Search results for "ExAC"

showing 10 items of 1440 documents

Three-body Coulomb interaction effects in the final state of thePb208(B8,Be7p)Pb208Coulomb breakup reaction

2005

The photodissociation reaction $^{8}\mathrm{B}+\ensuremath{\gamma}\ensuremath{\rightarrow}^{7}\mathrm{Be}+p$ is used to provide information on the astrophysical ${S}_{17}$ factor of the inverse radiative capture reaction, knowledge of which is crucial for an estimation of the high-energy neutrino flux from the sun. Since, at present, the Coulomb field of a fully stripped nucleus serves as the source of the photons, an adequate analysis requires a genuine three-body treatment of this reaction. Among the uncertainties still affecting present analyses, the possible modification of the dissociation cross section by the post-decay acceleration of the fragments $^{7}\mathrm{Be}$ and p in the targ…

PhysicsNuclear and High Energy PhysicsDipoleExact solutions in general relativityScatteringQuantum mechanicsCoulombInverseAtomic physicsMultipole expansionWave functionCharged particlePhysical Review C
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Corrigendum to “On magnetic guidance of charged particles” [Phys. Lett. B 755 (2016) 409–413]

2016

The quantities α′ n and α′ n f are the positions where R(α) in Eqs. (7) and (9) have their maxima, respectively. In Fig. 1(a) the approximation based on these equations is compared with exact results obtained on the basis of Ref. [3]. The position of the spikes are now exactly reproduced. However, for small R ’s there remain some deviations. In particular, for the lowest orbit the expression (α2 + − α2 0) of [2, Eq. (13)] gets imaginary for R/r0 < 0.246 and causes a little kink, see Fig. 1(a). This fact prompted Dubbers [2] replacing for R ≤ 0.34 the quantity α+(R) by the approximation which reads corrected [4] α0[1 + (R/r0)/(8 sin2 α0/2)]. In addition, the statement in Ref. [2] that normal…

PhysicsNuclear and High Energy PhysicsExact results010308 nuclear & particles physicsPosition (vector)0103 physical sciences010306 general physicsMaxima01 natural sciencesCharged particlelcsh:Physicslcsh:QC1-999Mathematical physicsPhysics Letters B
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SUPERFIELDS AND CANONICAL METHODS IN SUPERSPACE

1986

We consider the “supersymmetric roots” of the Heisenberg evolution equation as describing the dynamics of superfields in superspace. We investigate the superfield commutators and their equal time limits and exhibit their noncanonical character even for free superfields. For simplicity, we concentrate on the D=1 case, i.e., the superfield formulation of supersymmetric quantum mechanics in the Heisenberg picture and, as a soluble example, the supersymmetric oscillator. Finally, we express Noether’s theorem in superspace and give the definition of the global conserved supercharges.

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyAstronomy and AstrophysicsSuperfieldSuperspaceHigh Energy Physics::Theorysymbols.namesakeNonlinear Sciences::Exactly Solvable and Integrable SystemsCharacter (mathematics)Supersymmetric gauge theorysymbolsF-termSupersymmetric quantum mechanicsNoether's theoremHeisenberg pictureMathematical physicsModern Physics Letters A
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Three-Body Coulomb Final-State Interaction Effects in the Coulomb Breakup of Light Nuclei

2005

Coulomb breakup of a projectile in the Coulomb field of a fully stripped heavy nucleus is at present one of the most popular experimental methods to obtain information on reactions of interest in nuclear astrophysics. Its theoretical interpretation presents, however, considerable difficulties, due to the three-body nature and the infinite range of the Coulomb forces involved. Among the uncertainties affecting present analyses, the possible modification of the dissociation cross section by three-body Coulomb final-state interactions plays a major role. Various methods which have been proposed to deal with it are briefly reviewed. However, none of them is based on a consistent and mathematica…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsProjectileGeneral Physics and AstronomyFOS: Physical sciencesAstronomy and AstrophysicsBreakup01 natural sciences3. Good healthNuclear Theory (nucl-th)Wave–particle dualityAmplitudeExact solutions in general relativityClassical mechanics0103 physical sciencesNuclear astrophysicsCoulomb010306 general physicsQuantum
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Testing the mechanism of R-parity breaking with slepton LSP decays

2003

In supersymmetric models R-parity can be violated through either bilinear or trilinear terms in the superpotential, or both. If charged scalar leptons are the lightest supersymmetric particles, their decay properties can be used to obtain information about the relative importance of these couplings. We show that in some specific scenarios it is even possible to decide whether bilinear or trilinear terms give the dominant contribution to the neutrino mass matrix.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsScalar (mathematics)SuperpotentialHigh Energy Physics::PhenomenologyFOS: Physical sciencesBilinear interpolationFísicaSupersymmetry01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Nonlinear Sciences::Exactly Solvable and Integrable SystemsR-parity0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationLepton
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R-parity violating sneutrino decays

2004

R-parity can be violated through either bilinear and/or trilinear terms in the superpotential. The decay properties of sneutrinos can be used to obtain information about the relative importance of these couplings provided sneutrinos are the lightest supersymmetric particles. We show that in some specific scenarios it is even possible to decide whether bilinear or trilinear terms give the dominant contribution to the neutrino mass matrix.

PhysicsNuclear and High Energy PhysicsParticle physicsSuperpotentialHigh Energy Physics::PhenomenologyBilinear interpolationFOS: Physical sciencesFísicaMass matrixHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nonlinear Sciences::Exactly Solvable and Integrable SystemsR-parityHigh Energy Physics::ExperimentNeutrino
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Status and Prospects of Top-Quark Physics

2009

The top quark is the heaviest elementary particle observed to date. Its large mass of about 173 GeV/c^2 makes the top quark act differently than other elementary fermions, as it decays before it hadronises, passing its spin information on to its decay products. In addition, the top quark plays an important role in higher-order loop corrections to standard model processes, which makes the top quark mass a crucial parameter for precision tests of the electroweak theory. The top quark is also a powerful probe for new phenomena beyond the standard model. During the time of discovery at the Tevatron in 1995 only a few properties of the top quark could be measured. In recent years, since the star…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesElementary particleFermion01 natural sciencesStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Nonlinear Sciences::Exactly Solvable and Integrable Systems0103 physical sciencesPhysics::Atomic and Molecular ClustersHigh Energy Physics::Experiment010306 general physics
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Universal features of the nuclear matrix elements governing the mass sector of the 0νββ decay

2005

In this work we report on manifest universal features found in the nuclear matrix elements which govern the mass sector of the neutrinoless double beta decay. The results are based on the analysis of the calculated matrix elements corresponding to the decays of 76Ge, 82Se, 100Mo, and 116Cd. The results suggest a dominance of few low-lying nuclear states of few multipoles in these matrix elements. Dedicated charge-exchange reactions could be used to probe these key states to determine experimentally the value of the nuclear matrix element.

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)MatrixFísicaNeutrinoless double betaNuclear matrixNuclear physicsMatrix (mathematics)Double beta decayPartículas ElementalesElement (category theory)Multipole expansionNuclear ExperimentCiencias ExactasPhysics Letters B
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Schematic and realistic model calculations of the isovector spin monopole excitations in 116In

2012

The excitation of Gamow-Teller (GT) and isovector spin monopole (IVSM) Jπ=1+ modes in 116In by (p,n) and (n,p) charge-exchange reactions on 116Cd and on 116Sn, respectively, is studied within the framework of the quasiparticle random-phase approximation. The calculations have been performed both for schematic and realistic model situations. It appears that the calculated admixture of the IVSM and Gamow-Teller (GT) Jπ=1+ excitations is negligible and that the contribution to the strength above 20 MeV of excitation energy, in 116In, is due to the IVSM (σr2t ±) mode. This result is compared with the recent experimental work that reported a large amount of both (p,n) and (n,p) strength beyond 1…

PhysicsNuclear and High Energy Physicsta114IsovectorCondensed matter physicsCiencias FísicasMagnetic monopoleFísicaRadial dependence//purl.org/becyt/ford/1.3 [https]Astronomía//purl.org/becyt/ford/1 [https]Double beta decaySpin and isospin excitationsQuasiparticleExperimental workAtomic physicsExcitationEnergy (signal processing)CIENCIAS NATURALES Y EXACTASSpin-½
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Corrections for positon annihilation in flight in nuclear spectrometry

1973

Abstract Theories of positon single- and two-quanta annihilation in flight, the Fermi beta-decay theory, and theories of positon energy loss are used in calculations of total probabilities of annihilation in flight of positons in continuous spectra. The results are given in a nomogram useful in correcting for positon annihilation in flight in various nuclear-spectrometry experiments. Confirmation of the theoretical basis employed was obtained by comparing total absolute probabilities for annihilation in flight of 62 Cu positons in Perspex, copper, cadmium and lead, using a new differential method. The agreement with the theory was found to be excellent. A method for obtaining “correct” posi…

PhysicsNuclear physicsScintillationNonlinear Sciences::Exactly Solvable and Integrable SystemsAnnihilationContinuous spectrumGamma spectroscopyGeneral MedicineAtomic physicsSpectroscopySpectral lineSemiconductor detectorFermi Gamma-ray Space TelescopeNuclear Instruments and Methods
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