0000000001203458

AUTHOR

O. Vives

showing 10 related works from this author

Flavour-changing Higgs decays into bottom and strange quarks in supersymmetry

2015

In this work, we explore the flavour changing decays $H_i \to b s$ in a general supersymmetric scenario. In these models, the flavour changing decays arise at loop-level but, originating from a dimension-four operator, do not decouple and may provide a first sign of new physics for heavy masses beyond collider reach. In the framework of the minimal supersymmetric extension of the Standard Model (MSSM), we find that the largest branching ratio of the lightest Higgs ($H_1$) is ${\cal O}(10^{-6})$ after imposing present experimental constraints. While heavy Higgs states may still present branching ratios ${\cal O}(10^{-3})$. In a more general supersymmetric scenario, where additional Higgs sta…

High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::ExperimentHigh Energy Physics - Experiment
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Magnetic Monopole Search with the Full MoEDAL Trapping Detector in 13 TeV pp Collisions Interpreted in Photon-Fusion and Drell-Yan Production

2019

MoEDAL is designed to identify new physics in the form of stable or pseudostable highly ionizing particles produced in high-energy Large Hadron Collider (LHC) collisions. Here we update our previous search for magnetic monopoles in Run 2 using the full trapping detector with almost four times more material and almost twice more integrated luminosity. For the first time at the LHC, the data were interpreted in terms of photon-fusion monopole direct production in addition to the Drell-Yan-like mechanism. The MoEDAL trapping detector, consisting of 794 kg of aluminum samples installed in the forward and lateral regions, was exposed to 4.0 fb$^{-1}$ of 13 TeV proton-proton collisions at the LHC…

General PhysicsPhotonPhysics beyond the Standard ModelPhysics MultidisciplinaryMagnetic monopoleGeneral Physics and AstronomyFOS: Physical sciencesddc:500.27. Clean energy01 natural sciences114 Physical sciencesMoEDAL Collaboration09 EngineeringHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)STOPPING-POWER0103 physical sciences010306 general physicsPROTON COLLISIONS01 Mathematical SciencesParticle Physics - PhenomenologyPhysicsLarge Hadron ColliderLuminosity (scattering theory)Science & Technology02 Physical SciencesMagnetic monopoleInteraction pointhep-exDirac (video compression format)PhysicsCharge (physics)hep-phHigh Energy Physics - PhenomenologyPhysical SciencesLHCParticle Physics - Experiment
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Gamma-Z interferometry at a phi-factory

1995

We analyze the possibilities that the proposed $\Phi$-factories offer to measure $\gamma-Z$ interference. In the unpolarized beam case, we study different signatures in the $\rho \pi$ channel, taking advantage of the presence of the near-by $a_1$ resonance. We build a C-odd forward-backward asymmetry, estimated to be around $10^{-5}$, and (P-even, T-even) and (P-odd, T-odd) alignments of the $\rho$, to be seen from the angular distribution of its $\pi \pi$ decay products. With polarized electrons a left-right asymmetry around $2\times 10^{-4}$ is present in all channels. At leading order this asymmetry is independent of hadronic matrix elements and is sensitive to the $Z^0-s\bar{s}$ vector …

High Energy Physics - PhenomenologyFísicaHigh Energy Physics::Experiment
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Physics demos for all UVEG degrees: a unique project in Spain

2016

Abstract The Physics Demo Project at the University of Valencia ( www.uv.es/fisicademos ) has developed a collection of physics demonstrations to be used during lectures. It consists of more than 130 experimental demos about different physics topics. More than 30 professors borrow them whenever they lecture on physics in any of our 40 courses in 17 different science or technical degrees, involving 246 ECTS and more than 3500 students. Each demo kit with a simple experimental set displays a particular physics phenomenon. An on-line user guide highlights the main physics principles involved, instructions on how to use it and advices of how to link it to the theoretical concepts or to technica…

EngineeringPhysics education0211 other engineering and technologiesphysical phenomena02 engineering and technologyCiència Experimentsphysics demonstrationsHuman–computer interactionPhysical phenomenaPhenomenon0502 economics and businessMathematics educationteaching teamwork.demosGeneral Materials ScienceEveryday lifeSet (psychology)business.industry05 social sciencesFísicainnovative physics teaching021107 urban & regional planningexperimentsLecture hallCiència EnsenyamentScientific methodscientific methodbusiness050203 business & management
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On the full Boltzmann equations for leptogenesis

2009

We consider the full Boltzmann equations for standard and soft leptogenesis, instead of the usual integrated Boltzmann equations which assume kinetic equilibrium for all species. Decays and inverse decays may be inefficient for thermalising the heavy-(s)neutrino distribution function, leading to significant deviations from kinetic equilibrium. We analyse the impact of using the full kinetic equations in the case of a previously generated lepton asymmetry, and find that the washout of this initial asymmetry due to the interactions of the right-handed neutrino is larger than when calculated via the integrated equations. We also solve the full Boltzmann equations for soft leptogenesis, where t…

PhysicsleptogenesisParticle physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyFOS: Physical sciencesInverseFísicaAstronomy and AstrophysicsKinetic energyAsymmetrysymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution functionneutrino theoryLeptogenesisBoltzmann constantsymbolsphysics of the early universeHigh Energy Physics::ExperimentNeutrinomedia_commonLepton
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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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Prospects for discovering supersymmetric long-lived particles with MoEDAL

2020

We present a study on the possibility of searching for long-lived supersymmetric partners with the MoEDAL experiment at the LHC. MoEDAL is sensitive to highly ionising objects such as magnetic monopoles or massive (meta)stable electrically charged particles. We focus on prospects of directly detecting long-lived sleptons in a phenomenologically realistic model which involves an intermediate neutral long-lived particle in the decay chain. This scenario is not yet excluded by the current data from ATLAS or CMS, and is compatible with astrophysical constraints. Using Monte Carlo simulation, we compare the sensitivities of MoEDAL versus ATLAS in scenarios where MoEDAL could provide discovery re…

Astrophysics and AstronomyParticle physicsPhysics and Astronomy (miscellaneous)Regular Article - Experimental PhysicsPhysics::Instrumentation and DetectorsMagnetic monopoleFOS: Physical scienceslcsh:AstrophysicsElementary particle01 natural sciencesHigh Energy Physics - ExperimentParticle decayHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityInvariant mass010306 general physicsEngineering (miscellaneous)Particle Physics - Phenomenologyastro-ph.HEPhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)Large Hadron Colliderhep-ex010308 nuclear & particles physicsSuperpartnerhep-phSupersymmetryHigh Energy Physics - PhenomenologyMoEDAL experimentlcsh:QC770-798Astrophysics - High Energy Astrophysical PhenomenaParticle Physics - ExperimentEuropean Physical Journal
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Tree-level flavor-changing neutral currents in the B system: From CP asymmetries to rare decays

2001

Tree-level flavor-changing neutral currents (FCNC) are characteristic of models with extra vectorlike quarks. These new couplings can strongly modify the B/sup 0/ CP asymmetries without conflicting with low-energy constraints. In the light of low CP asymmetry in B to J/ psi K/sub S/, we discuss the implications of these contributions. We find that even these low values can be easily accommodated in these models. Furthermore, we show that the new data from B factories tend to favor an O(20) enhancement of the b to dll transition over the SM expectation. (25 refs).

FísicaParticle Physics - Phenomenology
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Search for magnetic monopoles with the MoEDAL prototype trapping detector in 8 TeV proton-proton collisions at the LHC

2016

The MoEDAL experiment is designed to search for magnetic monopoles and other highly-ionising particles produced in high-energy collisions at the LHC. The largely passive MoEDAL detector, deployed at Interaction Point 8 on the LHC ring, relies on two dedicated direct detection techniques. The first technique is based on stacks of nuclear-track detectors with surface area $\sim$18 m$^2$, sensitive to particle ionisation exceeding a high threshold. These detectors are analysed offline by optical scanning microscopes. The second technique is based on the trapping of charged particles in an array of roughly 800 kg of aluminium samples. These samples are monitored offline for the presence of trap…

ExoticsParticle physicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsProtonMagnetic monopoleFOS: Physical sciencesddc:500.2Particle and resonance production114 Physical sciences7. Clean energy01 natural sciencesMathematical SciencesHigh Energy Physics - Experimentlaw.inventionCOLLIDERHigh Energy Physics - Experiment (hep-ex)MAGNETIC MONOPOLESSTOPPING-POWERlawHadron-Hadron scattering (experiments)0103 physical sciencesFIELD010306 general physicsColliderHIGHLY IONIZING PARTICLESphysics.ins-detPhysicsOPALLarge Hadron ColliderSTABLE MASSIVE PARTICLEShep-ex010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Nuclear & Particles PhysicsPair productionMoEDAL experimentPhysical SciencesProduction (computer science)CHARGEParticle Physics - ExperimentEnergy (signal processing)Exotic
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Improved $\tau$-weapons for Higgs hunting

2013

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…

High Energy Physics - PhenomenologyHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment
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