Search results for "Zeros"

showing 9 items of 9 documents

Abelian realization of phenomenological two-zero neutrino textures

2014

In an attempt at explaining the observed neutrino mass-squared differences and leptonic mixing, lepton mass matrices with zero textures have been widely studied. In the weak basis where the charged lepton mass matrix is diagonal, various neutrino mass matrices with two zeros have been shown to be consistent with the current experimental data. Using the canonical and Smith normal form methods, we construct the minimal Abelian symmetry realizations of these phenomenological two-zero neutrino textures. The implementation of these symmetries in the context of the seesaw mechanism for Majorana neutrino masses is also discussed.

CP ViolationPhysicsSterile neutrinoParticle physicsNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesZerosHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismMass Matrix0103 physical sciencesCP violationlcsh:QC770-798High Energy Physics::Experimentlcsh:Nuclear and particle physics. Atomic energy. RadioactivityAbelian groupNeutrino010306 general physicsNeutrino oscillationLeptonNuclear Physics B
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Further monotonicity and convexity properties of the zeros of cylinder functions

1992

AbstractLet cvk be the kth positive zero of the cylinder function Cv(x,α)=Jv(x) cos α−Yv sin α, 0⩽α<π, where Jv(x) and Yv(x) are the Bessel functions of the first and the second kind, respectively. We prove that the function v(d2cvkddv2+δ)cvk increases with v⩾0 for suitable values of δ and k−απ⩾ 0.7070… . From this result under the same conditions we deduce, among other things, that cvk+12δv2 is convex as a function of v⩾0. Moreover, we show some monotonicity properties of the function c2vkv. Our results improve known results.

CerobiologyApplied MathematicsMathematical analysisRegular polygonZero (complex analysis)Monotonic functionFunction (mathematics)biology.organism_classificationConvexityCombinatoricsComputational Mathematicssymbols.namesakeZeros of Bessel functionssymbolsConvex functionBessel functionMathematicsJournal of Computational and Applied Mathematics
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On the orders of zeros of irreducible characters

2009

Let G be a finite group and p a prime number. We say that an element g in G is a vanishing element of G if there exists an irreducible character χ of G such that χ (g) = 0. The main result of this paper shows that, if G does not have any vanishing element of p-power order, then G has a normal Sylow p-subgroup. Also, we prove that this result is a generalization of some classical theorems in Character Theory of finite groups. © 2008 Elsevier Inc. All rights reserved.

Discrete mathematicsFinite groupPure mathematicsBrauer's theorem on induced charactersAlgebra and Number Theoryirreducible character zeroCharacter theorySylow theoremsPrime numberIrreducible elementFinite groupsCharacter (mathematics)Order (group theory)Zeros of charactersCharactersMathematics
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Existence theorems for m-accretive operators in Banach spaces

2005

Abstract In 1985, the second author proved a surjective result for m -accretive and ϕ -expansive mappings for uniformly smooth Banach spaces. However, in this case, we have been able to remove the uniform smoothness of the Banach space, without any additional assumption.

Discrete mathematicsMathematics::Functional AnalysisZeros for m-accretive operatorsApproximation propertySurjectivityApplied MathematicsEberlein–Šmulian theoremAccretivityUniformly convex spaceBanach manifoldFinite-rank operatorInterpolation spaceOpen mapping theorem (functional analysis)Lp spaceAnalysisMathematicsJournal of Mathematical Analysis and Applications
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Non-vanishing elements of finite groups

2010

AbstractLet G be a finite group, and let Irr(G) denote the set of irreducible complex characters of G. An element x of G is non-vanishing if, for every χ in Irr(G), we have χ(x)≠0. We prove that, if x is a non-vanishing element of G and the order of x is coprime to 6, then x lies in the Fitting subgroup of G.

Finite groupBrauer's theorem on induced charactersAlgebra and Number TheoryCoprime integers010102 general mathematics0102 computer and information sciences01 natural sciencesFitting subgroupFinite groupsCombinatorics010201 computation theory & mathematicsOrder (group theory)Zeros of charactersCharacters0101 mathematicsElement (category theory)MathematicsJournal of Algebra
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Zeros of {-1,0,1}-power series and connectedness loci for self-affine sets

2006

We consider the set W of double zeros in (0,1) for power series with coefficients in {-1,0,1}. We prove that W is disconnected, and estimate the minimum of W with high accuracy. We also show that [2^(-1/2)-e,1) is contained in W for some small, but explicit e&gt;0 (this was only known for e=0). These results have applications in the study of infinite Bernoulli convolutions and connectedness properties of self-affine fractals.

Power seriesDiscrete mathematics28A80Social connectednessGeneral Mathematics010102 general mathematics01 natural sciencesSet (abstract data type)Bernoulli's principleFractal30C1528A80 30B10Mathematics - Classical Analysis and ODEs0103 physical sciencesClassical Analysis and ODEs (math.CA)FOS: Mathematicsself-affine fractals010307 mathematical physicsAffine transformationZeros of power series0101 mathematicsMathematics
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The Large Hadron–Electron Collider at the HL-LHC

2021

The Large Hadron-Electron Collider (LHeC) is designed to move the field of deep inelastic scattering (DIS) to the energy and intensity frontier of particle physics. Exploiting energy-recovery technology, it collides a novel, intense electron beam with a proton or ion beam from the High-Luminosity Large Hadron Collider (HL-LHC). The accelerator and interaction region are designed for concurrent electron-proton and proton-proton operations. This report represents an update to the LHeC's conceptual design report (CDR), published in 2012. It comprises new results on the parton structure of the proton and heavier nuclei, QCD dynamics, and electroweak and top-quark physics. It is shown how the LH…

energy recoverylepton nucleus: scatteringparton: distribution functionhiukkasfysiikka7. Clean energy01 natural sciencesaccelerator physicsHigh Energy Physics - Phenomenology (hep-ph)HEAVY FLAVOR CONTRIBUTIONSenergy-recovery- linacNuclear Experimentcolliding beams [electron p]deep-inelastic scatteringtop and electroweak physicsnew physicsPhysicsSTRUCTURE-FUNCTION RATIOSMonte Carlo [numerical calculations]buildingsprimary [vertex]High Energy Physics - Phenomenologyelectron p: colliding beamskinematicsNuclear Physics - Theoryfinal state: hadronicp: distribution functionbeyond Standard Modelvertex: primarynumerical calculations: Monte Carlodistribution function [parton]High-lumiLHCSTRUCTURE-FUNCTION F-2(X[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]ion: beam[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesNuclear Theory (nucl-th)deep inelastic scatteringquantum chromodynamicsddc:530010306 general physicsdeep-inelastic scattering; high-lumi LHC; QCD; Higgs; top and electroweak physics; nuclear physics; beyond standard Model; energy-recovery- linac; accelerator physics010308 nuclear & particles physicshigh-lumi LHCresolutionscattering [electron p]structure function [nucleus]sensitivitybeam [electron]energy-recovery-linacHiggsacceptanceNuclear TheoryHIGH-ENERGY FACTORIZATIONdistribution function [p]density [parton]Higgs; High-lumi LHCHigh Energy Physics - Experimentdesign [detector]High Energy Physics - Experiment (hep-ex)electron: linear acceleratorelectron hadron: scatteringCERN LHC Coll: upgrade[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [electron hadron]FCCelectron: beamNuclear Experiment (nucl-ex)linear accelerator [electron]Nuclear ExperimentlatticesuperconductivityEnergy-recoverylinacBeyond Standard ModeNuclear physics; QCDelectron nucleus: colliding beamsparton: densitycolliding beams [electron nucleus]Particle Physics - ExperimentNUCLEON STRUCTURE FUNCTIONSNuclear and High Energy Physicsscattering [lepton nucleus]beam [ion]FOS: Physical sciencesnucleus: structure functionhadronic [final state]electron p: scatteringTRANSVERSE-MOMENTUM DEPENDENCEnuclear physics0103 physical sciencesNuclear Physics - Experimentstructureupgrade [CERN LHC Coll]detector: designParticle Physics - PhenomenologyDEEP-INELASTIC-SCATTERINGelectroweak interaction3-LOOP SPLITTING FUNCTIONSCLASSICAL RADIATION ZEROScalibrationAccelerators and Storage RingsQCDmagnethigh [current]13. Climate action[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]LHeCPhysics::Accelerator PhysicsJET CROSS-SECTIONSHigh Energy Physics::Experimentcurrent: highJournal of Physics G: Nuclear and Particle Physics
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Zespół przerostu bakteryjnego jelita cienkiego

2021

Zespół przerostu bakteryjnego jelita cienkiego (SIBO) jest heterogennym zespołem charakteryzującym się wzrostem liczby i/lub obecnością nietypowych bakterii w jelicie cienkim. Na złożoną etiologię SIBO składają się zaburzenia ochronnych mechanizmów przeciwbakteryjnych jak zmniejszona kwaśność soku żołądkowego, zewnątrzwydzielnicza niewydolność trzustki, zespoły niedoboru odporności oraz nieprawidłowości anatomiczne jak niedrożność jelita cienkiego, uchyłki, przetoki, hirurgiczna ślepa pętla, wcześniejsze resekcje krętniczo-kątnicze oraz zaburzenia ruchliwości. Objawy kliniczne SIBO mogą być niespecyficzne. Najczęściej występuje niestrawność, biegunka, wzdęcia, dyskomfort w jamie brzusznej. …

mikrobiotaSIBOIBSmicrobiotazespół przerostu bakteryjnego jelita cienkiegohydrogen breath testssmall intestine bacterial overgrowthwodorowe testy oddechowePostępy Mikrobiologii
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Properties of zeros of solutions to third order nonlinear differential equations

2013

We investigate the behavior of zeros of solutions to the certain type of third order nonlinear differential equations. We show that the behavior of zeros may be rather different and depend on the nature of nonlinearity in the equation. Main results in the paper are illustrated with a number of examples.

zeros of solutionsThird order nonlinearDifferential equationMathematical analysisdependence of zeros on initial dataType (model theory)third order nonlinear differential equationsNonlinear systemModeling and SimulationQA1-939super-linearityAnalysisMathematicssub-linearityMathematicsMathematical Modelling and Analysis
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