Search results for "Amplitude"

showing 10 items of 1169 documents

Measurement of the spin of the Xi(1530) resonance

2008

The properties of the Xi(1530) resonance are investigated in the Lambdac+ --> Xi- pi+ K+ decay process. The data sample was collected with the BaBar detector at the SLAC PEP-II asymmetric-energy e+ e- collider operating at center of mass energies 10.58 and 10.54 GeV. The corresponding integrated luminosity is approximately 230 inverse fb. The spin of the Xi(1530) is established to be 3/2. The existence of an S-wave amplitude in the Xi- pi+ system is inferred, and its interference with the Xi(1530)0 amplitude provides the first clear demonstration of the Breit-Wigner phase motion expected for the Xi(1530). The P_1(cos[theta(Xi-)]) Legendre polynomial moment indicates the presence of a sig…

Nuclear and High Energy PhysicsBABARElectron–positron annihilationFOS: Physical sciencesDalitz plotMASSPARTICLE PHYSICS; PEP2; BABAR01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciencesPEP2MASS; PARITY; WIDTH[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsPhysicsPARITY010308 nuclear & particles physicsHyperonWIDTHResonanceBABAR detectorHEPCharmed baryonsAmplitudeBaBarPARTICLE PHYSICSCenter of massFísica de partículesExperiments
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Measurement of the radiative K-e3 branching ratio

2005

We present a measurement of the relative branching ratio of the decay KL -> pi e nu gamma (Ke3gamma) with respect to KL-> pi e nu (gamma) (Ke3+Ke3gamma) decay. The result is based on observation of 19 000 Ke3gamma and 5.6 x 10^6 Ke3 decays. The value of the branching ratio is Br(Ke3gamma, Egamma^*>30 MeV,theta(e,gamma)^*>20^o)/Br(Ke3)= (0.964+-0.008+0.011-0.009)%. This result agrees with theoretical predictions but is at variance with a recently published result.

Nuclear and High Energy PhysicsChiral perturbation theoryPhotonHadronFOS: Physical scienceskaon decay; NEUTRAL KAON; branching ratio7. Clean energy01 natural sciencesNEUTRAL KAONHigh Energy Physics - ExperimentNuclear physicsmesoni KHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesRadiative transfer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]radiative kaon decays010306 general physicsmesoni K; decadimenti radiativiPhysics010308 nuclear & particles physicsBranching fractionK13 DECAYSBremsstrahlungkaon decayAmplitudedecadimenti radiativibranching ratioAtomic physicsParticle Physics - Experiment
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Quantum algorithms for search with wildcards and combinatorial group testing

2012

We consider two combinatorial problems. The first we call "search with wildcards": given an unknown n-bit string x, and the ability to check whether any subset of the bits of x is equal to a provided query string, the goal is to output x. We give a nearly optimal O(sqrt(n) log n) quantum query algorithm for search with wildcards, beating the classical lower bound of Omega(n) queries. Rather than using amplitude amplification or a quantum walk, our algorithm is ultimately based on the solution to a state discrimination problem. The second problem we consider is combinatorial group testing, which is the task of identifying a subset of at most k special items out of a set of n items, given the…

Nuclear and High Energy PhysicsFOS: Physical sciencesGeneral Physics and Astronomy0102 computer and information sciences01 natural sciencesUpper and lower boundsTheoretical Computer ScienceCombinatoricsSet (abstract data type)Amplitude amplification0103 physical sciencesQuantum walk010306 general physicsMathematical PhysicsMathematicsQuantum PhysicsQuery stringComputer Science::Information RetrievalString (computer science)Statistical and Nonlinear PhysicsWildcard charactercomputer.file_formatComputational Theory and Mathematics010201 computation theory & mathematicsQuantum algorithmQuantum Physics (quant-ph)computerQuantum Information and Computation
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Measurement of the phase between strong and electromagnetic amplitudes of J/ψ decays

2019

Kolcu, Onur Buğra (Arel Author)

Nuclear and High Energy PhysicsJ/Psi decayElectron–positron annihilationBESIII; Electromagnetic amplitude; J/ψ decay; Phase; Strong amplitude; High Energy Physics - Experiment; High Energy Physics - Experiment01 natural sciencesHigh Energy Physics - ExperimentNOSubatomär fysikSubatomic Physics0103 physical sciencesJ/ψ decayStrong amplitudeBorn approximation010306 general physicsPhysicsBESIII Electromagnetic amplitude J/ψ decay Phase Strong amplitudeAnnihilation010308 nuclear & particles physicsBranching fractionBESIIIlcsh:QC1-999BESIII; Electromagnetic amplitude; J/ψ decay; Phase; Strong amplitudeAmplitudeElectromagnetic amplitudePhaseHigh Energy Physics::ExperimentRelative phaseAtomic physicsJ/Psi Decaylcsh:Physics
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Meson Resonances at large Nc: Complex Poles vs Breit-Wigner Masses

2009

The rigorous quantum mechanical definition of a resonance requires determining the pole position in the second Riemann sheet of the analytically continued partial wave scattering amplitude in the complex Mandelstam s variable plane. For meson resonances we investigate the alternative Breit–Wigner (BW) definition within the large NC expansion. By assuming that the pole position is View the MathML source and exploiting unitarity, we show that the BW determination of the resonance mass differs from the pole position by View the MathML source terms, which can be extracted from ππ scattering data. For the case of the σ (f0(600)) pole, the BW scalar mass is predicted to occur at not, vert, simila…

Nuclear and High Energy PhysicsMesonScalar (mathematics)FOS: Physical sciences01 natural sciencesUnitarizationHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciences010306 general physicsScalar mesonChiral symmetriesScalar mesonPhysicsUnitarity010308 nuclear & particles physicsPlane (geometry)ScatteringLarge N-CResonanceFísicaScattering amplitudeHigh Energy Physics - PhenomenologyResonancesQuantum electrodynamics
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Implementing the three-particle quantization condition including higher partial waves

2019

We present an implementation of the relativistic three-particle quantization condition including both $s$- and $d$-wave two-particle channels. For this, we develop a systematic expansion about threshold of the three-particle divergence-free K matrix, $\mathcal{K}_{\mathrm{df,3}}$, which is a generalization of the effective range expansion of the two-particle K matrix, $\mathcal{K}_2$. Relativistic invariance plays an important role in this expansion. We find that $d$-wave two-particle channels enter first at quadratic order. We explain how to implement the resulting multichannel quantization condition, and present several examples of its application. We derive the leading dependence of the …

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)Relativistic invarianceFOS: Physical sciencesLattice QCD01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuadratic orderScattering Amplitudes010306 general physicsNuclear theoryCondensed Matter - Statistical MechanicsK matrixMathematical physicsPhysicsLattice Quantum Field TheoryStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDScattering amplitudeHigh Energy Physics - Phenomenologylcsh:QC770-798Journal of High Energy Physics
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Generalization of the model-independent Laurent–Pietarinen single-channel pole-extraction formalism to multiple channels

2016

A method to extract resonance pole information from single-channel partial-wave amplitudes based on a Laurent (Mittag-Leffler) expansion and conformal mapping techniques has recently been developed. This method has been applied to a number of reactions and provides a model-independent extraction procedure which is particularly useful in cases where a set of amplitudes is available only at discrete energies. This method has been generalized and applied to the case of a multi-channel fit, where several sets of amplitudes are analyzed simultaneously. The importance of unitarity constraints is discussed. The final result provides a powerful, model-independent tool for analyzing partial-wave amp…

Nuclear and High Energy PhysicsNuclear TheoryPartial wave analysisFOS: Physical sciencesConformal map01 natural sciencesNuclear Theory (nucl-th)Quantum mechanics0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear theoryPhysicsModel independent extractionUnitarity010308 nuclear & particles physicsMathematical analysisPartial wave analysisPartial wave analysis ; pole parameters ; model independent extractionlcsh:QC1-999Formalism (philosophy of mathematics)Amplitudelcsh:PhysicsPole parametersCommunication channelPhysics Letters B
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A strategy to study the role of the charm quark in explaining the Delta{I}=1/2 rule

2004

We present a strategy designed to separate several possible origins of the well-known enhancement of the Delta{I}=1/2 amplitude in non-leptonic kaon decays. In particular, we seek to disentangle the contribution of physics at the typical QCD scale (soft-gluon exchange) from the effects at the scale of the charm quark mass. This is achieved by considering QCD with an unphysically light charm quark, so that the theory possesses an approximate SU(4)_L x SU(4)_R chiral symmetry. By computing the relevant operator matrix elements and monitoring their values as the charm quark mass departs from the SU(4)-symmetric situation, the role of the charm quark can be assessed. We study the influence of t…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeLattice (group)FOS: Physical sciencesScale (descriptive set theory)weak decaysCharm quarkHigh Energy Physics - Phenomenology (hep-ph)lattice QCDHigh Energy Physics - Latticefield theory gauge theory lattice kaon decayskaon physicschiral lagrangiansLimit (mathematics)Quantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyAmplitudeOperator matrixHigh Energy Physics::Experiment
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The pion transition form factor and the pion distribution amplitude

2010

Recent BaBar data on the pion transition form factor, whose Q(2)-dependence is much steeper then predicted by asymptotic Quantum Chromodynamics (QCD), have caused a renewed interest in its theoretical description. We present here a formalism based on a model-independent description for low photon virtuality and a high photon virtuality description based on QCD, which match at a scale Q(0). The high photon virtuality description incorporates a flat pion distribution amplitude, phi(x) = 1, at the matching scale Q(0) and QCD evolution from Q(0) to Q > Q(0). The flat pion distribution is connected, through soft pion theorems and chiral symmetry, to the pion valence parton distribution at the sa…

Nuclear and High Energy PhysicsParticle physicsDistribution (number theory)Scale (ratio)High Energy Physics::LatticeFOS: Physical sciencesPartonAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesPartícules (Física nuclear)PionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesTwist010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyForm factor (quantum field theory)High Energy Physics - PhenomenologyAmplitudeFísica nuclearHigh Energy Physics::Experiment
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Constraining neutrinoless double beta decay

2011

A class of discrete flavor-symmetry-based models predicts constrained neutrino mass matrix schemes that lead to specific neutrino mass sum-rules (MSR). We show how these theories may constrain the absolute scale of neutrino mass, leading in most of the cases to a lower bound on the neutrinoless double beta decay effective amplitude.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesUpper and lower boundsHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationAbsolute scaleNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaMass matrixHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics::ExperimentNeutrino
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