Search results for "decay [muon]"

showing 10 items of 31 documents

Steam catalytic cracking of naphtha over ZSM-5 zeolite for production of propene and ethene: Micro and macroscopic implications of the presence of st…

2012

One option to produce more ethene and propene can be to crack naphtha type fractions in dedicated smaller FCC units. We present here the results obtained for high temperature steam catalytic cracking (SCC) of a representative naphtha product (n-heptane) with ZSM-5. It has been found that under those conditions the presence of steam produces an irreversible dealumination of the zeolite as well as a reversible deactivation due to the interaction of water with active sites with a negative effect on protolytic cracking. A kinetic decay model that takes into account the two phenomena has been developed. The apparent activation energy is lower in the presence of steam. It appears that whilst the …

Fluid catalytic crackingcomplex mixturesCatalysisCatalysisPropenechemistry.chemical_compoundEthyleneSteam crackingQUIMICA ORGANICAFCC unitsFluid catalytic crackingOrganic chemistryN-HeptanesZeoliteNaphthaTECNOLOGIA DEL MEDIO AMBIENTEFluid catalytic cracking unitHeptaneApparent activation energyDecay modelPropene selectivityProcess Chemistry and TechnologyActive sitefood and beveragesCokeHigh temperatureNaphthashumanitiesCrackingSteamZSM-5 zeoliteschemistryChemical engineeringPropyleneDispersion (chemistry)Coke precursorsDealumination
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Correlation at low temperature I. Exponential decay

2003

Abstract The present paper generalizes the analysis in (Ann. H. Poincare 1 (2000) 59, Math. J. (AMS) 8 (1997) 123) of the correlations for a lattice system of real-valued spins at low temperature. The Gibbs measure is assumed to be generated by a fairly general Hamiltonian function with pair interaction. The novelty, as compared to [2,20], is that the single-site (self-) energies of the spins are not required to have only a single local minimum and no other extrema. Our derivation of exponential decay of correlations goes through the spectral analysis of a deformed Laplacian closely related to the Witten Laplacian studied in [2,20]. We prove that this Laplacian has a spectral gap above zero…

Hamiltonian mechanicsExponential decay of correlationsSpinsZero (complex analysis)Lattice spin systemsGibbs measuresymbols.namesakeExponential growthQuantum mechanicssymbolsSpectral gapWitten LaplacianGibbs measureExponential decayLaplace operatorAnalysisMathematics
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Counting common perpendicular arcs in negative curvature

2013

Let $D^-$ and $D^+$ be properly immersed closed locally convex subsets of a Riemannian manifold with pinched negative sectional curvature. Using mixing properties of the geodesic flow, we give an asymptotic formula as $t\to+\infty$ for the number of common perpendiculars of length at most $t$ from $D^-$ to $D^+$, counted with multiplicities, and we prove the equidistribution in the outer and inner unit normal bundles of $D^-$ and $D^+$ of the tangent vectors at the endpoints of the common perpendiculars. When the manifold is compact with exponential decay of correlations or arithmetic with finite volume, we give an error term for the asymptotic. As an application, we give an asymptotic form…

Mathematics - Differential GeometryGeneral Mathematics[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]37D40 37A25 53C22 30F4001 natural sciencesDomain (mathematical analysis)Bowen-Margulis measurecommon perpendicularequidistributiondecay of correlation0502 economics and businessortholength spectrummixingAsymptotic formulaSectional curvatureTangent vectorMathematics - Dynamical Systems0101 mathematicsExponential decayskinning measurelaskeminenMathematicsconvexityApplied Mathematicsta111010102 general mathematics05 social sciencesMathematical analysisRegular polygonnegative curvatureRiemannian manifoldGibbs measureManifoldKleinian groups[MATH.MATH-DG]Mathematics [math]/Differential Geometry [math.DG]countingMathematics::Differential Geometrygeodesic arc050203 business & management
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Spectroscopy, lifetime and decay modes of the $T^-_{bb}$ tetraquark

2019

We present the first full-fledged study of the flavor-exotic isoscalar $T_{bb}^-\equiv b b \bar u \bar d$ tetraquark with spin and parity $J^P=1^+$. We report accurate solutions of the four-body problem in a quark model, characterizing the structure of the state as a function of the ratio $M_Q/m_q$ of the heavy to light quark masses. For such a standard constituent model, $T_{bb}^-$ lies approximately 150 MeV below the strong decay threshold $B^-\bar {B^*}^{0}$ and 105 MeV below the electromagnetic decay threshold $B^- \bar B^0 \gamma$. We evaluate the lifetime of $T_{bb}^-$, identifying the promising decay modes where the tetraquark might be looked for in future experiments. Its total deca…

Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesspinHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)multiquarkisoscalarquantum chromodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]structureconstituentlifetimequark modelhadron spectroscopyHigh Energy Physics::Phenomenologysemileptonic decayMULTIQUARK HADRONSquark: massHigh Energy Physics - PhenomenologySTATESparitytetraquark: decay modes[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimenttetraquark: wave function
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Determining Sneutrino Masses and Physical Implications

2005

In some areas of supersymmetry parameter space, sneutrinos are lighter than the charginos and the next-to-lightest neutralino, and they decay into the invisible neutrino plus lightest-neutralino channel with probability one. In such a scenario they can be searched for in decays of charginos that are pair-produced in e+e- collisions, and in associated sneutrino-chargino production in photon-electron collisions. The sneutrino properties can be determined with high accuracy from the edges of the decay energy spectra in the first case and from threshold scans in the second. In the final part of the report we investigate the mass difference of sneutrinos and charged sleptons between the third an…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesannihilation [electron positron]decay modes [chargino]SO(10) [grand unified theory]Nuclear physicsParticle decayHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrypair production [chargino]interaction [photon electron]Invariant massddc:530numerical calculationsPhysicsmass difference [slepton]High Energy Physics::PhenomenologySuperpartnerSupersymmetryboundary conditionseesaw modelHigh Energy Physics - PhenomenologyPair productionNeutralino(4lepton 2sneutrino) [final state]width [chargino]branching ratio [chargino]High Energy Physics::Experimentassociated production [sneutrino]Neutrinomass spectrum [sneutrino]
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Study of the f(2)(1270) , f(2)'(1525) , f(0)(1370) and f(0)(1710) in the J/psi radiative decays

2009

In this paper we present an approach to study the radiative decay modes of the J/psi into a photon and one of the tensor mesons f (2)(1270) , f' (2)(1525) , as well as the scalar ones f (0)(1370) and f (0)(1710) . Especially, we compare predictions that emerge from a scheme where the states appear dynamically in the solution of vector meson-vector meson scattering amplitudes to those from a (admittedly naive) quark model. We provide evidence that it might be possible to distinguish amongst the two scenarios, once improved data are available.

Nuclear and High Energy PhysicsParticle physicsPhotonMesonScalar (mathematics)Radiative decayhadronic decay [J/psi(3100)]01 natural sciencesf0(1710)bound state [vector meson]radiative decay [J/psi(3100)]0103 physical sciencesRadiative transferddc:530f0(1370)Tensor010306 general physicsnumerical calculationsdecay modes [J/psi(3100)]Physicsquark modelf2(1525)ratio [width]010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyQuark modelFísicascalar meson3. Good healthScattering amplitudef2(1270)tensor mesonHigh Energy Physics - Phenomenologywidth [J/psi(3100)]High Energy Physics::Experiment
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"Table 1.3" of "Production of muons from heavy-flavour hadron decays at high transverse momentum in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ and …

2021

$p_{\rm T}$-differential yield of muons from heavy-flavour hadron decays at forward rapidity ($2.5 < y < 4$) for central (0--10%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV.

PB PB --> MUON X1/NEV DN/DPT/DY OF HEAVY FLAVOUR DECAY MUONS2760High Energy Physics::PhenomenologyHigh Energy Physics::ExperimentNuclear Experiment
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"Table 1.2" of "Production of muons from heavy-flavour hadron decays at high transverse momentum in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ and …

2021

$p_{\rm T}$-differential yield of muons from heavy-flavour hadron decays at forward rapidity ($2.5 < y < 4$) for peripheral (60--80%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV.

PB PB --> MUON X1/NEV DN/DPT/DY OF HEAVY FLAVOUR DECAY MUONSHigh Energy Physics::Phenomenology5020High Energy Physics::ExperimentNuclear Experiment
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"Table 1.1" of "Production of muons from heavy-flavour hadron decays at high transverse momentum in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ and …

2021

$p_{\rm T}$-differential yield of muons from heavy-flavour hadron decays at forward rapidity ($2.5 < y < 4$) for central (0--10%) and semi-central (20--40%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV.

PB PB --> MUON X1/NEV DN/DPT/DY OF HEAVY FLAVOUR DECAY MUONSHigh Energy Physics::Phenomenology5020High Energy Physics::ExperimentNuclear Experiment
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"Table 20" of "Elliptic flow of muons from heavy-flavour hadron decays at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV"

2015

Elliptic flow of muons from heavy-flavour hadron decays as a function of the collision centrality extracted with two-particle cumulants method.

PB PB --> MUON XInclusive2760.0High Energy Physics::PhenomenologyHigh Energy Physics::ExperimentV2{2} OF HEAVY FLAVOUR DECAY MUONS vs. CENTNuclear ExperimentMuon production
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