Search results for "Matrix"

showing 10 items of 3205 documents

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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Correlation of pp data with predictions of improved six-quark structure models.

1987

Recent experimental data indicate a structure in \ensuremath{\Delta}${\ensuremath{\sigma}}_{L}$ corresponding to a pp mass of 2.7 GeV/${c}^{2}$, as earlier predicted for a six-quark $^{1}\mathrm{S}_{0}$ state by an R-matrix treatment of the cloudy-bag-model quark degrees of freedom interior to a coupled-isobar-channel system. The $^{1}\mathrm{S}_{0}$ model is improved to agree with 2\ensuremath{\pi} production data at 800 MeV laboratory energy. The resulting $^{1}\mathrm{S}_{0}$ partial wave and recently improved models of the background partial waves as well as older versions of the phase parameters predict experimental observables in the resonance region. The predicted width and inelastic…

Quantum chromodynamicsPhysicsQuarkParticle physicsQuark modelFísicaProduction (computer science)Inelastic scatteringWave functionEnergy (signal processing)R-matrixPhysical review. D, Particles and fields
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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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Semileptonic B ->pi decays from an Omnes improved nonrelativistic constituent quark model

2005

The semileptonic $B\to \pi l^+ \nu_l$ decay is studied starting from a simple quark model which includes the influence of the $B^*$ pole. To extend the predictions of a nonrelativistic constituent quark model from its region of applicability near $q^2_{\rm max}=(m_B-m_\pi)^2$ to all $q^2$ values accessible in the physical decay, we use a novel multiply-subtracted Omn\`es dispersion relation, which considerably diminishes the form factor dependence on the elastic $\pi B \to \pi B$ scattering amplitudes at high energies. By comparison to the experimental branching fraction we extract $|V_{ub}| = 0.0034 \pm 0.0003 ({\rm exp}) \pm 0.0007 ({\rm theory})$. To further test our framework, we also s…

Quantum chromodynamicsSemileptonic decayPhysicsNuclear and High Energy PhysicsParticle physicsBranching fractionCabibbo–Kobayashi–Maskawa matrixQuark modelConstituent quarkFísicaLattice QCDCrystallographyHigh Energy Physics - PhenomenologyB meson
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Non-Markovianity of Gaussian Channels

2015

We introduce a necessary and sufficient criterion for the non-Markovianity of Gaussian quantum dynamical maps based on the violation of divisibility. The criterion is derived by defining a general vectorial representation of the covariance matrix which is then exploited to determine the condition for the complete positivity of partial maps associated to arbitrary time intervals. Such construction does not rely on the Choi-Jamiolkowski representation and does not require optimization over states.

Quantum decoherenceGaussianFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciences010305 fluids & plasmasGaussian random fieldsymbols.namesakeQuantum mechanics0103 physical sciencesGaussian functionApplied mathematics010306 general physicsRepresentation (mathematics)Mathematical PhysicsQCQuantum PhysicsCovariance matrixMathematical Physics (math-ph)Divisibility rule16. Peace & justiceGaussian filterCondensed Matter - Other Condensed MattersymbolsQuantum Physics (quant-ph)Other Condensed Matter (cond-mat.other)Physical Review Letters
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Incommensurate phases of a bosonic two-leg ladder under a flux

2016

A boson two--leg ladder in the presence of a synthetic magnetic flux is investigated by means of bosonization techniques and Density Matrix Renormalization Group (DMRG). We follow the quantum phase transition from the commensurate Meissner to the incommensurate vortex phase with increasing flux at different fillings. When the applied flux is $\rho \pi$ and close to it, where $\rho$ is the filling per rung, we find a second incommensuration in the vortex state that affects physical observables such as the momentum distribution, the rung-rung correlation function and the spin-spin and charge-charge static structure factors.

Quantum phase transitionBosonizationBosonisation[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]IncommensurationsFOS: Physical sciencesGeneral Physics and Astronomychamps de jauge artificiels01 natural sciences010305 fluids & plasmasPhysics and Astronomy (all)Condensed Matter - Strongly Correlated ElectronsCorrelation functionGauge fieldsCondensed Matter::Superconductivity0103 physical sciencesBosonizationtranstion commensurable-incommensurable010306 general physicsCommensurate-Incommensurate transitions[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsartificial gauge fieldsDensity matrix renormalization groupGauge fields; Incommensurations; Meissner to vortex transition; Physics and Astronomy (all)Vortex stateMagnetic fluxVortexQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality.Quantum Gases (cond-mat.quant-gas)Meissner to vortex transitionCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum GasesQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality
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Nonequilibrium critical scaling in quantum thermodynamics

2016

The emerging field of quantum thermodynamics is contributing important results and insights into archetypal many-body problems, including quantum phase transitions. Still, the question whether out-of-equilibrium quantities, such as fluctuations of work, exhibit critical scaling after a sudden quench in a closed system has remained elusive. Here, we take a novel approach to the problem by studying a quench across an impurity quantum critical point. By performing density matrix renormalization group computations on the two-impurity Kondo model, we are able to establish that the irreversible work produced in a quench exhibits finite-size scaling at quantum criticality. This scaling faithfully …

Quantum phase transitionFOS: Physical sciencesNon-equilibrium thermodynamics02 engineering and technology01 natural sciencesCondensed Matter - Strongly Correlated Electronsquant-phCritical point (thermodynamics)Quantum critical pointQuantum mechanics0103 physical sciencesStatistical physicscond-mat.stat-mech010306 general physicsQuantum thermodynamicsCondensed Matter - Statistical MechanicsPhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)Strongly Correlated Electrons (cond-mat.str-el)Density matrix renormalization group021001 nanoscience & nanotechnology2-IMPURITY KONDO PROBLEM; MATRIX RENORMALIZATION-GROUP; JARZYNSKI EQUALITY; CRITICAL-POINT; SYSTEMS; MODELcond-mat.str-elQuantum Physics (quant-ph)0210 nano-technologyKondo modelCritical exponentPhysical Review B
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Quantum Lower Bound for Graph Collision Implies Lower Bound for Triangle Detection

2015

We show that an improvement to the best known quantum lower bound for GRAPH-COLLISION problem implies an improvement to the best known lower bound for TRIANGLE problem in the quantum query complexity model. In GRAPH-COLLISION we are given free access to a graph $(V,E)$ and access to a function $f:V\rightarrow \{0,1\}$ as a black box. We are asked to determine if there exist $(u,v) \in E$, such that $f(u)=f(v)=1$. In TRIANGLE we have a black box access to an adjacency matrix of a graph and we have to determine if the graph contains a triangle. For both of these problems the known lower bounds are trivial ($\Omega(\sqrt{n})$ and $\Omega(n)$, respectively) and there is no known matching upper …

Quantum queryQuantum PhysicsGeneral Computer ScienceFree accessTheoryofComputation_GENERALCollisionUpper and lower boundsOmegaGraphCombinatoricsComputer Science - Computational ComplexityAdjacency matrixQuantumMathematicsMathematicsofComputing_DISCRETEMATHEMATICS
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The triple collinear limit of one-loop QCD amplitudes

2003

We consider the singular behaviour of one-loop QCD matrix elements when several external partons become simultaneously parallel. We present a new factorization formula that describes the singular collinear behaviour directly in colour space. The collinear singularities are embodied in process-independent splitting matrices that depend on the momenta, flavours, spins and colours of the collinear partons. We give the general structure of the infrared and ultraviolet divergences of the one-loop splitting matrices. We also present explicit one-loop results for the triple collinear splitting, $q \to q {\bar Q} Q$, of a quark and a quark--antiquark pair of different flavours. The one-loop triple …

QuarkNuclear and High Energy PhysicsParticle physicsCiencias FísicasHigh Energy Physics::LatticeFOS: Physical sciencesPartonSpace (mathematics)//purl.org/becyt/ford/1 [https]Matrix (mathematics)High Energy Physics - Phenomenology (hep-ph)FactorizationAmplitudesParticle Physics - PhenomenologyQuantum chromodynamicsPhysicsTripleHigh Energy Physics::PhenomenologyFísica//purl.org/becyt/ford/1.3 [https]QcdAstronomíaHigh Energy Physics - PhenomenologyGravitational singularityHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)CollinearCIENCIAS NATURALES Y EXACTAS
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Scalar K pi form factor and light quark masses

2006

5 páginas, 2 figuras, 2 tablas.-- PACS numbers: 12.15.Ff, 14.65.Bt, 11.55.Hx.-- arXiv:hep-ph/0605095v2

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeScalar (mathematics)Nuclear TheoryFOS: Physical sciencesStrangenessAstrophysicsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Particle decayHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics - LatticeInvariant massNuclear ExperimentQuantum chromodynamicsPhysicsCabibbo–Kobayashi–Maskawa matrixAstrophysics (astro-ph)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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