Search results for "lower bound"

showing 10 items of 269 documents

Quantum benchmark for teleportation and storage of squeezed states.

2007

We provide a quantum benchmark for teleportation and storage of single-mode squeezed states with zero displacement and a completely unknown degree of squeezing along a given direction. For pure squeezed input states, a fidelity higher than 81.5% has to be attained in order to outperform any classical strategy based on an estimation of the unknown squeezing and repreparation of squeezed states. For squeezed thermal input states, we derive an upper and a lower bound on the classical average fidelity which tighten for moderate degree of mixedness. These results enable a critical discussion of recent experiments with squeezed light.

PhysicsCondensed Matter::Quantum GasesQuantum Physicsmedia_common.quotation_subjectGeneral Physics and AstronomyFidelityFOS: Physical sciencesQuantum PhysicsUpper and lower boundsTeleportationDisplacement (vector)Quantum mechanicsBenchmark (computing)Quantum information scienceQuantum Physics (quant-ph)QuantumSqueezed coherent statemedia_commonPhysical review letters
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Mass relations in noncommutative geometry revisited

1997

We generalize the notion of the 'noncommutative coupling constant' given by Kastler and Sch"ucker by dropping the constraint that it commute with the Dirac-operator. This leads essentially to the vanishing of the lower bound for the Higgsmass and of the upper bound for the W-mass.

PhysicsCoupling constantConstraint (information theory)High Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics - Theory (hep-th)Mathematics::Operator AlgebrasFOS: Physical sciencesUpper and lower boundsNoncommutative geometryMathematical physics
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Transition behavior in the channel capacity of two-quibit channels with memory

2004

We prove that a general upper bound on the maximal mutual information of quantum channels is saturated in the case of Pauli channels with an arbitrary degree of memory. For a subset of such channels we explicitly identify the optimal signal states. We show analytically that for such a class of channels entangled states are indeed optimal above a given memory threshold.

PhysicsData_CODINGANDINFORMATIONTHEORYCoherent informationQuantum channelQuantum capacityTopologyUpper and lower boundsAtomic and Molecular Physics and OpticsClassical capacityQuantum mechanicsQuantum informationAmplitude damping channelQuantum mutual informationComputer Science::Information Theory
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Electroweak precision data and right-handed gauge bosons

1998

The implication of recent electroweak precision data for left-right symmetric models is examined. We establish a lower bound on the charged and neutral right-handed gauge bosons independent of the right-handed neutrino mass and of any restrictions or implied symmetries on the right KM matrix.

PhysicsGauge bosonParticle physicsPhysics and Astronomy (miscellaneous)Right handedCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyElectroweak interactionTechnicolorUpper and lower boundsQuantum electrodynamicsHomogeneous spaceNeutrinoEngineering (miscellaneous)The European Physical Journal C
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Minimal mass size of a stable He-3 cluster

2005

The minimal number of 3He atoms required to form a bound cluster has been estimated by means of a Diffusion Monte Carlo procedure within the fixed-node approximation. Several importance sampling wave functions have been employed in order to consider different shell-model configurations. The resulting upper bound for the minimal number is 32 atoms.

PhysicsMonte Carlo methodFOS: Physical sciencesFísicaUpper and lower boundsAtomic and Molecular Physics and OpticsDynamic Monte Carlo methodCluster (physics)Monte Carlo integrationDiffusion Monte CarloStatistical physicsPhysics - Atomic and Molecular ClustersWave functionAtomic and Molecular Clusters (physics.atm-clus)Importance sampling
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Longitudinal and azimuthal evolution of two-particle transverse momentum correlations in Pb–Pb collisions at sNN=2.76TeV

2020

This paper presents the first measurements of the charge independent (CI) and charge dependent (CD) two-particle transverse momentum correlators G2CI and G2CD in Pb–Pb collisions at sNN=2.76TeV by the ALICE collaboration. The two-particle transverse momentum correlator G2 was introduced as a measure of the momentum current transfer between neighboring system cells. The correlators are measured as a function of pair separation in pseudorapidity (Δη) and azimuth (Δφ) and as a function of collision centrality. From peripheral to central collisions, the correlator G2CI exhibits a longitudinal broadening while undergoing a monotonic azimuthal narrowing. By contrast, G2CD exhibits a narrowing alo…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsCharge (physics)01 natural sciencesUpper and lower boundsNuclear physicsMomentumAzimuthTransverse planePseudorapidity0103 physical sciencesRapidityImpact parameterNuclear Experiment010306 general physicsPhysics Letters B
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Search for the Higgs boson in the H→WW→ℓνjj decay channel at s=7 TeV with the ATLAS detector

2012

A search for the Standard Model Higgs boson has been performed in the H→WW→lνjj channel using 4.7 fb^(−1) of pp collision data recorded at a centre-of-mass energy of √s = 7 TeV with the ATLAS detector at the Large Hadron Collider. Higgs boson candidates produced in association with zero, one or two jets are included in the analysis to maximize the acceptance for both gluon fusion and weak boson fusion Higgs boson production processes. No significant excess of events is observed over the expected background and limits on the Higgs boson production cross section are derived for a Higgs boson mass in the range 300 GeV<m_H<600 GeV. The best sensitivity is reached for m_H=400 GeV, where the obse…

PhysicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology7. Clean energy01 natural sciencesUpper and lower boundsSearch for the Higgs bosonStandard ModelGluonNuclear physicsmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesHiggs bosonmedicineHigh Energy Physics::Experiment010306 general physicsBosonPhysics Letters B
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Probing new physics by comparing solar and KamLAND data

2004

We explore whether KamLAND and solar data may end up inconsistent when analyzed in terms of two-flavor neutrino oscillations. If this turned out to be the case, one would be led to conclude that there is more new physics, besides neutrino masses and mixing, in the leptonic sector. On the other hand, given that KamLAND and solar data currently agree when analyzed in terms of two-flavor neutrino oscillations, one is able to place nontrivial bounds on several manifestations of new physics. In particular, we compute how well a combined KamLAND and solar data analysis is able to constrain a specific form of violation of CPT invariance by placing a very stringent upper bound, |Delta m^2 - Delta b…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCPT symmetryPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaWeinberg angleParameter space01 natural sciencesUpper and lower boundsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesInvariant massHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillation
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Hefty MSSM-like light Higgs in extended gauge models

2011

It is well known that in the MSSM the lightest neutral Higgs h^0 must be, at the tree level, lighter than the Z boson and that the loop corrections shift this stringent upper bound up to about 130 GeV. Extending the MSSM gauge group in a suitable way, the new Higgs sector dynamics can push the tree-level mass of h^0 well above the tree-level MSSM limit if it couples to the new gauge sector. This effect is further pronounced at the loop level and h^0 masses in the 140 GeV ballpark can be reached easily. We exemplify this for a sample setting with a low-scale U(1)_R x U(1)_B-L gauge symmetry in which neutrino masses can be implemented via the inverse seesaw mechanism.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGauge (firearms)01 natural sciencesUpper and lower boundsHiggs sectorHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Gauge group0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsGauge symmetry
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Current cosmological bounds on neutrino masses and relativistic relics

2004

We combine the most recent observations of large-scale structure (2dF and SDSS galaxy surveys) and cosmic microwave anisotropies (WMAP and ACBAR) to put constraints on flat cosmological models where the number of massive neutrinos and of massless relativistic relics are both left arbitrary. We discuss the impact of each dataset and of various priors on our bounds. For the standard case of three thermalized neutrinos, we find an upper bound on the total neutrino mass sum m_nu &lt; 1.0 (resp. 0.6) eV (at 2sigma), using only CMB and LSS data (resp. including priors from supernovae data and the HST Key Project), a bound that is quite insensitive to the splitting of the total mass between the th…

PhysicsNuclear and High Energy PhysicsParticle physicsCosmic microwave backgroundDark matterAstrophysics (astro-ph)FOS: Physical sciencesFísicaAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsUpper and lower boundsCMB cold spotMassless particleHigh Energy Physics - PhenomenologySupernovaHigh Energy Physics - Phenomenology (hep-ph)Observational cosmologyNeutrino
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