Search results for "Graph theory"

showing 10 items of 784 documents

Collective subspaces for large amplitude motion and the generator coordinate method

1979

The collection path $|\ensuremath{\varphi}(q)〉$ to be used in a microscopic description of large amplitude collective motion is determined by means of the generator coordinate method. By varying the total energy with respect to $|\ensuremath{\varphi}(q)〉$ and performing an adiabatic expansion a hierarchy of equations is obtained which determines uniquely a hierarchy of collective paths with increasing complexity. To zeroth order the $|\ensuremath{\varphi}(q)〉$ are Slater determinants, to first order they include 2p-2h correlations. In both cases simple noninterative prescriptions for an explicit construction of the path are derived. For a correlated path their solutions agree at the Hartree…

PhysicsNuclear and High Energy PhysicsGenerator (category theory)Quantum mechanicsPath (graph theory)Slater determinantSemiclassical physicsPerturbation theory (quantum mechanics)Adiabatic processRandom phase approximationLinear subspaceMathematical physicsPhysical Review C
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The new FL measurement from HERA and the dipole model

2012

From the new measurement of F_L at HERA we derive fixed-Q^2 averages . We compare these with bounds which are rigorous in the framework of the standard dipole picture. The bounds are sharpened by including information on the charm structure function F_2^(c). Within the experimental errors the bounds are respected by the data. But for 3.5 GeV^2 <= Q^2 <= 20 GeV^2 the central values of the data are close to and in some cases even above the bounds. Data on F_L/F_2 significantly exceeding the bounds would rule out the standard dipole picture at these kinematic points. We discuss, furthermore, how data respecting the bounds but coming close to them can give information on questions like colour t…

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::PhenomenologyStructure functionFOS: Physical sciencesHERADipole modelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyCross section (physics)DipoleTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Saturation (graph theory)High Energy Physics::ExperimentCharm (quantum number)Physics Letters B
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Two-Loop Vertices in Quantum Field Theory: Infrared Convergent Scalar Configurations

2003

A comprehensive study is performed of general massive, scalar, two-loop Feynman diagrams with three external legs. Algorithms for their numerical evaluation are introduced and discussed, numerical results are shown for all different topologies, and comparisons with analytical results, whenever available, are performed. An internal cross-check, based on alternative procedures, is also applied. The analysis of infrared divergent configurations, as well as the treatment of tensor integrals, will be discussed in two forthcoming papers.

PhysicsNuclear and High Energy PhysicsLoop (graph theory)Wave function renormalizationScalar (physics)Vertex functionFOS: Physical sciencesTheoretical physicssymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsBibliographysymbolsFeynman diagramTensorQuantum field theory
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Neutrino mean free path and in-medium nuclear interaction

2002

Neutrinos produced during the collapse of a massive star are trapped in a nuclear medium (the proto-neutron star). Typically, neutrino energies (10-100 MeV) are of the order of nuclear giant resonances energies. Hence, neutrino propagation is modified by the possibility of coherent scattering on nucleons. We have compared the predictions of different nuclear interaction models. It turns out that their main discrepancies are related to the density dependence of the k-effective mass as well as to the onset of instabilities as density increases. This last point had led us to a systematic study of instabilities of infinite matter with effective Skyrme-type interactions. We have shown that for s…

PhysicsNuclear and High Energy PhysicsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsMean free pathScatteringNuclear TheoryFísicaFOS: Physical sciencesStar (graph theory)01 natural sciences7. Clean energyNuclear interactionNuclear physicsNuclear Theory (nucl-th)0103 physical sciencesNeutrino010306 general physicsNucleonNuclear Experiment
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An A4 model for lepton masses and mixings

2009

We study an extension of the standard model based on the flavor symmetry A(4) only. Neutrino Majorana mass terms arise from a dimension five operator and charged lepton masses from renormalizable Yukawa couplings. We introduce three Higgs doublets that belong to one triplet irreducible representation of A(4). We study the most general A(4)-invariant scalar potential and the phenomenological consequences of the model. We find that the reactor angle could be as large as sin(2)theta(13max)similar to 0.03, while the atmospheric mixing angle theta(23) is close to maximal, sin(2)theta(23)=1/2.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDimension (graph theory)High Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesWeinberg angle7. Clean energy01 natural sciencesStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Irreducible representation0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsNeutrino oscillationParticle Physics - PhenomenologyLepton
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New Physics and Evidence for a Complex CKM

2005

We carefully analyse the present experimental evidence for a complex CKM matrix, even allowing for New Physics contributions to $\epsilon_{K}$, $a_{J/\Psi K_S}$, $\Delta M_{B_{d}}$, $\Delta M_{B_{s}}$, and the $\Delta I=1/2$ piece of $B\to\rho\rho$ and $B\to\rho\pi$. We emphasize the crucial r\^ ole played by the angle $\gamma$ in both providing irrefutable evidence for a complex CKM matrix and placing constraints on the size of NP contributions. It is shown that even if one allows for New Physics a real CKM matrix is excluded at a 99.92% C.L., and the probability for the phase $\gamma$ to be in the interval $[-170^\circ;-10^\circ]\cup [10^\circ;170^\circ]$ is 99.7%.

PhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelPhase (waves)FOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Interval (graph theory)High Energy Physics::ExperimentParticle Physics - Phenomenology
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Large lepton mixing and supernova 1987A

2000

We reconsider the impact of $\bar\nu_e \leftrightarrow \bar\nu_{\mu,\tau}$ neutrino oscillations on the observed $\bar\nu_e$ signal of supernova SN 1987A. Performing a maximum-likelihood analysis using as fit parameters the released binding energy $\Eb$ and the average neutrino energy $\Ee$, we find as previous analyses that $\bar\nu_e \leftrightarrow \bar\nu_{\mu,\tau}$ oscillations with large mixing angles have lower best-fit values for $\Ee$ than small-mixing angle (SMA) oscillations. Moreover, the inferred value of $\Ee$ is already in the SMA case lower than those found in simulations. This apparent conflict has been interpreted as evidence against the large mixing oscillation solutions…

PhysicsNuclear and High Energy PhysicsParticle physicsDegree (graph theory)OscillationHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)FísicaSolar neutrino problemSupernovaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoNeutrino oscillationParticle Physics - PhenomenologyLepton
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On-shell two-loop three-gluon vertex

1998

The two-loop three-gluon vertex is calculated in an arbitrary covariant gauge, in the limit when two of the gluons are on the mass shell. The corresponding two-loop results for the ghost-gluon vertex are also obtained. It is shown that the results are consistent with the Ward-Slavnov-Taylor identities.

PhysicsNuclear and High Energy PhysicsParticle physicsLoop (graph theory)High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyShell (structure)Vertex functionFOS: Physical sciencesGauge (firearms)GluonHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Vertex modelVertex (curve)Covariant transformationHigh Energy Physics::ExperimentParticle Physics - Phenomenology
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Bounds on models with one latticized extra dimension

2003

We study an extension of the standard model with one latticized extra dimension accessible to all fields. The model is characterized by the size of the extra dimension and the number of sites, and contains a tower of massive particles. At energies lower than the mass of the new particles there are no tree-level effects. Therefore, bounds on the scale of new physics can only be set from one-loop processes. We calculate several observables sensitive to loop-effects, such as the $\rho$ parameter, $b\to s \gamma$, $Z\to b\bar b$, and the $B^0\rightleftharpoons\bar{B}^0$ mixing, and use them to set limits on the lightest new particles for different number of sites. It turns out that the continuo…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelLattice field theoryDimension (graph theory)FOS: Physical sciencesFísicaObservableFermionTower (mathematics)Standard ModelLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)
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Angular variation of hard back-to-back hadron suppression in heavy-ion collisions

2008

The basic idea of jet tomography is to infer information about the density evolution of the medium created in heavy-ion (A-A) collisions by studying the suppression of hard probes in an A-A environment as compared to the baseline process known from p-p collisions. The suppression of back-to-back correlations in heavy-ion collisions allows, due to a different geometrical bias, a view into the medium which is qualitatively different from the one offered by single hadron suppression. A control parameter for the suppression corresponding to a systematic variation of in-medium pathlengths and density can be obtained by studying collisions at finite impact parameter b. A systematic variation of p…

PhysicsNuclear and High Energy PhysicsParticle physicsPlane (geometry)HadronMonte Carlo methodFOS: Physical sciencesFunction (mathematics)Jet (particle physics)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Path lengthPath (graph theory)Impact parameterNuclear Experiment
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