Search results for "weak [Gravitational lensing]"

showing 10 items of 636 documents

CMB Anisotropy Computations Using Hydra Gas Code

2014

From FFP6 to FFP11, we presented the advances in our Cosmic Microwave Background (CMB) anisotropy computations using N-body Hydra Codes. For such computations, codes without baryons were used: First sequential versions and afterwards parallel ones. With both of them we computed the weak lensing and the Rees-Sciama contributions to the CMB angular power spectrum. Using our numerical techniques, we reported a lensing effect higher than that estimated in previous papers (for very small angular scales). Our CMB computations require less interpolations and approximations than other approaches. This could explain part of our excess of power in lensing computations. Our higher time and angular res…

BaryonPhysicsComputationCosmic microwave backgroundDark matterAstrophysics::Instrumentation and Methods for AstrophysicsSpectral densityAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsAnisotropySpectral lineWeak gravitational lensingComputational physics
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A New Numerical Approach to Estimate the Sunyaev–Zel’dovich Effect

2013

Several years ago, we designed a particular ray tracing method. Combined with a Hydra parallel code (without baryons), it may compute some CMB anisotropies: weak lensing (WL) and Rees–Sciama (RS) effects. Only dark matter is fully necessary to estimate these effects. For very small angular scales, we made an exhaustive study leading to a lensing contribution slightly—but significantly—greater than previous ones. Afterwards, the same ray tracing procedure was included in a parallel Hydra code with baryons. The resulting code was then tested. This code is being currently applied to the study of the thermal and kinetic Sunyaev–Zel’dovich (SZ) contributions to the CMB anisotropies. We present h…

BaryonPhysicsRay tracing (physics)Cosmic microwave backgroundDark matterAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsTest particleKinetic energySunyaev–Zel'dovich effectWeak gravitational lensing
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Influence of a thin horizontal weak layer on the mechanical behaviour of shallow foundations resting on sand

2021

The presence of minor details of the ground, including soil or rock masses, occurs more frequently than what is normally believed. Thin weak layers, shear bands, and slickensided surfaces can substantially affect the behaviour of foundations, as well as that of other geostructures. In fact, they can affect the failure mechanisms, the ultimate bearing capacity of footings, and the safety factor of the geotechnical system. In this research, numerically conducted through Finite Element Code Plaxis 2D, the influence of a horizontal thin weak layer on the mechanical behaviour of shallow footings was evaluated. The obtained results prove that the weak layer strongly influences both the failure me…

Bearing capacityQE1-996.5FEMSafety factorSettore ICAR/07 - GeotecnicaFoundation (engineering)GeologyWeak layerFinite element methodShear (sheet metal)Shallow foundationFailure mechanismsGeneral Earth and Planetary SciencesGeotechnical engineeringBearing capacityLayer (electronics)Shear strength (discontinuity)GeologyStrip footing
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Wave propagation in 1D elastic solids in presence of long-range central interactions

2011

Abstract In this paper wave propagation in non-local elastic solids is examined in the framework of the mechanically based non-local elasticity theory established by the author in previous papers. It is shown that such a model coincides with the well-known Kroner–Eringen integral model of non-local elasticity in unbounded domains. The appeal of the proposed model is that the mechanical boundary conditions may easily be imposed because the applied pressure at the boundaries of the solid must be equilibrated by the Cauchy stress. In fact, the long-range forces between different volume elements are modelled, in the body domain, as central body forces applied to the interacting elements. It is …

Body forceAcoustics and UltrasonicsCONTINUAWave propagationMechanical EngineeringWeak solutionMODELSElastic energyGRADIENT ELASTICITYWeak formulationElasticity (physics)Condensed Matter PhysicsWave equationMEDIANONLOCAL ELASTICITYClassical mechanicsMechanics of MaterialsBoundary value problemSettore ICAR/08 - Scienza Delle CostruzioniMathematicsJournal of Sound and Vibration
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Driven Bose-Hubbard Model with a Parametrically Modulated Harmonic Trap

2016

We investigate a one-dimensional Bose–Hubbard model in a parametrically driven global harmonic trap. The delicate interplay of both the local interaction of the atoms in the lattice and the driving of the global trap allows us to control the dynamical stability of the trapped quantum many-body state. The impact of the atomic interaction on the dynamical stability of the driven quantum many-body state is revealed in the regime of weak interaction by analyzing a discretized Gross–Pitaevskii equation within a Gaussian variational ansatz, yielding a Mathieu equation for the condensate width. The parametric resonance condition is shown to be modified by the atom interaction strength. In particul…

Bose–Hubbard modelquantum many-body systemsFOS: Physical sciencesHarmonic (mathematics)02 engineering and technologyBose–Hubbard modelWeak interaction01 natural sciencessymbols.namesakeQuantum mechanics0103 physical sciencesAtomquantum gas010306 general physicsQuantumAnsatzPhysicsCondensed Matter::Quantum Gasesta114021001 nanoscience & nanotechnologyMathieu functionQuantum Gases (cond-mat.quant-gas)symbolsParametric oscillator0210 nano-technologyCondensed Matter - Quantum Gasesharmonic trap
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Bounded and unbounded solutions for a class of quasi-linear elliptic problems with a quadratic gradient term

2001

Abstract Our aim in this article is to study the following nonlinear elliptic Dirichlet problem: − div [a(x,u)·∇u]+b(x,u,∇u)=f, in Ω; u=0, on ∂Ω; where Ω is a bounded open subset of RN, with N>2, f∈L m (Ω) . Under wide conditions on functions a and b, we prove that there exists a type of solution for this problem; this is a bounded weak solution for m>N/2, and an unbounded entropy solution for N/2>m⩾2N/(N+2). Moreover, we show when this entropy solution is a weak one and when can be taken as test function in the weak formulation. We also study the summability of the solutions.

Bounded and unbounded solutionsQuasi-linear elliptic problemsDirichlet problemMathematics(all)Pure mathematicsApplied MathematicsGeneral MathematicsWeak solutionMathematical analysisQuadratic functionWeak formulationNonlinear systemElliptic curveQuadratic equationBounded functionQuadratic gradient termMathematicsJournal de Mathématiques Pures et Appliquées
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Search for anomalous production of events with two photons and additional energetic objects at CDF

2010

27 páginas, 17 figuras, 5 tablas.-- CDF Collaboration: et al.

COLLIDER DETECTORNuclear and High Energy PhysicsParticle physicsMEDIATED SUPERSYMMETRY-BREAKINGPhysics beyond the Standard ModelP(P)OVER-BAR COLLISIONSFOS: Physical sciencesElementary particleddc:500.2GAMMA PRODUCTION114 Physical sciences01 natural sciences7. Clean energyHigh Energy Physics - ExperimentMEDIATED SUPERSYMMETRY-BREAKING; CENTRAL ELECTROMAGNETIC CALORIMETER; ELECTROWEAK SYMMETRY-BREAKING; LARGE EXTRA DIMENSIONS; P(P)OVER-BAR COLLISIONS; COLLIDER DETECTOR; GAMMA PRODUCTION; ROOT-S=1.96 TEV; QCD; PYTHIA-5.7Nuclear physicsHigh Energy Physics - Experiment (hep-ex)13.85Rm; 13.85Qk; 18.80.-j; 14.80.Ly0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PYTHIA-5.7010306 general physicsPhysicsMuonLuminosity (scattering theory)hep-ex010308 nuclear & particles physicsPhysicsLARGE EXTRA DIMENSIONSQCDCENTRAL ELECTROMAGNETIC CALORIMETERROOT-S=1.96 TEVLarge extra dimensionHigh Energy Physics::ExperimentELECTROWEAK SYMMETRY-BREAKINGCollider Detector at FermilabEvent (particle physics)Lepton
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CODEX Weak Lensing Mass Catalogue and implications on the mass-richness relation

2021

The COnstrain Dark Energy with X-ray clusters (CODEX) sample contains the largest flux limited sample of X-ray clusters at $0.35 = \alpha \mu + \beta$, with $\mu = \ln (M_{200c}/M_{\mathrm{piv}})$, and $M_{\mathrm{piv}} = 10^{14.81} M_{\odot}$. We find a slope $\alpha = 0.49^{+0.20}_{-0.15}$, normalization $ \exp(\beta) = 84.0^{+9.2}_{-14.8}$ and $\sigma_{\ln \lambda | \mu} = 0.17^{+0.13}_{-0.09}$ using CFHT richness estimates. In comparison to other weak lensing richness-mass relations, we find the normalization of the richness statistically agreeing with the normalization of other scaling relations from a broad redshift range ($0.0<z<0.65$) and with different cluster selection (X-ray, Sun…

COSMOLOGICAL CONSTRAINTSCosmology and Nongalactic Astrophysics (astro-ph.CO)FOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsLambdaPROFILE01 natural sciences114 Physical sciencesgravitational lensing: weakMAXBCGweak [gravitational lensing]0103 physical sciencesLARGE-SCALE STRUCTUREclusters: general [galaxies]PROBE010303 astronomy & astrophysicsWeak gravitational lensingGalaxy clusterLOCUSSPhysicsTEMPERATURE RELATION010308 nuclear & particles physicsAstronomy and Astrophysicsobservations [cosmology]RedshiftREDUCTIONSpace and Planetary Sciencegravitational lensing: weak; galaxies: clusters: general; cosmology: observationsgalaxies: clusters: generalcosmology: observationsGIANTSGALAXY CLUSTERS[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Astrophysics - Cosmology and Nongalactic Astrophysics
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HfF+ as a candidate to search for the nuclear weak quadrupole moment

2018

Nuclei with a quadrupole deformation, such as $^{177}\mathrm{Hf}$ have enhanced weak quadrupole moment which induces the tensor weak electron-nucleus interaction in atoms and molecules. Corresponding parity-non-conserving (PNC) effect is strongly enhanced in the ${}^{3}{\mathrm{\ensuremath{\Delta}}}_{1}$ electronic state of the $^{177}\mathrm{HfF}^{+}$ cation which has very close opposite parity levels mixed by this tensor interaction. In the present paper we perform relativistic many-body calculations of this PNC effect. It is shown that the tensor weak interaction induced by the weak quadrupole moment gives the dominating contribution to the PNC effects in $^{177}\mathrm{HfF}^{+}$ which s…

Chemical Physics (physics.chem-ph)PhysicsAtomic Physics (physics.atom-ph)Nuclear TheoryAtoms in moleculesFOS: Physical sciencesParity (physics)Weak interaction01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmasPhysics - Chemical Physics0103 physical sciencesQuadrupoleNeutronPhysics::Atomic PhysicsAtomic physics010306 general physicsPhysical Review A
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Measuring molecular parity nonconservation using nuclear-magnetic-resonance spectroscopy

2017

The weak interaction does not conserve parity and therefore induces energy shifts in chiral enantiomers that should in principle be detectable in molecular spectra. Unfortunately, the magnitude of the expected shifts are small and in spectra of a mixture of enantiomers, the energy shifts are not resolvable. We propose a nuclear magnetic resonance (NMR) experiment in which we titrate the chirality (enantiomeric excess) of a solvent and measure the diasteriomeric splitting in the spectra of a chiral solute in order to search for an anomalous offset due to parity nonconservation (PNC). We present a proof-of-principle experiment in which we search for PNC in the \textsuperscript{13}C resonances…

Chemical Physics (physics.chem-ph)PhysicsGeneral PhysicsChemical shiftphysics.chem-phFOS: Physical sciencesParity (physics)Nuclear magnetic resonance spectroscopyWeak interaction010402 general chemistry01 natural sciencesSpectral lineMathematical Sciences0104 chemical sciences3. Good healthPhysics - Chemical Physics0103 physical sciencesPhysical SciencesChemical SciencesPhysics::Atomic PhysicsAtomic physicsEnantiomer010306 general physicsEnantiomeric excessChirality (chemistry)
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