Search results for "Crete"

showing 10 items of 2495 documents

Do T asymmetries for neutrino oscillations in uniform matter have a CP-even component?

2019

Observables of neutrino oscillations in matter have, in general, contributions from the effective matter potential. It contaminates the CP violation asymmetry adding a fake effect that has been recently disentangled from the genuine one by their different behavior under T and CPT. Is the genuine T-odd CPT-invariant component of the CP asymmetry coincident with the T asymmetry? Contrary to CP, matter effects in uniform matter cannot induce by themselves a non-vanishing T asymmetry; however, the question of the title remained open. We demonstrate that, in the presence of genuine CP violation, there is a new non-vanishing CP-even, and so CPT-odd, component in the T asymmetry in matter, which i…

Nuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFOS: Physical sciencesDiscrete Symmetries01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityBeta (velocity)010306 general physicsNeutrino oscillationMixing (physics)media_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyObservableHigh Energy Physics - PhenomenologyCP violationlcsh:QC770-798CP violationHigh Energy Physics::ExperimentNeutrinoEnergy (signal processing)Journal of High Energy Physics
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Signatures of the genuine and matter-induced components of the CP violation asymmetry in neutrino oscillations

2018

CP asymmetries for neutrino oscillations in matter can be disentangled into the matter-induced CPT-odd (T-invariant) component and the genuine T-odd (CPT-invariant) component. For their understanding in terms of the relevant ingredients, we develop a new perturbative expansion in both $\Delta m^2_{21},\, |a| \ll |\Delta m^2_{31}|$ without any assumptions between $\Delta m^2_{21}$ and $a$, and study the subtleties of the vacuum limit in the two terms of the CP asymmetry, moving from the CPT-invariant vacuum limit $a \to 0$ to the T-invariant limit $\Delta m^2_{21} \to 0$. In the experimental region of terrestrial accelerator neutrinos, we calculate their approximate expressions from which we…

Nuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectPhase (waves)FOS: Physical sciencesDiscrete Symmetries01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityLimit (mathematics)010306 general physicsNeutrino oscillationmedia_commonPhysics010308 nuclear & particles physicsOscillationHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyCP violationCP violationlcsh:QC770-798High Energy Physics::ExperimentNeutrinoLepton
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Correcting for Potential Barriers in Quantum Walk Search

2015

A randomly walking quantum particle searches in Grover's $\Theta(\sqrt{N})$ iterations for a marked vertex on the complete graph of $N$ vertices by repeatedly querying an oracle that flips the amplitude at the marked vertex, scattering by a "coin" flip, and hopping. Physically, however, potential energy barriers can hinder the hop and cause the search to fail, even when the amplitude of not hopping decreases with $N$. We correct for these errors by interpreting the quantum walk search as an amplitude amplification algorithm and modifying the phases applied by the coin flip and oracle such that the amplification recovers the $\Theta(\sqrt{N})$ runtime.

Nuclear and High Energy PhysicsQuantum PhysicsTheoryofComputation_COMPUTATIONBYABSTRACTDEVICESComplete graphGeneral Physics and AstronomyFOS: Physical sciencesTheoryofComputation_GENERALStatistical and Nonlinear PhysicsOracleTheoretical Computer ScienceVertex (geometry)CombinatoricsAmplitudeComputational Theory and MathematicsAmplitude amplificationTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYGrover's algorithmQuantum algorithmQuantum walkQuantum Physics (quant-ph)Mathematical PhysicsMathematicsMathematicsofComputing_DISCRETEMATHEMATICS
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Measurement of the b hadron lifetime with the dipole method

1993

A measurement of the average lifetime of b hadrons has been performed with the dipole method on a sample of 260000 hadronic Z decays recorded with the ALEPH detector during 1991. The dipole is the distance between the vertices built in the opposite hemispheres. The mean dipole is extracted from all the events without attempting b enrichment. Comparing the average of the data dipole distribution with a Monte Carlo calibration curve obtained with different b lifetimes, an average b hadron lifetime of 1.51 +/- 0.08 ps is extracted. RI ANTONELLI, ANTONELLA/C-6238-2011; Buttar, Craig/D-3706-2011; Stahl, Achim/E-8846-2011; Passalacqua, Luca/F-5127-2011; Murtas, Fabrizio/B-5729-2012; St.Denis, Ric…

Nuclear and High Energy Physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]Calibration curveElectron–positron annihilationMonte Carlo methodHadronElementary particleDiscrete dipole approximation01 natural sciencesinformationNuclear physicsALEPH Experiment0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]mutualisation.010306 general physicsALEPH experimentPhysics010308 nuclear & particles physicsPhysicsmediologyterritoryDipoleHigh Energy Physics::Experimentterritorial intelligenceParticle Physics - Experiment
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Two-step nilpotent Leibniz algebras

2022

In this paper we give a complete classification of two-step nilpotent Leibniz algebras in terms of Kronecker modules associated with pairs of bilinear forms. In particular, we describe the complex and the real case of the indecomposable Heisenberg Leibniz algebras as a generalization of the classical $(2n+1)-$dimensional Heisenberg Lie algebra $\mathfrak{h}_{2n+1}$. Then we use the Leibniz algebras - Lie local racks correspondence proposed by S. Covez to show that nilpotent real Leibniz algebras have always a global integration. As an application, we integrate the indecomposable nilpotent real Leibniz algebras with one-dimensional commutator ideal. We also show that every Lie quandle integr…

Numerical AnalysisAlgebra and Number Theory17A32 22A30 20M99Mathematics::History and OverviewMathematics::Rings and AlgebrasMathematics - Rings and AlgebrasSettore MAT/02 - AlgebraRings and Algebras (math.RA)Coquegigrue problemFOS: MathematicsDiscrete Mathematics and CombinatoricsNilpotent Leibniz algebrasGeometry and TopologySettore MAT/03 - GeometriaLeibniz algebrasLie racks
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On the condition number of the antireflective transform

2010

Abstract Deconvolution problems with a finite observation window require appropriate models of the unknown signal in order to guarantee uniqueness of the solution. For this purpose it has recently been suggested to impose some kind of antireflectivity of the signal. With this constraint, the deconvolution problem can be solved with an appropriate modification of the fast sine transform, provided that the convolution kernel is symmetric. The corresponding transformation is called the antireflective transform. In this work we determine the condition number of the antireflective transform to first order, and use this to show that the so-called reblurring variant of Tikhonov regularization for …

Numerical AnalysisAlgebra and Number TheoryBoundary conditionsTikhonov regularizationMathematical analysisDeconvolutionUpper and lower boundsRegularization (mathematics)ConvolutionTikhonov regularizationTransformation (function)Discrete Mathematics and CombinatoricsApplied mathematicsFast sine transformGeometry and TopologyUniquenessDeconvolutionCondition numberAntireflective transformMathematicsLinear Algebra and its Applications
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Explicit solutions for second-order operator differential equations with two boundary-value conditions. II

1992

AbstractBoundary-value problems for second-order operator differential equations with two boundary-value conditions are studied for the case where the companion operator is similar to a block-diagonal operator. This case is strictly more general than the one treated in an earlier paper, and it provides explicit closed-form solutions of boundary-value problem in terms of data without increasing the dimension of the problem.

Numerical AnalysisAlgebra and Number TheoryMathematical analysisSemi-elliptic operatorp-LaplacianOrder operatorDiscrete Mathematics and CombinatoricsBoundary value problemGeometry and TopologyC0-semigroupDifferential algebraic geometryTrace operatorNumerical partial differential equationsMathematicsLinear Algebra and its Applications
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Matrices A such that A^{s+1}R = RA* with R^k = I

2018

[EN] We study matrices A is an element of C-n x n such that A(s+1)R = RA* where R-k = I-n, and s, k are nonnegative integers with k >= 2; such matrices are called {R, s+1, k, *}-potent matrices. The s = 0 case corresponds to matrices such that A = RA* R-1 with R-k = I-n, and is studied using spectral properties of the matrix R. For s >= 1, various characterizations of the class of {R, s + 1, k, *}-potent matrices and relationships between these matrices and other classes of matrices are presented. (C) 2018 Elsevier Inc. All rights reserved.

Numerical AnalysisClass (set theory)Algebra and Number TheorySpectral properties0211 other engineering and technologies021107 urban & regional planning010103 numerical & computational mathematics02 engineering and technologyMatrius (Matemàtica)01 natural sciencesCombinatoricsMatrix (mathematics)Discrete Mathematics and CombinatoricsGeometry and Topology0101 mathematicsÀlgebra linealMATEMATICA APLICADA{R s+1 k *}-potent matrixK-involutoryMathematics
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Step-by-step integration for fractional operators

2018

Abstract In this paper, an approach based on the definition of the Riemann–Liouville fractional operators is proposed in order to provide a different discretisation technique as alternative to the Grunwald–Letnikov operators. The proposed Riemann–Liouville discretisation consists of performing step-by-step integration based upon the discretisation of the function f(t). It has been shown that, as f(t) is discretised as stepwise or piecewise function, the Riemann–Liouville fractional integral and derivative are governing by operators very similar to the Grunwald–Letnikov operators. In order to show the accuracy and capabilities of the proposed Riemann–Liouville discretisation technique and th…

Numerical AnalysisDiscretizationApplied Mathematics02 engineering and technologyFunction (mathematics)DerivativeWhite noise01 natural sciences010305 fluids & plasmasExponential functionFractional calculus020303 mechanical engineering & transports0203 mechanical engineeringModeling and SimulationStep function0103 physical sciencesPiecewiseApplied mathematicsFractional Calculus Riemman–Liouville Grünwald–Letnikov Discrete fractional operatorsMathematics
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Multialternating Jordan polynomials and codimension growth of matrix algebras

2007

Abstract Let R be the Jordan algebra of k  ×  k matrices over a field of characteristic zero. We exhibit a noncommutative Jordan polynomial f multialternating on disjoint sets of variables of order k 2 and we prove that f is not a polynomial identity of R . We then study the growth of the polynomial identities of the Jordan algebra R through an analysis of its sequence of Jordan codimensions. By exploiting the basic properties of the polynomial f , we are able to prove that the exponential rate of growth of the sequence of Jordan codimensions of R in precisely k 2 .

Numerical AnalysisJordan matrixPolynomialPure mathematicsAlgebra and Number TheoryJordan algebraMathematics::Rings and AlgebrasJordan algebraZero (complex analysis)Polynomial identityExponential growthNoncommutative geometryCodimensionsMatrix polynomialsymbols.namesakeMatrix (mathematics)symbolsDiscrete Mathematics and CombinatoricsGeometry and TopologyMathematicsCharacteristic polynomial
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