Search results for "Variant"

showing 10 items of 1267 documents

Tridimensional invariant correlation based on phase-coded and sine-coded range images

1998

New methods for recognition of range images based on correlation are presented. The techniques allow the detection of a range image of a tridimensional pattern whatever its position along the x, y and z axes. The first method uses the phase-coding of the range image in order to obtain invariance along the z-axis in the correlation process. The second method uses the sine-coding of the range image in order to obtain better discrimination than that obtained with phase-coding. The third method is a hybrid one that makes use of sine-coding for the input scene and phase-coding for the reference image, so both the full translation invariance and high discrimination abilities are obtained. Compute…

PhysicsReference imageOpticsbusiness.industrySineInvariant (physics)businessAlgorithmTranslation invarianceJournal of Optics
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FINITE-RANGE SEPARABLE PAIRING INTERACTION WITHIN NEW N[sup 3]LO DFT APPROACH

2011

For over four decades, the Skyrme functional within various parametrizations has been used to calculate nuclear properties. In the last few years there was a number of attempts to improve its performance and introduce generalized forms. In particular, the most general phenomenologi‐cal quasi‐local energy density functional, which contains all combinations of density, spin‐density, and their derivatives up to the sixth order (N3LO), was proposed in reference [1]. Since in the phe‐nomenological functional approaches the particle‐particle (pp) interaction channel is treated independently from the particle‐hole (ph) channel, there remains a question of what pairing interaction is suitable to us…

PhysicsRenormalizationAngular momentumTheoretical physicsPairingQuantum electrodynamicsNuclear structureInvariant (mathematics)Energy functionalSeparable spaceSpin-½AIP Conference Proceedings
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Type D vacuum solutions: a new intrinsic approach

2013

We present a new approach to the intrinsic properties of the type D vacuum solutions based on the invariant symmetries that these spacetimes admit. By using tensorial formalism and without explicitly integrating the field equations, we offer a new proof that the upper bound of covariant derivatives of the Riemann tensor required for a Cartan-Karlhede classification is two. Moreover we show that, except for the Ehlers-Kundt's C-metrics, the Riemann derivatives depend on the first order ones, and for the C-metrics they depend on the first order derivatives and on a second order constant invariant. In our analysis the existence of an invariant complex Killing vector plays a central role. It al…

PhysicsRiemann curvature tensorPure mathematicsPhysics and Astronomy (miscellaneous)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Invariant (physics)Upper and lower boundsGeneral Relativity and Quantum Cosmologysymbols.namesakeRiemann hypothesisKilling vector fieldGeneral Relativity and Quantum CosmologyHomogeneous spacesymbolsCovariant transformationField equation
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Measurements of branching fractions, rate asymmetries, and angular distributions in the rare decays B→K + - and B→K* + -

2006

We present measurements of the flavor-changing neutral current decays B -> K center dot(+)center dot(-) and B -> K-*center dot(+)center dot(-), where center dot(+)center dot(-) is either an e(+)e(-) or mu(+)mu(-) pair. The data sample comprises 229x10(6) Upsilon(4S)-> B (B) over bar decays collected with the BABAR detector at the PEP-II e(+)e(-) storage ring. Flavor-changing neutral current decays are highly suppressed in the standard model and their predicted properties could be significantly modified by new physics at the electroweak scale. We measure the branching fractions B(B -> K center dot(+)center dot(-))=(0.34 +/- 0.07 +/- 0.02)x10(-6), B(B -> K-*center dot(+)center dot(-))=(0.78(-…

PhysicsSemileptonic decayNuclear and High Energy PhysicsElectron pairMuon010308 nuclear & particles physicsBranching fractionElectron–positron annihilationParticle physicsBABAR detectorCondensed Matter::Mesoscopic Systems and Quantum Hall Effect01 natural sciencesHEPNuclear physics0103 physical sciencesBaBarInvariant massB mesonHigh Energy Physics::ExperimentAtomic physics010306 general physicsFísica de partículesExperimentsLepton
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A missing link: What is behind de Broglie's "Periodic phenomenon"?

1996

The present work constitutes an attempt to give the interpretation of de Broglie's internal periodic phenomenon which ascribes the frequencym0c2/h to each single entity in its eigensystem of coordinates. This phenomenon provides existence in principle of the ideal proper-time scale, making it possible to identify the geometric proper-time interval with a physically existing one, thus ensuring the realization of basic postulates of the relativity theory. According to the latter, neither time nor de Broglie's frequency are invariant with respect to the Lorentz transformation of the coordinate system. A search for the fundamental invariant demands passing over to dimensionless quantities, and …

PhysicsSequenceLorentz transformationCoordinate systemGeneral Physics and AstronomyNatural numberInvariant (physics)Theoretical physicssymbols.namesakeTheory of relativityClassical mechanicssymbolsProper timeMatter wave
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Triangle singularity in the B−→K−π0X(3872) reaction and sensitivity to the X(3872) mass

2020

We have done a study of the ${B}^{\ensuremath{-}}\ensuremath{\rightarrow}{K}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}X(3872)$ reaction by means of a triangle mechanism via the chain of reactions: ${B}^{\ensuremath{-}}\ensuremath{\rightarrow}{K}^{\ensuremath{-}}{D}^{*0}{\overline{D}}^{*0}$; ${D}^{*0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}{D}^{0}$; ${D}^{0}{\overline{D}}^{*0}\ensuremath{\rightarrow}X(3872)$. We show that this mechanism generates a triangle singularity in the ${\ensuremath{\pi}}^{0}X(3872)$ invariant mass for a very narrow window of the $X(3872)$ mass, around the present measured values, and show that the peak positions and the shape of the mass distributions are sensitiv…

PhysicsSingularity010308 nuclear & particles physics0103 physical sciencesMass spectrumInvariant massSensitivity (control systems)Atomic physics010306 general physics01 natural sciencesX(3872)Physical Review D
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Invariant density and time asymptotics for collisionless kinetic equations with partly diffuse boundary operators

2018

This paper deals with collisionless transport equationsin bounded open domains $\Omega \subset \R^{d}$ $(d\geq 2)$ with $\mathcal{C}^{1}$ boundary $\partial \Omega $, orthogonallyinvariant velocity measure $\bm{m}(\d v)$ with support $V\subset \R^{d}$ and stochastic partly diffuse boundary operators $\mathsf{H}$ relating the outgoing andincoming fluxes. Under very general conditions, such equations are governedby stochastic $C_{0}$-semigroups $\left( U_{\mathsf{H}}(t)\right) _{t\geq 0}$ on $%L^{1}(\Omega \times V,\d x \otimes \bm{m}(\d v)).$ We give a general criterion of irreducibility of $%\left( U_{\mathsf{H}}(t)\right) _{t\geq 0}$ and we show that, under very natural assumptions, if an …

PhysicsStochastic semigroupApplied MathematicsKinetic equation010102 general mathematicsConvergence to equilibriumZero (complex analysis)Boundary (topology)01 natural sciencesMeasure (mathematics)010101 applied mathematicsConvergence to equilibrium; Kinetic equation; Stochastic semigroupFlow (mathematics)[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Bounded functionCompactness theorem[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Ergodic theory[MATH.MATH-AP] Mathematics [math]/Analysis of PDEs [math.AP][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]0101 mathematicsInvariant (mathematics)Mathematical PhysicsAnalysisMathematical physicsAnnales de l'Institut Henri Poincaré C, Analyse non linéaire
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Driving topological phases by spatially inhomogeneous pairing centers

2017

We investigate the effect of periodic and disordered distributions of pairing centers in a one-dimensional itinerant system to obtain the microscopic conditions required to achieve an end Majorana mode and the topological phase diagram. Remarkably, the topological invariant can be generally expressed in terms of the physical parameters for any pairing center configuration. Such a fundamental relation allows us to unveil hidden local symmetries and to identify trajectories in the parameter space that preserve the non-trivial topological character of the ground state. We identify the phase diagram with topologically non-trivial domains where Majorana modes are completely unaffected by the spa…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed Matter - SuperconductivityFOS: Physical sciences02 engineering and technologyParameter space021001 nanoscience & nanotechnologyTopology01 natural sciencesSuperconductivity (cond-mat.supr-con)MAJORANACondensed Matter - Strongly Correlated ElectronsPairing0103 physical sciencesHomogeneous spaceInvariant (mathematics)010306 general physics0210 nano-technologyGround statePhase diagramPhysical Review B
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Topological Hamiltonian as an exact tool for topological invariants

2012

We propose the concept of `topological Hamiltonian' for topological insulators and superconductors in interacting systems. The eigenvalues of topological Hamiltonian are significantly different from the physical energy spectra, but we show that topological Hamiltonian contains the information of gapless surface states, therefore it is an exact tool for topological invariants.

PhysicsSuperconductivityHigh Energy Physics - TheoryStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciencesCondensed Matter PhysicsTopology01 natural sciences010305 fluids & plasmassymbols.namesakeCondensed Matter - Strongly Correlated ElectronsGapless playbackHigh Energy Physics - Theory (hep-th)Topological insulator0103 physical sciencessymbolsTopological invariantsGeneral Materials Science010306 general physicsHamiltonian (quantum mechanics)Mathematics::Symplectic GeometryEigenvalues and eigenvectorsJournal of Physics Condensed Matter
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Λ(1405) resonance as a superposition of two states

2008

Chiral unitarity models have shown the existence of two states with the same quantum numbers in the vicinity of the Λ(1405), both contributing to the final experimental invariant mass distribution. The K − p → π 0 π 0 Σ 0 reaction, discussed in detail in this work, gives maximal possible weight to the second Λ(1405) state, which is narrower and of higher energy than the nominal Λ(1405). The calculated distribution of π 0 Σ 0 states forming the Λ(1405) is in agreement with a recent experimental data, and shows a peak at 1420 MeV and a relatively narrow width of Γ = 38 MeV. In contrast, the π − p → K 0 πΣ reaction gives more weight to the pole at lower energy and with a larger width. The data…

PhysicsSuperposition principleUnitarityBound stateInvariant massState (functional analysis)Atomic physicsQuantum numberResonance (particle physics)Bar (unit)
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