigm, where flavour changing processes are suppressed by localising different fermion field wave-functions at different positions (in the extra dimensions) in a thick brane. We study the consequences of suppressing lepton number violating charged lepton decays within this scenario for lepton masses and mixing angles. In particular, we find that charged lepton mass matrices are constrained to be quasi-diagonal. We further consider whether the same paradigm can be used to naturally explain small Dirac neutrino masses by considering the existence of three right-handed neutrinos in the brane, and discu…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFermionLepton numberMAJORANAExtra dimensionsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoBraneParticle Physics - PhenomenologyLepton
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Exploring the intrinsic Lorentz-violating parameters at DUNE

2018

Neutrinos can push our search for new physics to a whole new level. What makes them so hard to be detected, what allows them to travel humongous distances without being stopped or deflected allows to amplify Planck suppressed effects (or effects of comparable size) to a level that we can measure or bound in DUNE. In this work we analyze the sensitivity of DUNE to CPT and Lorentz-violating interactions in a framework that allows a straightforward extrapolation of the bounds obtained to any phenomenological modification of the dispersion relation of neutrinos.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelLorentz transformationExtrapolationFOS: Physical sciences01 natural sciencesMeasure (mathematics)Partícules (Física nuclear)lcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciencessymbolsSensitivity (control systems)NeutrinoPlanck010306 general physicslcsh:PhysicsPhysics Letters B
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Transplanckian inflation as gravity echoes

2015

In this work, we show that, in the presence of non-minimal coupling to gravity, it is possible to generate sizeable tensor modes in single-field models without transplanckian field values. These transplanckian field values apparently needed in Einstein gravity to accommodate the experimental results may only be due to our insistence of imposing a minimal coupling of the inflaton field to gravity in a model with non-minimal couplings. We present three simple single-field models that prove that it is possible accommodate a large tensor-to-scalar ratio without requiring transplanckian field values within the slow-roll regime.

High Energy Physics - TheoryNuclear and High Energy PhysicsGravity (chemistry)Cosmology and Nongalactic Astrophysics (astro-ph.CO)Field (physics)FOS: Physical sciences01 natural sciencesGravitationTheoretical physicsGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesTensor010306 general physicsMinimal couplingPhysicsInflation (cosmology)010308 nuclear & particles physicsFísicaInflatonlcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Einstein field equationslcsh:PhysicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Gravity triggered neutrino condensates

2010

In this work we use the Schwinger-Dyson equations to study the possibility that an enhanced gravitational attraction triggers the formation of a right-handed neutrino condensate, inducing dynamical symmetry breaking and generating a Majorana mass for the right-handed neutrino at a scale appropriate for the seesaw mechanism. The composite field formed by the condensate phase could drive an early epoch of inflation. We find that to the lowest order, the theory does not allow dynamical symmetry breaking. Nevertheless, thanks to the large number of matter fields in the model, the suppression by additional powers in G of higher order terms can be compensated, boosting them up to their lowest ord…

PhysicsAstrofísicaNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Spontaneous symmetry breakingHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGravitationHigh Energy Physics - PhenomenologyExplicit symmetry breakingMAJORANASeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryNeutrinoAstrophysics - Cosmology and Nongalactic AstrophysicsLepton
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New physics vs new paradigms: distinguishing CPT violation from NSI

2019

Our way of describing Nature is based on local relativistic quantum field theories, and then CPT symmetry, a natural consequence of Lorentz invariance, locality and hermiticity of the Hamiltonian, is one of the few if not the only prediction that all of them share. Therefore, testing CPT invariance does not test a particular model but the whole paradigm. Current and future long baseline experiments will assess the status of CPT in the neutrino sector at an unprecedented level and thus its distinction from similar experimental signatures arising from non-standard interactions is imperative. Whether the whole paradigm is at stake or just the standard model of neutrinos crucially depends on th…

Physics::General PhysicsPhysics and Astronomy (miscellaneous)CPT symmetryPhysics beyond the Standard ModelFOS: Physical scienceslcsh:AstrophysicsLorentz covariance01 natural sciencesPartícules (Física nuclear)High Energy Physics - Experimentsymbols.namesakeTheoretical physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuantum field theory010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsLocalityHigh Energy Physics::PhenomenologyHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentNeutrinoHamiltonian (quantum mechanics)
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Electroweak phase transition in left-right symmetric models

1998

We study the finite-temperature effective potential of minimal left-right symmetric models containing a bidoublet and two triplets in the scalar sector. We perform a numerical analysis of the parameter space compatible with the requirement that baryon asymmetry is not washed out by sphaleron processes after the electroweak phase transition. We find that the spectrum of scalar particles for these acceptable cases is consistent with present experimental bounds.

PhysicsNuclear and High Energy PhysicsPhase transitionParticle physicsThermal quantum field theoryCritical phenomenaHigh Energy Physics::PhenomenologyScalar (mathematics)Electroweak interactionFísicaFOS: Physical sciencesParameter spaceSphaleronHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryPhysical Review D
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Non-decoupling and lepton number violation in left-right models

1996

We argue that large non-decoupling effects of heavy neutrinos can appear naturally in manifestly left-right symmetric models due to the minimization conditions of the scalar potential and the structure of vev's imposed by phenomenology. We derive constraints on off-diagonal light-heavy and heavy-heavy neutrino mixings from the searches for lepton violating decays $\mu\rightarrow e\gamma,$ $\mu\rightarrow e e^-e^+$ and $\mu-e$ conversion in nuclei. The most stringent limits come from the latter process because its amplitude shows a quadratic non-decoupling dependence on the heavy neutrino mass. Due to the suppression of right-handed currents by large $W_R$ mass the present experiments are no…

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaScalar potentialDecoupling (cosmology)Lepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quadratic equationAmplitudeHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentPhenomenology (particle physics)Lepton
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Oscillations, neutrino masses and scales of new physics

1999

We show that all the available experimental information involving neutrinos can be accounted for within the framework of already existing models where neutrinos have zero mass at tree level, but obtain a small Dirac mass by radiative corrections.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelDirac (software)FOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyTree (data structure)High Energy Physics - Phenomenology (hep-ph)Zero massRadiative transferHigh Energy Physics::ExperimentNeutrino
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Spontaneous baryogenesis in spiral inflation

2019

We examined the possibility of spontaneous baryogenesis driven by the inflaton in the scenario of spiral inflation, and found the parametric dependence of the late-time baryon number asymmetry. As a result, it is shown that, depending on the effective coupling of baryon/lepton number violating operators, it is possible to obtain the right amount of asymmetry even in the presence of a matter-domination era as long as such era is relatively short. In a part of the parameter space, the required expansion rate during inflation is close to the current upper-bound, and hence can be probed in the near future experiments.

Particle physicsPhysics and Astronomy (miscellaneous)media_common.quotation_subjectFOS: Physical scienceslcsh:AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsParameter space01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)media_commonInflation (cosmology)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInflatonLepton numberBaryonBaryogenesisHigh Energy Physics - Phenomenologylcsh:QC770-798Baryon numberEuropean Physical Journal C: Particles and Fields
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Quantum decoherence and neutrino data

2006

In this work we perform global fits of microscopic decoherence models of neutrinos to all available current data, including LSND and KamLAND spectral distortion results. In previous works on related issues the models used were supposed to explain LSND results by means of quantum gravity induced decoherence. However those models were purely phenomenological without any underlying microscopic basis. It is one of the main purposes of this article to use detailed microscopic decoherence models with complete positivity, to fit the data.The decoherence in these models has contributions not only from stochastic quantum gravity vacua operating as a medium, but also from conventional uncertainties i…

PhysicsNuclear and High Energy PhysicsQuantum decoherenceOscillationFOS: Physical sciencesFísicaNeutrino beamHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsQuantum gravityHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationOrder of magnitudeEnergy (signal processing)Nuclear Physics B
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Modified majoron model for cosmological anomalies

2020

The vacuum expectation value $v_s$ of a Higgs triplet field $\Delta$ carrying two units of lepton number $L$ induces neutrino masses $\propto v_s$. The neutral component of $\Delta$ gives rise to two Higgs particles, a pseudoscalar $A$ and a scalar $S$. The most general renormalizable Higgs potential $V$ for $\Delta $ and the Standard-Model Higgs doublet $\Phi$ does not permit the possibility that the mass of either $A$ or $S$ is small, of order $v_s$, while the other mass is heavy enough to forbid the decay $Z\to A S$ to comply with LEP 1 data. We present a model with additional dimension-6 terms in $V$, in which this feature is absent and either $A$ or $S$ can be chosen light. Subsequentl…

High Energy Astrophysical Phenomena (astro-ph.HE)PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)01 natural sciencesLepton numberPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonddc:530High Energy Physics::ExperimentNeutrinoAstrophysics - High Energy Astrophysical Phenomena010306 general physicsAstrophysics - Cosmology and Nongalactic AstrophysicsVacuum expectation valueMajoronBosonPhysical Review D
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Gravitino dark matter in the constrained next-to-minimal supersymmetric standard model with neutralino next-to-lightest superpartner

2010

The viability of a possible cosmological scenario is investigated. The theoretical framework is the constrained next-to-minimal supersymmetric standard model (cNMSSM), with a gravitino playing the role of the lightest supersymmetric particle (LSP) and a neutralino acting as the next-to-lightest supersymmetric particle (NLSP). All the necessary constraints from colliders and cosmology have been taken into account. For gravitino we have considered the two usual production mechanisms, namely out-of equillibrium decay from the NLSP, and scattering processes from the thermal bath. The maximum allowed reheating temperature after inflation, as well as the maximum allowed gravitino mass are determi…

High Energy Physics - TheoryPhysicsInflation (cosmology)Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesSuperpartnerFísicaGeneral Relativity and Quantum Cosmology (gr-qc)Lightest Supersymmetric ParticleGeneral Relativity and Quantum CosmologyNext-to-Minimal Supersymmetric Standard ModelHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)NeutralinoGravitinoHigh Energy Physics::ExperimentAstrophysics - Cosmology and Nongalactic AstrophysicsMinimal Supersymmetric Standard Model
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Constraining New Physics with the Fermilab Measurement ofCPViolation inB→ψKs

1999

Recently, the CDF Collaboration has reported a measurement of the CP asymmetry in the $B\ensuremath{\rightarrow}\ensuremath{\psi}{K}_{s}$ decay: ${a}_{\ensuremath{\psi}{K}_{s}}{\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.79}_{\ensuremath{-}0.44}^{+0.41}$. We analyze the constraints that follow from this measurement on the size and the phase of contributions from new physics to $B\ensuremath{-}\overline{B}$ mixing. Defining the relative phase between the full ${M}_{12}$ amplitude and the standard model contribution to be $2{\ensuremath{\theta}}_{d}$, we find a new bound: $\mathrm{sin}2{\ensuremath{\theta}}_{d}\ensuremath{\gtrsim}\ensuremath{-}0.6(\ensuremath{-}0.87)$ at $1\ensuremat…

PhysicsParticle physicsPhysics beyond the Standard ModelGeneral Physics and AstronomyFermilabRelative phaseStandard ModelPhysical Review Letters
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