Search results for "Mathematical physics"

showing 10 items of 2687 documents

Gravity waves from non-minimal quadratic inflation

2015

We discuss non-minimal quadratic inflation in supersymmetric (SUSY) and non-SUSY models which entails a linear coupling of the inflaton to gravity. Imposing a lower bound on the parameter cR, involved in the coupling between the inflaton and the Ricci scalar curvature, inflation can be attained even for subplanckian values of the inflaton while the corresponding effective theory respects the perturbative unitarity up to the Planck scale. Working in the non-SUSY context we also consider radiative corrections to the inflationary potential due to a possible coupling of the inflaton to bosons or fermions. We find ranges of the parameters, depending mildly on the renormalization scale, with adju…

Inflation (cosmology)PhysicsHigh Energy Physics - TheoryCosmology and Nongalactic Astrophysics (astro-ph.CO)UnitaritySuperpotentialHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and AstrophysicsSupersymmetryAstrophysics::Cosmology and Extragalactic AstrophysicsInflatonCoupling (probability)High Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Effective field theoryScalar curvatureMathematical physicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Precision luminosity measurements at LHCb

2014

Measuring cross-sections at the LHC requires the luminosity to be determined accurately at each centre-of-mass energy $\sqrt{s}$. In this paper results are reported from the luminosity calibrations carried out at the LHC interaction point 8 with the LHCb detector for $\sqrt{s}$ = 2.76, 7 and 8 TeV (proton-proton collisions) and for $\sqrt{s_{NN}}$ = 5 TeV (proton-lead collisions). Both the "van der Meer scan" and "beam-gas imaging" luminosity calibration methods were employed. It is observed that the beam density profile cannot always be described by a function that is factorizable in the two transverse coordinates. The introduction of a two-dimensional description of the beams improves sig…

Instrumentation for particle accelerators and storage rings - high energy (linear acceleratorsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)cluster finding[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment06.20.fbInstrumentationMathematical PhysicsQCPhysicsLuminosity (scattering theory)Large Hadron ColliderPattern recognition cluster finding calibration and fitting methodssynchrotrons)DetectorPattern recognition cluster finding calibration and fitting methodsComputer interfacecalibration and fitting methodsFísica nuclearTracking and position-sensitive detectorLHCParticle Physics - ExperimentParticle physics29.40.GxPattern recognition cluster finding calibration and fitting methods; Instrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons)Astrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsLHCb - Abteilung HofmannPattern recognition cluster finding calibration and fitting methodInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons)NOConsistency (statistics)Pattern recognitionCalibrationSDG 7 - Affordable and Clean EnergyInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons)/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyInteraction pointStandards and calibrationFunction (mathematics)29.50.+vLHCbInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons); Pattern recognition cluster finding calibration and fitting methods; Instrumentation; Mathematical PhysicsTEVPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons); Pattern recognition cluster finding calibration and fitting methodsEnergy (signal processing)
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A family of complex potentials with real spectrum

1999

We consider a two-parameter non-Hermitian quantum mechanical Hamiltonian operator that is invariant under the combined effects of parity and time reversal transformations. Numerical investigation shows that for some values of the potential parameters the Hamiltonian operator supports real eigenvalues and localized eigenfunctions. In contrast with other parity times time reversal symmetric models which require special integration paths in the complex plane, our model is integrable along a line parallel to the real axis.

Integrable systemFOS: Physical sciencesGeneral Physics and AstronomyComplex planeQuantum mechanicsMathematical analysisQuantumsymbols.namesakeHamiltonian (quantum mechanics)EigenfunctionEigenvalues and eigenvectorsEigenvalues and eigenvectorsPhysicsIntegrable systemQuantum PhysicsPhysicsMathematical analysisFísicaStatistical and Nonlinear PhysicsParity (physics)EigenfunctionInvariant (physics)Invariant (physics)Parity (physics)Mathematical physicssymbolsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)Complex planeMathematics
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On the integrability of the extended nonlinear Schrödinger equation and the coupled extended nonlinear Schrödinger equations

2000

We consider the extended nonlinear Schr¨ (ENLS) equation which governs the propagation of nonlinear optical fields in a fibre with higher-order effects such as higher-order dispersion and self-steepening. We show that the ENLS equation does not pass the Painlev´ test. Similarly, we claim that the coupled ENLS equations and N -coupled ENLS equations which govern the simultaneous propagation of two and more nonlinear fields in optical fibres are also not integrable from the Painlev´ e analysis point of view.

Integrable systemMathematical analysisGeneral Physics and AstronomyStatistical and Nonlinear PhysicsSchrödinger equationsymbols.namesakeNonlinear opticalNonlinear systemClassical mechanicssymbolsDispersion (water waves)Nonlinear Schrödinger equationMathematical PhysicsMathematicsJournal of Physics A: Mathematical and General
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Spatially chaotic configurations and functional equations with rescaling

1996

The functional equation is associated with the appearance of spatially chaotic structures in amorphous (glassy) materials. Continuous compactly supported solutions of the above equation are of special interest. We shall show that there are no such solutions for , whereas such a solution exists for almost all . The words `for almost all q' in the previous sentence cannot be omitted. There are exceptional values of q in the interval for which there are no integrable solutions. For example, , which is the reciprocal of the `golden ratio' is such an exceptional value. More generally, if is any Pisot - Vijayaraghavan number, or any Salem number, then is an exceptional value.

Integrable systemSalem numberMathematical analysisFunctional equationChaoticGeneral Physics and AstronomyValue (computer science)Statistical and Nonlinear PhysicsInterval (mathematics)Mathematical PhysicsReciprocalMathematicsJournal of Physics A: Mathematical and General
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Radon transform as a set of probability distributions

2009

It is proved that the Radon transform of the Wigner function gives the probability distributions related to measuring the observable operators obtained as linear combinations of position and momentum of the relevant particle. The generalization to an arbitrary number of degrees of freedom is given.

Integral transformsOptical tomographySettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciRadon transformCharacteristic function (probability theory)Mathematical analysisWigner semicircle distributionCondensed Matter PhysicsConvolution of probability distributionsAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaRegular conditional probabilityProbability distributionWigner distribution functionQuantum tomographyMathematical PhysicsMathematicsK-distribution
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Hysteresis Model of Unconscious-Conscious Interconnection: Exploring Dynamics on m-Adic Trees

2015

The theoretical model outlined in this paper, has been experimentally validated by: H. Kim ,J-Y. Moon ,G.A. Mashour & U. Lee, ''Mechanisms of hysteresis in human brain networks during transitions of consciousness and unconsciousness: Theoretical principles and empirical evidence'', PLOS-Computational Biology, August 30, 2018, https://journals.plos.org/ploscompbiol/article?id=10.1371/journal.pcbi.1006424; International audience; In this brief note, we focus attention on a possible implementation of a basic hysteretic pattern (the Preisach one), suitably generalized, into a formal model of unconscious-conscious interconnection and based on representation of mental entities by m-adic numbers. …

InterconnectionhysteresiUnconscious mindm-adic treeGeneral Mathematics[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]Representation (systemics)unconscious[SHS.PSY]Humanities and Social Sciences/Psychologyunconsciou[MATH.MATH-FA]Mathematics [math]/Functional Analysis [math.FA]Focus (linguistics)AlgebraHysteresishysteresisp-adic treeDynamics (music)[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Algebra over a field[PHYS.COND]Physics [physics]/Condensed Matter [cond-mat]MathematicsPreisach model
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Transcranial magnetic resonance imaging-guided focused ultrasound treatment at 1.5 T: a retrospective study on treatment and patient-related paramete…

2020

Objective: To present a retrospective analysis of patient- and sonication-related parameters of a group of patients treated with a transcranial magnetic resonance imaging (MRI)-guided focused ultrasound (tcMRgFUS) system integrated with a 1.5-T MRI unit. Methods: The data obtained from 59 patients, who underwent the tcMRgFUS procedure from January 2015 to April 2019, were retrospectively reviewed for this study. The following data, among others, were mainly collected: skull density ratio (SDR), skull area (SA), number of available transducer elements (Tx), and estimated focal power at target (FP). For each of the four different treatment stages, we calculated the number of sonication proces…

Interventional magnetic resonance imagingMaterials Science (miscellaneous)medicine.medical_treatmentParkinson's diseaseEssential TremorBiophysicsGeneral Physics and Astronomy01 natural sciencesFocused ultrasound0103 physical sciencesmedicinePlane orientationInterventional Magnetic Resonance ImagingPhysical and Theoretical Chemistry010306 general physicsMathematical Physicsmedicine.diagnostic_testbusiness.industryThalamotomySettore MED/27 - NeurochirurgiaSettore MED/37 - NeuroradiologiaMagnetic resonance imagingRetrospective cohort studystereotaxic techniqueslcsh:QC1-999Settore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Parkinson Disease.essential tremor; high-intensity focused ultrasound ablation; interventional magnetic resonance imaging; Parkinson's disease; stereotaxic techniquesCoronal planeStereotaxic techniqueHigh-Intensity Focused Ultrasound AblationStereotaxic TechniqueSettore MED/26 - NeurologiaNuclear medicinebusinessSettore MED/36 - Diagnostica Per Immagini E Radioterapialcsh:Physics
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Three-dimensional singletons

1990

The three-dimensional analog of singleton gauge theory turns out to be related to the topological gauge theory of Schwartz and Witten. It is a fully-fledged gauge theory, though it involves only a single scalar field. Real, physical degrees of freedom propagate in 3-space, but they are ‘confined’ in the sense that they cannot be detected locally. The physical Hamiltonian density is not zero, but it is concentrated on the boundary at spatial infinity. This boundary surface, a torus, supports a two-dimensional conformal field theory.

Introduction to gauge theoryHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice field theoryStatistical and Nonlinear PhysicsGeometryMathematical PhysicsGauge anomalyBRST quantizationGauge symmetryMathematicsGauge fixingMathematical physicsLetters in Mathematical Physics
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Some topological invariants for three-dimensional flows

2001

We deal here with vector fields on three manifolds. For a system with a homoclinic orbit to a saddle-focus point, we show that the imaginary part of the complex eigenvalues is a conjugacy invariant. We show also that the ratio of the real part of the complex eigenvalue over the real one is invariant under topological equivalence. For a system with two saddle-focus points and an orbit connecting the one-dimensional invariant manifold of those points, we compute a conjugacy invariant related to the eigenvalues of the vector field at the singularities. (c) 2001 American Institute of Physics.

Invariant polynomialApplied MathematicsMathematical analysisInvariant manifoldGeneral Physics and AstronomyStatistical and Nonlinear PhysicsFinite type invariantConjugacy classHeteroclinic orbitHomoclinic orbitInvariant (mathematics)Mathematical PhysicsCenter manifoldMathematicsChaos: An Interdisciplinary Journal of Nonlinear Science
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