Search results for "Matrix"

showing 10 items of 3205 documents

Violation of matter-antimatter symmetry

2001

A small matter-antimatter asymmetry of the weak force was experimentally established. This CP violation may be related to the small excess of matter from the big bang. The nature of CP violation in the K0 system has been clarified after 35 years of experimentation: it is due to a small part of the weak interaction (“milliweak interaction”). A non-trivial phase in the weak quark mixing matrix generates “direct CP violation” in the weak Hamiltonian. The experiments demonstrating direct CP violation are discussed.

PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyWeak interactionAsymmetrysymbols.namesakeAntimattersymbolsCP violationHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)media_commonAnnalen der Physik
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Observation of direct CP violation in kaon decays

2019

A small matter-antimatter asymmetry of the weak force was experimentally established. This CP violation may be related to the small excess of matter from the big bang. The nature of CP violation in the K0 system has been clarified after 37 years of experimentation: it is due to a small part of the weak interaction (“milliweak interaction”). A non-trivial phase in the weak quark mixing matrix generates “direct CP violation” in the weak Hamiltonian. The experiments demonstrating direct CP violation are discussed.

PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyParity (physics)Cosmological modelWeak interactionAsymmetryNuclear physicssymbols.namesakeElectromagnetic calorimetersymbolsCP violationHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)media_common
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CP Violation in the K 0 System

2002

A small matter-antimatter asymmetry of the weak force was experimentally established. This CP violation may be related to the small excess of matter from the big bang. The nature of CP violation in the K 0 system has been clarified after 35 years of experimentation: it is due to a small part of the weak interaction (“illiweak interaction”). A non-trivial phase in the weak quark mixing matrix generates “direct CP violation” in the weak Hamiltonian. The experiments demonstrating direct CP violation are discussed.

PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyWeak interactionAsymmetrysymbols.namesakeElectromagnetic calorimetersymbolsCP violationHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)media_common
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Chiral unitary theory: Application to nuclear problems

2001

In this talk we briefly describe some basic elements of chiral perturbation theory, $\chi PT$, and how the implementation of unitarity and other novel elements lead to a better expansion of the $T$ matrix for meson meson and meson baryon interactions. Applications are then done to the $ \pi \pi $ interaction in nuclear matter in the scalar and vector channels, antikaons in nuclei and $K^-$ atoms, and how the $\phi$ meson properties are changed in a nuclear medium.

PhysicsParticle physicsChiral perturbation theoryNuclear TheoryMesonUnitarityHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesFísicaNuclear matterUnitary stateBaryonNuclear Theory (nucl-th)Matrix (mathematics)High Energy Physics::ExperimentNuclear Experiment
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The pionic beta decay in chiral perturbation theory

2003

Within the framework of chiral perturbation theory with virtual photons and leptons, we present an updated analysis of the pionic beta decay including all electromagnetic contributions of order e**2 p**2. We discuss the extraction of the Cabibbo-Kobayashi-Maskawa matrix element |Vud| from experimental data. The method employed here is consistent with the analogous treatment of the Kl3 decays and the determination of |Vus|.

PhysicsParticle physicsChiral perturbation theoryPhysics and Astronomy (miscellaneous)[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)Virtual particle01 natural sciencesBeta decay3. Good health[PHYS.HPHE] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesMatrix elementHigh Energy Physics::Experiment[PHYS.HTHE] Physics [physics]/High Energy Physics - Theory [hep-th]010306 general physicsEngineering (miscellaneous)Lepton
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WEAK DECAY OF Λ–HYPERNUCLEI

2005

The nonmesonic weak decay of L hypernuclei is studied in a shell model framework. A complete strangeness-changing weak LN!NN transition potential, based on one boson exchange, is constructed by including the exchange of the pseudoscalar mesons p, K, h as well as the vector mesons r,v, and K*, whose weak-coupling constants are obtained from soft meson theorems and SU~6! w . General expressions for nucleons in arbitrary shells are obtained. The transition matrix elements include realistic LN short-range correlations and NN final state interactions based on the Nijmegen baryon-baryon potential. The decay rates are found to be especially sensitive to the inclusion of the strange mesons K and K*…

PhysicsParticle physicsChiral perturbation theoryProtonMesonmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyNuclear TheoryStochastic matrixAsymmetryPseudoscalarHigh Energy Physics::ExperimentNuclear ExperimentNucleonmedia_commonBosonTheoretical Nuclear Physics in Italy
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Analysis of the nonleptonic two-body decays of the Λ hyperon

2021

We systematically study two-body nonleptonic decays of light lambda hyperon $\Lambda \to p \pi^- (n\pi^0)$ with account for both short- and long-distance effects. The short-distance effects are induced by five topologies of external and internal weak $W^\pm$ exchange, while long-distance effects are saturated by an inclusion of the so-called pole diagrams with intermediate $\frac{1}{2}^+$ and $\frac{1}{2}^-$ baryon resonances. The contributions from $\frac12^+$ resonances are calculated straightforwardly by account for nucleon and $\Sigma$ baryons whereas the contributions from $\frac{1}{2}^-$ resonances are calculated by using the well-known soft-pion theorem in the current-algebra approac…

PhysicsParticle physicsDiagramHyperonLambdaвнешний W-обменBaryonвнутренний W-обменMatrix (mathematics)Λ-гипероныHigh Energy Physics - PhenomenologyAmplitudeдвухчастичные нелептонные распадыNucleonOrder of magnitudePhysical Review
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Fascinating puzzle called double beta decay

2019

The question of whether neutrinos are Majorana or Dirac particles and what are their average masses remains one of the most fundamental problems in physics today. Observation of neutrinoless double beta decay (0νββ) would verify the Majorana nature of the neutrino and constrain the absolute scale of the neutrino mass spectrum. The inverse half-life for 0νββ-decay is given by the product of a phase space factor (PSF), a nuclear matrix element (NME), which both rely on theoretical description, and a function f containing the physics beyond the standard model. Recent calculations of PSF and NME will be reviewed together with comparison to other available results. These calculations serve the p…

PhysicsParticle physicsDirac (video compression format)Physics beyond the Standard ModelHigh Energy Physics::Phenomenologyneutriinotdouble beta decaynuclear matrix elementshiukkasfysiikkaMAJORANADouble beta decayPhase spaceMass spectrumHigh Energy Physics::ExperimentNeutrinoydinfysiikkaAbsolute scale
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Exclusive Semileptonic B and D Decays

1989

Interest in semileptonic (s.l.) bottom meson decays in the last few years has focused on the lepton energy end point spectrum. Theoretical models were needed for the description of the endpoint spectrum in order to be able to experimentally extract values for the ratio of KM matrix elements |Vbu/Vbc|. As approximately 90% of the total s.l. decay rate of bottom mesons is into the exclusive modes D and D* it was quite natural to try and model the endpoint spectrum by exclusive contributions. This approach was pioneered by GILMAN, ISGUR and WISE (GIW) in [1].

PhysicsParticle physicsEnd pointMesonCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologySpectrum (functional analysis)Theoretical modelsOrder (group theory)High Energy Physics::ExperimentLepton
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Constraints on the unitarity triangle angleγfrom Dalitz plot analysis ofB0→DK+π−decays

2016

The first study is presented of CP violation with an amplitude analysis of the Dalitz plot of B0→DK+π- decays, with D→K+π-, K+K-, and π+π-. The analysis is based on a data sample corresponding to 3.0 fb-1 of pp collisions collected with the LHCb detector. No significant CP violation effect is seen, and constraints are placed on the angle γ of the unitarity triangle formed from elements of the Cabibbo-Kobayashi-Maskawa quark mixing matrix. Hadronic parameters associated with the B0→DK∗(892)0 decay are determined for the first time. These measurements can be used to improve the sensitivity to γ of existing and future studies of the B0→DK∗(892)0 decay.

PhysicsParticle physicsFuture studiesUnitarity010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHadronDalitz plot01 natural sciencesNuclear physicsAmplitude0103 physical sciencesCP violation010306 general physicsPhysical Review D
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