Search results for " Matrix"

showing 10 items of 2053 documents

Lévy flights in an infinite potential well as a hypersingular Fredholm problem.

2016

We study L\'evy flights {{with arbitrary index $0< \mu \leq 2$}} inside a potential well of infinite depth. Such problem appears in many physical systems ranging from stochastic interfaces to fracture dynamics and multifractality in disordered quantum systems. The major technical tool is a transformation of the eigenvalue problem for initial fractional Schr\"odinger equation into that for Fredholm integral equation with hypersingular kernel. The latter equation is then solved by means of expansion over the complete set of orthogonal functions in the domain $D$, reducing the problem to the spectrum of a matrix of infinite dimensions. The eigenvalues and eigenfunctions are then obtained numer…

Quantum PhysicsMathematical analysisSpectrum (functional analysis)Orthogonal functionsFredholm integral equationEigenfunctionParticle in a boxMathematics::Spectral Theory01 natural sciences010305 fluids & plasmasSchrödinger equationMathematics - Spectral Theorysymbols.namesakeSpectrum of a matrix0103 physical sciencessymbols010306 general physicsEigenvalues and eigenvectorsCondensed Matter - Statistical MechanicsMathematical PhysicsMathematics - ProbabilityMathematicsPhysical review. E
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Recovering Quantum Properties of Continuous-Variable States in the Presence of Measurement Errors.

2016

We present two results which combined enable one to reliably detect multimode, multipartite entanglement in the presence of measurement errors. The first result leads to a method to compute the best (approximated) physical covariance matrix given a measured non-physical one. The other result states that a widely used entanglement condition is a consequence of negativity of partial transposition. Our approach can quickly verify entanglement of experimentally obtained multipartite states, which is demonstrated on several realistic examples. Compared to existing detection schemes, ours is very simple and efficient. In particular, it does not require any complicated optimizations.

Quantum PhysicsObservational errorComputer scienceCovariance matrixFOS: Physical sciencesGeneral Physics and AstronomyQuantum PhysicsQuantum entanglement01 natural sciencesMultipartite entanglementStandard deviation010305 fluids & plasmasMultipartiteSimple (abstract algebra)0103 physical sciencesStatistical physicsQuantum Physics (quant-ph)010306 general physicsQuantumPhysical review letters
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Determination of the form factors for the decayB0→D*−l+νland of the CKM matrix element|Vcb|

2008

We present a combined measurement of the Cabibbo-Kobayashi-Maskawa matrix element vertical bar V-cb vertical bar and of the parameters rho(2), R-1(1), and R-2(1), which fully characterize the form factors for the B-0 -> D*(-)center dot(+)nu(center dot) decay in the framework of heavy-quark effective field theory. The results, based on a selected sample of about 52 800 B-0 -> D*(-)center dot(+)nu(center dot) decays, recorded by the BABAR detector, are rho(2)=1.157 +/- 0.094 +/- 0.027, R-1(1)=1.327 +/- 0.131 +/- 0.043, R-2(1)=0.859 +/- 0.077 +/- 0.021, and F(1)vertical bar V-cb vertical bar=(34.7 +/- 0.4 +/- 1.0)x10(-3). The first error is the statistical and the second is the systematic unce…

Quantum chromodynamicsPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsBranching fractionCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationLattice field theoryAnalytical chemistry01 natural sciencesParticle identificationParticle decayLattice (order)0103 physical sciences010306 general physicsPhysical Review D
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Mass Hierarchy, Mixing, CP-Violation and Higgs Decay---or Why Rotation is Good for Us

2011

The idea of a rank-one rotating mass matrix (R2M2) is reviewed detailing how it leads to ready explanations both for the fermion mass hierarchy and for the distinctive mixing patterns between up and down fermion states, which can be and have been tested against experiment and shown to be fully consistent with existing data. Further, R2M2 is seen to offer, as by-products: (i) a new solution of the strong CP problem in QCD by linking the theta-angle there to the Kobayashi-Maskawa CP-violating phase in the CKM matrix, and (ii) some novel predictions of possible anomalies in Higgs decay observable in principle at the LHC. A special effort is made to answer some questions raised.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsObservableMass matrixAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonCP violationStrong CP problemHigh Energy Physics::ExperimentMixing (physics)
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Comprehensive measurements oft-channel single top-quark production cross sections ats=7  TeVwith the ATLAS detector

2014

This article presents measurements of the t-channel single top-quark ((t) over bart) and top-antiquark (_ t) total production cross sections sdtq_ and sd _ tq_, their ratio Rt sdtq_= sd _ tq_, and a measurement of the inclusive production cross section sdtq _ _ tq_ in proton-proton collisions at ffiffiffi ps = 7 TeV at the LHC. Differential cross sections for the tq and _ tq processes are measured as a function of the transverse momentum and the absolute value of the rapidity of t and _ t, respectively. The analyzed data set was recorded with the ATLAS detector and corresponds to an integrated luminosity of 4.59 fb-1. Selected events contain one charged lepton, large missing transverse mome…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrix01 natural sciencesStandard ModelNuclear physicsmedicine.anatomical_structurePair productionAtlas (anatomy)0103 physical sciencesmedicineRapidity010306 general physicsLeptonPhysical Review D
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Kaon Decays in the Standard Model

2011

A comprehensive overview of kaon decays is presented. The Standard Model predictions are discussed in detail, covering both the underlying short-distance electroweak dynamics and the important interplay of QCD at long distances. Chiral perturbation theory provides a universal framework for treating leptonic, semileptonic and nonleptonic decays including rare and radiative modes. All allowed decay modes with branching ratios of at least 10^(-11) are analyzed. Some decays with even smaller rates are also included. Decays that are strictly forbidden in the Standard Model are not considered in this review. The present experimental status and the prospects for future improvements are reviewed.

Quantum chromodynamicsPhysicsParticle physicsChiral perturbation theoryCabibbo–Kobayashi–Maskawa matrixElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyFísicaHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferBibliographyCP violationHigh Energy Physics::Experiment
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Extraction of heavy-quark-expansion parameters from unquenched lattice data on pseudoscalar and vector heavy-light meson masses

2017

We present a precise lattice computation of pseudoscalar and vector heavy-light meson masses for heavy-quark masses ranging from the physical charm mass up to $\ensuremath{\simeq}4$ times the physical $b$-quark mass. We employ the gauge configurations generated by the European Twisted Mass Collaboration (ETMC) with ${N}_{f}=2+1+1$ dynamical quarks at three values of the lattice spacing ($a\ensuremath{\simeq}0.062,0.082,0.089\text{ }\text{ }\mathrm{fm}$) with pion masses in the range ${M}_{\ensuremath{\pi}}\ensuremath{\simeq}210--450\text{ }\text{ }\mathrm{MeV}$. The heavy-quark mass is simulated directly on the lattice up to $\ensuremath{\simeq}3$ times the physical charm mass. The interpol…

Quantum chromodynamicsPhysicsParticle physicsHigh Energy Physics - Lattice; High Energy Physics - Lattice; High Energy Physics - Phenomenology; Physics and Astronomy (miscellaneous)MesonPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theory01 natural sciencesPseudoscalarHigh Energy Physics - PhenomenologyPionLattice constantHigh Energy Physics - LatticeLattice (order)0103 physical sciencesHigh Energy Physics::Experiment010306 general physics
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Determination of the Pseudoscalar Decay Constant fDs+ via Ds+→μ+νμ

2019

Using a 3.19  fb^{-1} data sample collected at an e^{+}e^{-} center-of-mass energy of E_{cm}=4.178  GeV with the BESIII detector, we measure the branching fraction of the leptonic decay D_{s}^{+}→μ^{+}ν_{μ} to be B_{D_{s}^{+}→μ^{+}ν_{μ}}=(5.49±0.16_{stat}±0.15_{syst})×10^{-3}. Combining our branching fraction with the masses of the D_{s}^{+} and μ^{+} and the lifetime of the D_{s}^{+}, we determine f_{D_{s}^{+}}|V_{cs}|=246.2±3.6_{stat}±3.5_{syst}  MeV. Using the c→s quark mixing matrix element |V_{cs}| determined from a global standard model fit, we evaluate the D_{s}^{+} decay constant f_{D_{s}^{+}}=252.9±3.7_{stat}±3.6_{syst}  MeV. Alternatively, using the value of f_{D_{s}^{+}} calculat…

Quantum chromodynamicsPhysicsPseudoscalarCrystallographyBranching fractionCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationLattice (order)0103 physical sciencesGeneral Physics and AstronomyExponential decay010306 general physics01 natural sciencesPhysical Review Letters
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A Comprehensive Mechanism Reproducing the Mass and Mixing Parameters of Quarks and Leptons

2013

It is shown that if, from the starting point of a universal rank-one mass matrix long favored by phenomenologists, one adds the assumption that it rotates (changes its orientation in generation space) with changing scale, one can reproduce, in terms of only six real parameters, all the 16 mass ratios and mixing parameters of quarks and leptons. Of these 16 quantities so reproduced, 10 for which data exist for direct comparison (i.e. the CKM elements including the CP-violating phase, the angles theta(12), theta(13), theta(23) in nu-oscillation, and the masses m(c), m(mu), m(e)) agree well with experiment, mostly to within experimental errors; four others (m(s), m(u), m(d), m(nu 2)), the expe…

Quantum chromodynamicsPhysicsQuarkNuclear and High Energy PhysicsParticle physicsPMNS matrixCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesOrder (ring theory)Astronomy and AstrophysicsMass matrixAtomic and Molecular Physics and OpticsOrientation (vector space)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CKM matrixFermion massesHigh Energy Physics::ExperimentCP phaseNeutrinoLepton
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Developing the Framed Standard Model

2011

The framed standard model (FSM) suggested earlier, which incorporates the Higgs field and 3 fermion generations as part of the framed gauge theory structure, is here developed further to show that it gives both quarks and leptons hierarchical masses and mixing matrices akin to what is experimentally observed. Among its many distinguishing features which lead to the above results are (i) the vacuum is degenerate under a global $su(3)$ symmetry which plays the role of fermion generations, (ii) the fermion mass matrix is "universal", rank-one and rotates (changes its orientation in generation space) with changing scale $\mu$, (iii) the metric in generation space is scale-dependent too, and in …

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsFermionAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)Higgs fieldTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Strong CP problemHigh Energy Physics::ExperimentGauge theory
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