Search results for "Free parameter"

showing 9 items of 49 documents

High-temperature series analysis of the p-state Potts glass model on d-dimensional hypercubic lattices

1999

We analyze recently extended high-temperature series expansions for the “Edwards-Anderson” spin-glass susceptibility of the p-state Potts glass model on d-dimensional hypercubic lattices for the case of a symmetric bimodal distribution of ferro- and antiferromagnetic nearest-neighbor couplings \(\). In these star-graph expansions up to order 22 in the inverse temperature \(\), the number of Potts states p and the dimension d are kept as free parameters which can take any value. By applying several series analysis techniques to the new series expansions, this enabled us to determine the critical coupling Kc and the critical exponent \(\) of the spin-glass susceptibility in a large region of …

PhysicsSpin glassSeries (mathematics)Critical phenomenaCondensed Matter PhysicsCondensed Matter::Disordered Systems and Neural NetworksElectronic Optical and Magnetic MaterialsPadé approximantCondensed Matter::Strongly Correlated ElectronsStatistical physicsSeries expansionCritical exponentFree parameterPotts modelThe European Physical Journal B
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Diabatic description of charmoniumlike mesons. II. Mass corrections and strong decay widths

2021

From a diabatic bound state approach to $J^{PC}=1^{--}$ and $(0,1,2)^{++}$ charmoniumlike resonances below $4.1$ GeV, formulated in terms of ${c\overline{c}}$ and closed meson-meson channels, we calculate mass shifts and widths due to open meson-meson channels. This calculation does not involve any new free parameter, so comparison of our predictions with existing data provides a direct test of our approach. Further mass corrections are also estimated and good agreement with the measured masses comes out. As for the calculated widths, overall reasonable, they point out to the need of some refinement of our current bound state approximation for an accurate description of data. These results …

Quantum chromodynamicsPhysicsParticle physicsCurrent (mathematics)Meson010308 nuclear & particles physicsDiabaticFOS: Physical sciencesResonance01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Direct test0103 physical sciencesBound stateHigh Energy Physics::Experiment010306 general physicsFree parameterPhysical Review D
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Mixed finite elements for nonlocal elastic multilayered composite plate refined theories

2020

Abstract A novel mixed finite element formulation for the layerwise analysis of nonlocal multilayered composite plates is presented. The finite elements are formulated starting from the weak form of a set of governing equations for the laminate layers that were deduced via the Reissner Mixed Variational Theorem. The primary variables, namely displacements and out-of-plane stresses, are expressed at layer level as through-the-thickness expansions of suitable selected functions with coefficients approximated by the finite element scheme. The through-the-thickness expansion order is considered as a free parameter. This way, finite elements for different refined higher order plate theories can …

Refined plate theorieQuadrilateralMathematical analysisReissner Mixed Variational Theorem02 engineering and technology021001 nanoscience & nanotechnologyFinite element methodSet (abstract data type)Mixed finite element020303 mechanical engineering & transports0203 mechanical engineeringNonlocal elasticityComposite platePlate theoryCeramics and CompositesOrder (group theory)Settore ING-IND/04 - Costruzioni E Strutture Aerospaziali0210 nano-technologyLaminated compositesCivil and Structural EngineeringFree parameterMathematicsVariable (mathematics)Composite Structures
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Non-linear System Identification with Composite Relevance Vector Machines

2007

Nonlinear system identification based on relevance vector machines (RVMs) has been traditionally addressed by stacking the input and/or output regressors and then performing standard RVM regression. This letter introduces a full family of composite kernels in order to integrate the input and output information in the mapping function efficiently and hence generalize the standard approach. An improved trade-off between accuracy and sparsity is obtained in several benchmark problems. Also, the RVM yields confidence intervals for the predictions, and it is less sensitive to free parameter selection. Teoría de la Señal y Comunicaciones

Relevance Vector MachinesTelecomunicacionesNonlinear system identificationbusiness.industryRVMApplied MathematicsNonlinear System IdentificationRegression analysisPattern recognitionComposite kernelsFunction (mathematics)Support vector machineNonlinear systemStatistics::Machine LearningSignal ProcessingBenchmark (computing)3325 Tecnología de las TelecomunicacionesRelevance (information retrieval)Artificial intelligenceElectrical and Electronic EngineeringbusinessMathematicsFree parameter
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StalAge – An algorithm designed for construction of speleothem age models

2011

Abstract Here we present a new algorithm ( StalAge ), which is designed to construct speleothem age models. The algorithm uses U-series ages and their corresponding age uncertainty for modelling and also includes stratigraphic information in order to further constrain and improve the age model. StalAge is applicable to problematic datasets that include outliers, age inversions, hiatuses and large changes in growth rate. Manual selection of potentially inaccurate ages prior to application is not required. StalAge can be applied by the general, non-expert user and has no adjustable free parameters. This offers the highest degree of reproducibility and comparability of speleothem records from …

Smoothing splineSpline (mathematics)Robustness (computer science)StratigraphyOutlierBayesian probabilityEarth and Planetary Sciences (miscellaneous)Range (statistics)GeologySample (statistics)AlgorithmGeologyFree parameterQuaternary Geochronology
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Thermodynamic and kinetic properties of water–oil–surfactant mixtures

1998

Abstract We present experimental data on thermodynamic and kinetic properties of the emulsification failure of a droplet-phase microemulsion, and model them by a bending free energy. In contrast to most other models used to describe water–oil–surfactant mixtures no entropic contributions are included in the present description. Still, there is quantitative agreement between theory and measurements, even though there are no free parameters in our model – only experimentally accessible material constants appear.

Statistics and ProbabilityMaterials scienceProperties of waterThermodynamicsBendingCondensed Matter PhysicsKinetic energychemistry.chemical_compoundPulmonary surfactantchemistryMaterial constantsMicroemulsionMaterial propertiesFree parameterPhysica A: Statistical Mechanics and its Applications
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Duality and spatial inhomogeneity

2001

Within the framework on non-extensive thermostatistics we revisit the recently advanced q-duality concept. We focus our attention here on a modified q-entropic measure of the spatial inhomogeneity for binary patterns. At a fixed length-scale this measure exhibits a generalised duality that links appropriate pairs of q and q' values. The simplest q q' invariant function, without any free parameters, is deduced here. Within an adequate interval q < qo < q', in which the function reaches its maximum value at qo, this invariant function accurately approximates the investigated q-measure, nitidly evidencing the duality phenomenon. In the close vicinity of qo, the approximate meaningful rel…

Statistics and ProbabilityPhysicsStatistical Mechanics (cond-mat.stat-mech)Value (computer science)Binary numberDuality (optimization)FOS: Physical sciencesFunction (mathematics)Interval (mathematics)Condensed Matter PhysicsMeasure (mathematics)Focus (optics)Condensed Matter - Statistical MechanicsMathematical physicsFree parameter
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A Unified Theory of Psychophysical Laws in Auditory Intensity Perception.

2020

Psychophysical laws quantitatively relate perceptual magnitude to stimulus intensity. While most people have accepted Stevens's power function as the psychophysical law, few believe in Fechner's original idea using just-noticeable-differences (jnd) as a constant perceptual unit to educe psychophysical laws. Here I present a unified theory in hearing, starting with a general form of Zwislocki's loudness function (1965) to derive a general form of Brentano's law. I will arrive at a general form of the loudness-jnd relationship that unifies previous loudness-jnd theories. Specifically, the "slope," "proportional-jnd," and "equal-loudness, equal-jnd" theories, are three additive terms in the ne…

medicine.medical_treatmentmedia_common.quotation_subjectlcsh:BF1-990BioengineeringLoudnessWeber's lawStevens's lawClinical ResearchCochlear implantPerceptionHypothesis and TheorymedicineStevens’s lawjust-noticeable-differences (jnd)PsychologyauditoryPower functionUnified field theoryGeneral PsychologyBackward maskingmedia_commonAssistive Technologyintensity discriminationRehabilitationNeurosciencesloudnessWeber’s lawZwislockilcsh:PsychologyLawForward maskingjust-noticeable-differencesCognitive SciencesFechner's lawPsychologyFechner’s lawFree parameter
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Search for Electron Antineutrino Appearance in a Long-baseline Muon Antineutrino Beam

2020

Electron antineutrino appearance is measured by the T2K experiment in an accelerator-produced antineutrino beam, using additional neutrino beam operation to constrain parameters of the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) mixing matrix. T2K observes 15 candidate electron antineutrino events with a background expectation of 9.3 events. Including information from the kinematic distribution of observed events, the hypothesis of no electron antineutrino appearance is disfavored with a significance of 2.40 σ and no discrepancy between data and PMNS predictions is found. A complementary analysis that introduces an additional free parameter which allows non-PMNS values of electron neutrino and a…

muon antineutrino beamGeneral Physics and Astronomyantineutrino/mu: secondary beamKAMIOKANDEantineutrino/e: particle identification01 natural sciences09 EngineeringHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)secondary beam [neutrino/mu][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]neutrino/e: particle identificationQCPhysics02 Physical SciencesPhysicsJ-PARC LabT2K experimentelectron antineutrinoT2K CollaborationkinematicsPhysical SciencesParticle Physics - ExperimentT2K experiment in an accelerator-producedGeneral Physics530 PhysicsPhysics MultidisciplinaryFOS: Physical sciencesparticle identification [antineutrino/e]Neutrino beamsecondary beam [antineutrino/mu]530Physics::GeophysicsNuclear physics0103 physical sciencesmixingddc:530010306 general physics01 Mathematical SciencesMuonScience & Technologyparticle identification [neutrino/e]hep-exbackgroundHigh Energy Physics - Experiment; High Energy Physics - Experimentneutrino/mu: secondary beamantineutrino: oscillationoscillation [antineutrino]Elementary Particles and FieldsHigh Energy Physics::ExperimentPMNSElectron neutrinoBeam (structure)Free parameterexperimental results
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