Search results for "Functional analysis"

showing 10 items of 1059 documents

Towards the field theory of the Standard Model on fractional D6-branes on T6 /ℤ6 ′ : Yukawa couplings and masses

2012

We present the perturbative Yukawa couplings of the Standard Model on fractional intersecting D6-branes on T6/Z6' and discuss two mechanisms of creating mass terms for the vector-like particles in the matter spectrum, through perturbative three-point couplings and through continuous D6-brane displacements.

PhysicsStandard Model (mathematical formulation)Theoretical physicsSpectrum (functional analysis)Yukawa potentialBrane cosmologyGeneral Physics and AstronomyField theory (psychology)Fortschritte der Physik
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How to solve Fokker-Planck equation treating mixed eigenvalue spectrum?

2013

An analogy of the Fokker-Planck equation (FPE) with the Schr\"odinger equation allows us to use quantum mechanics technique to find the analytical solution of the FPE in a number of cases. However, previous studies have been limited to the Schr\"odinger potential with a discrete eigenvalue spectrum. Here, we will show how this approach can be also applied to a mixed eigenvalue spectrum with bounded and free states. We solve the FPE with boundaries located at x=\pm L/2 and take the limit L\rightarrow\infty, considering the examples with constant Schr\"{o}dinger potential and with P\"{o}schl-Teller potential. An oversimplified approach was proposed earlier by M.T. Araujo and E. Drigo Filho. A…

PhysicsStatistical Mechanics (cond-mat.stat-mech)Physics and Astronomy (miscellaneous)Spectrum (functional analysis)FOS: Physical sciencesFokker-Planck equationSchrödinger equationMathematical Physics (math-ph)Mathematics::Spectral TheoryCondensed Matter Physicslcsh:QC1-999Pöschl-Teller potentialFokker–Planck equationEigenvalues and eigenvectorsCondensed Matter - Statistical MechanicsMathematical Physicslcsh:PhysicsMathematical physics
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Analytic density functionals with initial-state dependence and memory

2013

We analytically construct the wave function that, for a given initial state, produces a prescribed density for a quantum ring with two non-interacting particles in a singlet state. In this case the initial state is completely determined by the initial density, the initial time-derivative of the density and a single integer that characterizes the (angular) momentum of the system. We then give an exact analytic expression for the exchange-correlation potential that relates two non-interacting systems with different initial states. This is used to demonstrate how the Kohn-Sham procedure predicts the density of a reference system without the need of solving the reference system's Schr\"odinger …

PhysicsStrongly Correlated Electrons (cond-mat.str-el)ta114FOS: Physical sciences02 engineering and technologyState (functional analysis)Function (mathematics)Time-dependent density functional theory021001 nanoscience & nanotechnology01 natural sciencesAtomic and Molecular Physics and OpticsMomentumCondensed Matter - Strongly Correlated ElectronsIntegerQuantum mechanicsKernel (statistics)0103 physical sciencesStatistical physics010306 general physics0210 nano-technologyAdiabatic processQuantumPhysical Review A
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γ-ray and decay spectroscopy of194,195,196At

2013

Excited states of ${}^{195}$At have been studied by means of in-beam $\ensuremath{\gamma}$-ray spectroscopy and the recoil-decay tagging technique. A strongly coupled rotational band feeding the $\ensuremath{\alpha}$-decaying $7/{2}^{\ensuremath{-}}$ state via unobserved transitions was identified. This band is presumably built on the oblate proton ${I}^{\ensuremath{\pi}}=13/{2}^{+}$ state. Confirming earlier measurements, $\ensuremath{\alpha}$ decays from the $1/{2}^{+}$ and $7/{2}^{\ensuremath{-}}$ states were observed. Additionally, an $E3$ branch competing with the $\ensuremath{\alpha}$ decay of the $7/{2}^{\ensuremath{-}}$ state was inferred. Also $\ensuremath{\alpha}$ decays of the od…

PhysicsStrongly coupledNuclear and High Energy PhysicsProtonExcited stateOblate spheroidState (functional analysis)Alpha decayAtomic physicsSpectroscopyPhysical Review C
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Phase diagram of dirty two-band superconductors and observability of impurity-induced $s+is$ state

2016

We investigate the phase diagram of dirty two-band superconductors. This paper primarily focuses on the properties and observability of the time-reversal symmetry-breaking $s+is$ superconducting states, which can be generated in two-band superconductors by interband impurity scattering. We show that such states can appear in two distinct ways. First, according to a previously discussed scenario, the $s+is$ state can form as an intermediate phase at the impurity-driven crossover between $s_{\pm}$ and $s_{++}$ states. We show that there is a second scenario where domains of the $s+is$ state exists in the form of an isolated dome inside the $s_{\pm}$ domain, completely detached from the transi…

PhysicsSuperconductivityta114Condensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesState (functional analysis)superconductors01 natural sciences010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)Two bandImpurityCondensed Matter::Superconductivity0103 physical sciencesObservability010306 general physicsphase diagramsPhase diagram
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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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Phonons in an inhomogeneous continuum: Vibrations of an embedded nanoparticle

2004

The spectrum of acoustic vibrational modes of an inhomogeneous elastic continuum are analyzed with application to a spherical nanoparticle embedded in an infinite glass block. The relationship of these modes to the discrete vibrational spectrum of a free sphere is studied. The vibrational modes of a sphere with a fixed surface are relevant in some situations. Comparisons are also made to calculations of mode frequency and damping based on complex valued frequency.

PhysicsSurface (mathematics)Condensed Matter - Materials Sciencebusiness.industryPhononContinuum (design consultancy)Spectrum (functional analysis)Materials Science (cond-mat.mtrl-sci)FOS: Physical sciencesNanoparticleCondensed Matter PhysicsMolecular physicsHot bandElectronic Optical and Magnetic MaterialsVibrationOpticsMolecular vibrationbusinessPhysical Review B
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The average over a sphere

1980

Abstract The N points ri and the N segments ΔΩi of the unit sphere used in the numerical approximation of the average over the sphere are optimized to approximate the average of the set of spherical harmonics {;Yl,m;l = 0, 1, 2, …, L}; up to L = 18. The symmetry of f( r ) can be taken into acount by using only a distinct subquantity of the N point {; r i , ΔΩ i }; . Sets for N = 48n (n = 1, 2, …, 6) are tabulated. The advantage of the method is shown by the calculation of a powder Mossbauer spectrum including electric and magnetic hyperfine interactions.

PhysicsUnit sphereNumerical approximationSpectrum (functional analysis)Mössbauer spectroscopySpherical harmonicsPoint (geometry)General MedicineAtomic physicsHyperfine structureSymmetry (physics)Nuclear Instruments and Methods
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Precision Spectroscopy of Deeply Bound Pionic Atoms and Partial Restoration of Chiral Symmetry in Medium

2011

We study theoretically the formation spectra of deeply bound pionic atoms expected to be observed by experiments with high energy resolution at RIBF/RIKEN, and we discuss in detail the possibilities to extract new information on the pion properties at finite density from the observed spectra, which may provide information on partial restoration of chiral symmetry in medium. We find that the non-yrast pionic states such as 2s are expected to be seen in the (d,3He) spectra, which will be helpful to reduce uncertainties of the theoretical calculations in the neutron wave functions in nucleus. The observation of the 2s state with the ground 1s state is also helpful to reduce the experimental un…

PhysicsWave function renormalizationPhysics and Astronomy (miscellaneous)Nuclear TheoryNuclear TheoryFOS: Physical sciencesState (functional analysis)Spectral lineNuclear Theory (nucl-th)PionNeutronAtomic physicsWave functionConstant (mathematics)Nuclear ExperimentExcitation
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Theρ(ω)/B*(B) system and bound states in the unitary local Hidden Gauge approach

2016

In this work, we study systems composed of a ρ/ω and B* meson pair. We find three bound states in isospin, spin-parity channels (1/2, 0+ ), (1/2, 1+ ) and (1/2, 2+ ). The state with J = 2 can be a good candidate for the B * 2 (5747). We also study the ρB system, and a bound state with mass 5728 MeV and width around 20 MeV is obtained, which can be identified with the B 1 (5721) resonance. In the case of I = 3/2, one obtains repulsion and thus, no exotic (molecular) mesons in this sector are generated in the approach.

PhysicsWork (thermodynamics)Particle physicsMeson010308 nuclear & particles physicsPhysicsQC1-999State (functional analysis)Gauge (firearms)01 natural sciencesResonance (particle physics)Unitary stateIsospin0103 physical sciencesBound stateAtomic physics010306 general physicsEPJ Web of Conferences
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