Search results for "BN"

showing 10 items of 1136 documents

Clinical, pathologic, and genetic features of massive soft tissue neurofibromas in a Sicilian patient

2008

Abstract CONTEXT: Lipase maturation factor 1 (LMF1) gene is a novel candidate gene in severe hypertriglyceridemia. Lmf1 is involved in the maturation of lipoprotein lipase (LPL) and hepatic lipase in endoplasmic reticulum. To date only one patient with severe hypertriglyceridemia and related disorders was found to be homozygous for a nonsense mutation in LMF1 gene (Y439X). OBJECTIVE: The objective of the study was to investigate LMF1 gene in hypertriglyceridemic patients in whom mutations in LPL, APOC2, and APOA5 genes had been excluded. RESULTS: The resequencing of LMF1 gene led to the discovery of a novel homozygous nonsense mutation in one patient with severe hypertriglyceridemia and rec…

Nonsynonymous substitutionMalecongenital hereditary and neonatal diseases and abnormalitiesPathologymedicine.medical_specialtyHeterozygoteNeurofibromatosis 1BiopsyDNA Mutational AnalysisMutation MissenseSoft Tissue NeoplasmsDermatologymassive soft tissue neurofibromas NeurofibromatosisBiologymedicine.disease_causeFrameshift mutationExonGenes Neurofibromatosis 1medicineSettore MED/35 - Malattie Cutanee E VenereeMissense mutationHumansNeurofibromatosisFrameshift MutationGeneSicilyGeneticsMutationHeterozygote advantageGeneral MedicineExonsMiddle Agedmedicine.diseasenervous system diseasesGene Expression Regulation NeoplasticButtocks
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Permutable subnormal subgroups of finite groups

2009

The aim of this paper is to prove certain characterization theorems for groups in which permutability is a transitive relation, the so called PT -groups. In particular, it is shown that the finite solvable PT -groups, the finite solvable groups in which every subnormal subgroup of defect two is permutable, the finite solvable groups in which every normal subgroup is permutable sensitive, and the finite solvable groups in which conjugatepermutability and permutability coincide are all one and the same class. This follows from our main result which says that the finite modular p-groups, p a prime, are those p-groups in which every subnormal subgroup of defect two is permutable or, equivalentl…

Normal subgroupClass (set theory)PermutableMathematics::CombinatoricsGeneral MathematicsSubnormalModular p-groupGrups Teoria deCharacterization (mathematics)Prime (order theory)PT -groupSubnormal subgroupCombinatoricsMathematics::Group TheorySolvable groupPermutable primeÀlgebraAlgebra over a fieldMATEMATICA APLICADAMathematicsConjugate-Permutable
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On finite groups generated by strongly cosubnormal subgroups

2003

[EN] Two subgroups A and B of a group G are cosubnormal if A and B are subnormal in their join and are strongly cosubnormal if every subgroup of A is cosubnormal with every subgroup of B. We find necessary and sufficient conditions for A and B to be strongly cosubnormal in and, if Z is the hypercentre of G=, we show that A and B are strongly cosubnormal if and only if G/Z is the direct product of AZ/Z and BZ/Z. We also show that projectors and residuals for certain formations can easily be constructed in such a group. Two subgroups A and B of a group G are N-connected if every cyclic subgroup of A is cosubnormal with every cyclic subgroup of B (N denotes the class of nilpotent groups). Thou…

Normal subgroupFinite groupHypercentreAlgebra and Number TheoryStrongly cosubnormal subgroupsFormationN-connected subgroupsFitting subgroupCombinatoricsSubnormal subgroupSubgroupLocally finite groupCharacteristic subgroupIndex of a subgroupFinite groupMATEMATICA APLICADAMatemàticaSubnormal subgroupMathematicsNilpotent group
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First observation of a baryonic Bc+ decay

2014

A baryonic decay of the $B_c^+$ meson, $B_c^+\to J/\psi p\overline{p}\pi^+$, is observed for the first time, with a significance of $7.3$ standard deviations, in $pp$ collision data collected with the LHCb detector and corresponding to an integrated luminosity of $3.0$ fb$^{-1}$ taken at center-of-mass energies of $7$ and $8$ $\mathrm{TeV}$. With the $B_c^+\to J/\psi \pi^+$ decay as normalization channel, the ratio of branching fractions is measured to be \begin{equation*} \frac{\mathcal{B}(B_c^+\to J/\psi p\overline{p}\pi^+)}{\mathcal{B}(B_c^+\to J/\psi \pi^+)} = 0.143^{\,+\,0.039}_{\,-\,0.034}\,(\mathrm{stat})\pm0.013\,(\mathrm{syst}). \end{equation*} The mass of the $B_c^+$ meson is dete…

Nuclear TheoryAnalytical chemistryGeneral Physics and Astronomy01 natural sciencesSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]TOOLFactorizationNuclear ExperimentQCPhysicsPhysicsParticle physics12.39.StPhysical SciencesComputer Science::Mathematical SoftwareFísica nuclearLHCMESONParticle Physics - ExperimentComputer Science::Machine LearningMeson530 Physics14.40.NdPhysics MultidisciplinaryFOS: Physical sciencesPhysics InstituteLHCb - Abteilung HofmannAstrophysics::Cosmology and Extragalactic AstrophysicsComputer Science::Digital LibrariesNONuclear physicsPhysics and Astronomy (all)Hadronic decays of bottom meson0103 physical sciencesPi010306 general physicsScience & Technology010308 nuclear & particles physicshep-exHigh Energy Physics::Phenomenologymeson; toolBaryonLHCb13.25.HwBottom mesons (|B|>0)High Energy Physics::ExperimentFísica de partículesExperiments
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Precision Measurement of the Mass and Lifetime of the Ξ[0 over b] Baryon

2014

Using a proton-proton collision data sample corresponding to an integrated luminosity of 3 fb$^{-1}$ collected by LHCb at center-of-mass energies of 7 and 8 TeV, about 3800 $\Xi_b^0\to\Xi_c^+\pi^-$, $\Xi_c^+\to pK^-\pi^+$ signal decays are reconstructed. From this sample, the first measurement of the $\Xi_b^0$ baryon lifetime is made, relative to that of the $\Lambda_b^0$ baryon. The mass differences $M(\Xi_b^0)-M(\Lambda_b^0)$ and $M(\Xi_c^+)-M(\Lambda_c^+)$ are also measured with precision more than four times better than the current world averages. The resulting values are $\frac{\tau_{\Xi_b^0}}{\tau_{\Lambda_b^0}} = 1.006\pm0.018\pm0.010$, $M(\Xi_b^0) - M(\Lambda_b^0) = 172.44\pm0.39\pm…

Nuclear TheoryAnalytical chemistryGeneral Physics and Astronomyinclusive weak decays; discarding 1/N(C); beaty; charm; ruleLambdaHigh Energy Physics - Experimenthigh energy physicsSettore FIS/04 - Fisica Nucleare e Subnucleare[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]INCLUSIVE WEAK DECAYS; DISCARDING 1/N(C); BEAUTY; CHARM; RULENuclear ExperimentQCPhysicsprecision measurementPhysicsintegrated luminosityParticle physicsBEAUTYtransverse momentaPseudorapidityPhysical SciencesTransverse momentumINCLUSIVE WEAK DECAYSFísica nuclearLHC13.30.Egtellurium compoundsParticle Physics - Experiment530 PhysicsAstrophysics::High Energy Astrophysical PhenomenaPhysics MultidisciplinarypseudorapiditiesPhysics InstituteLHCb - Abteilung HofmannAstrophysics::Cosmology and Extragalactic AstrophysicsCHARMNuclear physicsPhysics and Astronomy (all)Pi14.20.MrScience & Technologycenter-of-mass energiesmass differencetransverse momenta; precision measurement; center-of-mass energies; tellurium compounds; production rates; pseudorapidities; high energy physics; integrated luminosity; hadrons; mass difference; proton proton collisionsDISCARDING 1/N(C)BaryonLHCbproton proton collisionshadronsHadronic decays of baryonBottom baryons (|B|>0)Physics::Accelerator Physicsproduction ratesFísica de partículesExperimentsRULE
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Performance of the ATLAS detector using first collision data

2010

More than half a million minimum-bias events of LHC collision data were collected by the ATLAS experiment in December 2009 at centre-of-mass energies of 0.9 TeV and 2.36 TeV. This paper reports on studies of the initial performance of the ATLAS detector from these data. Comparisons between data and Monte Carlo predictions are shown for distributions of several track- and calorimeter-based quantities. The good performance of the ATLAS detector in these first data gives confidence for successful running at higher energies.

Nuclear and High Energy PhysicsParticle physicsAtlas detectorPhysics::Instrumentation and DetectorsMonte Carlo methodFOS: Physical sciencesddc:500.253001 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)LHC ; ATLAS ; Minimum-bias ; 900 GeV ; 2.36 TeV ; PerformanceAtlas (anatomy)0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy PhysicsDetectors and Experimental Techniques010306 general physicsCiencias ExactasDetectors de radiacióPhysicsHadron-Hadron ScatteringLarge Hadron Collider010308 nuclear & particles physicsATLAS DetectorSettore FIS/01 - Fisica SperimentaleATLAS experimentFísicaATLASCollisionmedicine.anatomical_structureExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Search for events with large missing transverse momentum, jets, and at least two tau leptons in 7 TeV proton–proton collision data with the ATLAS det…

2012

A search for events with large missing transverse momentum, jets, and at least two tau leptons has been performed using 2 fb[superscript −1] of proton–proton collision data at √s = 7 TeV recorded with the ATLAS detector at the Large Hadron Collider. No excess above the Standard Model background expectation is observed and a 95% CL upper limit on the visible cross section for new phenomena is set, where the visible cross section is defined by the product of cross section, branching fraction, detector acceptance and event selection efficiency. A 95% CL lower limit of 32 TeV is set on the gauge-mediated supersymmetry breaking (GMSB) scale Λ independent of tan β. These limits provide the most s…

Nuclear and High Energy PhysicsParticle physicsAtlas detectortau leptonsAstrophysics::High Energy Astrophysical PhenomenaPhysics beyond the Standard ModelMonte Carlo methodFOS: Physical sciencesddc:500.27. Clean energy01 natural sciences530Partícules (Física nuclear)Settore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)tau leptons; jets; ATLAS detector0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physicstransverse momentum: missing-energy; new physics; Monte Carlo; supersymmetry: symmetry breaking; 70000 GeV-cms; jet: multiple production; mediation: gauge; supersymmetry: parameter space; tau: semileptonic decay; CERN LHC Coll; ATLAS; p p --> (n)jet 2tau anything; experimental results; cross section: upper limit; p p: scattering010306 general physicsNuclear ExperimentCiencias ExactasDetectors de radiacióPhysics010308 nuclear & particles physicsAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaATLASCollisionDYNAMICAL SUPERSYMMETRY BREAKINGHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsTransverse momentumComputingMethodologies_DOCUMENTANDTEXTPROCESSINGPhysics::Accelerator Physicsproton-proton collisionsHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentLepton
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Measurement of the B-0 -> K*(0) e(+) e(-) branching fraction at low dilepton mass

2013

The branching fraction of the rare decay B-0 -> K*(0) e(+) e(-) in the dilepton mass region from 30 to 1000 MeV/c(2) has been measured by the LHCb experiment, using pp collision data, corresponding to an integrated luminosity of 1.0 fb(-1), at a centre-of-mass energy of 7 TeV. The decay mode B-0 -> J/psi (e(+) e(-)) K*(0) is utilized as a normalization channel. The branching fraction B(B-0 -> K*(0) e(+) e(-)) is measured to be B(B-0 -> K*(0) e(+) e(-))(30-1000 MeV/c2) = (3.1(-0.8)(-0.3)(+0.9)(+0.2) +/- 0.2) x 10(-7) where the fi rst error is statistical, the second is systematic, and the third comes from the uncertainties on the B-0 -> J/K*(0) and J/psi -> e(+) e(-) branching fractions.

Nuclear and High Energy PhysicsParticle physicsB physicModels beyond the standard modelFlavour Changing Neutral CurrentsFOS: Physical sciencesHadrons01 natural sciencesDECAYSB physicsPartícules (Física nuclear)High Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNeutral currentHigh Energy Physics - Experiment (hep-ex)Neutral currents0103 physical sciencesLeptonic semileptonic and radiative decays of bottom meson[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]TOOLDECAYS; TOOL010306 general physicsLarge Hadron Collider (France and Switzerland)QCPhysicsFlavour Changing Neutral CurrentHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionB physics; Branching fraction; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decayHigh Energy Physics::PhenomenologyGran Col·lisionador d'Hadrons3. Good healthCromodinàmica quànticaFIS/01 - FISICA SPERIMENTALERare decayB physics; Branching fraction; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decay; Nuclear and High Energy PhysicsBottom mesons (|B|>0); Leptonic semileptonic and radiative decays of bottom mesons; Neutral currents; Models beyond the standard modelLeptonic semileptonic and radiative decays of bottom mesonsBottom mesons (|B|>0)Branching fractionHigh Energy Physics::ExperimentFísica nuclearDECAYParticle Physics - ExperimentQuantum chromodynamics
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Extending the DAMA annual-modulation region by inclusion of the uncertainties in astrophysical velocities

1999

The original annual-modulation region, singled out by the DAMA/NaI experiment for direct detection of WIMPs, is extended by taking into account the uncertainties in the galactic astrophysical velocities. Also the effect due to a possible bulk rotation for the dark matter halo is considered. We find that the range for the WIMP mass becomes 30 GeV < m_chi < 130 GeV at 1-sigma C.L. with a further extension in the upper bound, when a possible bulk rotation of the dark matter halo is taken into account. We show that the DAMA results, when interpreted in the framework of the Minimal Supersymmetric extension of the Standard Model, are consistent with a relic neutralino as a dominant componen…

Nuclear and High Energy PhysicsParticle physicsDAMA/LIBRACold dark matterDark matterFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsAstrophysicsSettore FIS/04 - Fisica Nucleare e SubnucleareGalactic haloHigh Energy Physics - Phenomenology (hep-ph)DARK-MATTERSUPERSYMMETRYLight dark matterPhysicsDARK-MATTER; Dark matter annual modulation signature; SUPERSYMMETRY; SIGNAL;Settore FIS/01 - Fisica SperimentaleAstrophysics (astro-ph)Astrophysics::Instrumentation and Methods for AstrophysicsSIGNALDark matter haloHigh Energy Physics - PhenomenologyDark matter annual modulation signatureWeakly interacting massive particlesDAMA/NaI
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Searches for violation of lepton flavour and baryon number in tau lepton decays at LHCb

2013

Searches for the lepton flavour violating decay tau(-) -> mu(-)mu(+)mu(-) and the lepton flavour and baryon number violating decays tau(-) -> (p) over bar mu(+)mu(-) and tau(-) -> p mu(-)mu(-) have been carried out using proton-proton collision data, corresponding to an integrated luminosity of 1.0 fb(-1), taken by the LHCb experiment at root s = 7 TeV. No evidence has been found for any signal, and limits have been set at 90% confidence level on the branching fractions: B(tau(-) -> mu(-)mu(+)mu(-) mu(+)mu(-)) p mu(-)mu(-)) (p) over bar mu(+)mu(-) and tau(-) -> p mu(-)mu(-) decay modes represent the first direct experimental limits on these channels.

Nuclear and High Energy PhysicsParticle physicsFlavourDecays of leptons; Global symmetries (e.g. baryon number lepton number); 13.35.-r; 11.30.Fs;FOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNuclear physicslepton number)High Energy Physics - Experiment (hep-ex)Violació CP (Física nuclear)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]LHC flavour physics lepton number11.30.FsNeutrinsNeutrinos010306 general physicsParticles (Nuclear physics)Physics13.35.-rDecays of leptonsLarge Hadron Collider010308 nuclear & particles physicsGlobal symmetries (e.g. baryon number lepton number)Leptons (Física nuclear)Global symmetries (e.g.High Energy Physics::Phenomenologybaryon numberDecays of lepton3. Good healthFIS/01 - FISICA SPERIMENTALELeptons (Nuclear physics)Física nuclearHigh Energy Physics::ExperimentBaryon numberNeutrino11.30.FFIS/04 - FISICA NUCLEARE E SUBNUCLEAREParticle Physics - ExperimentLeptonCP violation (Nuclear physics)Physics Letters B
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