Search results for "Radiative transition"

showing 6 items of 6 documents

Search for theY(4140)viae+e−→γϕJ/ψats=4.23, 4.26 and 4.36 GeV

2015

Using data samples collected at center-of-mass energies root s = 4.23, 4.26, and 4.36 GeV with the BESIII detector operating at the BEPCII storage ring, we search for the production of the charmoniumlike state Y(4140) through a radiative transition followed by its decay to phi J/psi. No significant signal is observed and upper limits on sigma[e(+)e(-) -> gamma Y(4140)] . B(Y(4140) -> phi J/psi at the 90% confidence level are estimated as 0.35, 0.28, and 0.33 pb at root s = 4.23, 4.26, and 4.36 GeV, respectively.

PhysicsNuclear physicsNuclear and High Energy PhysicsTheoretical physicsElectron–positron annihilationRadiative transitionHigh Energy Physics::ExperimentStorage ringPhysical Review D
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Evidence forηc(2S)inψ(3686)→γKS0K±π∓π+π−

2013

We search for the M1 radiative transition psi(3686) -> gamma eta(c)(2S) by reconstructing the exclusive eta(c)(2S) -> (KSK +/-)-K-0 pi(-/+)pi(+)pi(-) decay using 1.06 X 10(8) psi(3686) events collected with the BESIII detector. The signal is observed with a statistical significance of greater than 4 standard deviations. The measured mass of the eta(c)(2S) is 3646.9 +/- 1.6(stat) +/- 3.6(syst) MeV/c(2), and the width is 9.9 +/- 4.8(stat) +/- 2.9(syst) MeV/c(2). The product branching fraction is measured to be B(psi(3686) -> gamma eta(c)(2S)) X B(eta(c)(2S) -> gamma(KSK +/-)-K-0 pi(-/+)pi(+)pi(-) = (7.03 +/- 2.10(stat) +/- 0.70(syst)) X 10(-6). This measurement complements a previous BESIII m…

PhysicsNuclear and High Energy PhysicsNuclear magnetic resonanceBranching fractionElectron–positron annihilationPiAnalytical chemistryRadiative transitionHigh Energy Physics::ExperimentNuclear ExperimentPhysical Review D
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XYZ physics at BESIII

2014

In this talk, we present the recent study on the charmonium-like states from the BESIII Collaboration based on large data samples above DD¯$D\overline D $ threshold. The observation of X(3872) from the Y(4260) radiative transition, the study of the Y states from the e+e− → π+π−hc process, and the observation of the charged Zc states are included.

Nuclear physicsPhysicsParticle physicsPhysicsQC1-999Radiative transitionX(3872)EPJ Web of Conferences
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Mechanisms of Strong Photoluminescence from Si Nanocrystals

2011

Photoluminescence mechanisms (models) are reviewed and experimental data are analyzed based on our model, related to direct radiative transitions from the second conduction sub-band to the first one.

Materials sciencePhotoluminescenceAuger effectbusiness.industryGeneral EngineeringPorous siliconThermal conductionsymbols.namesakeNanocrystalsymbolsRadiative transferOptoelectronicsRadiative transitionPhotoluminescence excitationbusinessAdvanced Materials Research
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Optical transitions and excitonic recombination in InAs/InP self-assembled quantum wires

2001

InAs self-assembled quantum wire structures have been grown on InP substrates and studied by means of photoluminescence and polarized-light absorption measurements. According to our calculations, the observed optical transitions in each sample are consistent with wires of different heights, namely from 6 to 13 monolayers. The nonradiative mechanism limiting the emission intensity at room temperature is related to thermal escape of carriers out of the wires.

PhotoluminescenceIII-V semiconductorsPhysics and Astronomy (miscellaneous)ExcitonCondensed Matter::Materials ScienceIndium compoundsMonolayerLight absorptionAbsorption (electromagnetic radiation)QuantumPhotoluminescencePhysicsAtmospheric escapebusiness.industryQuantum wireSelf-assemblyInterface statesCondensed Matter::Mesoscopic Systems and Quantum Hall EffectLight polarisationSemiconductor quantum wiresOptoelectronicsExcitonsSelf-assemblyNonradiative transitionsbusiness
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Observation ofe+e−→γX(3872)at BESIII

2014

Using data collected with the BESIII detector operating at the Beijing Electron Positron Collider at center-of-mass energies of root s = 4.23, 4.26, and 4.36 GeV, we observe e(+)e(-) -> pi(0)pi(0)h(c) for the first time. The Born cross sections are measured and found to be about half of those of e(+)e(-) -> pi(+)pi(-)h(c) within less than 2 sigma. In the pi(0)h(c) mass spectrum, a structure at 4.02 GeV/c(2) is found. It is most likely to be the neutral isospin partner of the Z(c)(4020)(+/-) observed in the process of e(+)e(-) -> pi(+)pi(-)h(c) being found. A fit to the pi(0)h(c) invariant mass spectrum, with the width of the Z(c)(4020)(0) fixed to that of its charged isospin partner and pos…

Physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationAnalytical chemistryGeneral Physics and AstronomySigmaElectronMass spectrometry01 natural sciencesNuclear physicsPositronIsospin0103 physical sciencesPiMass spectrumRadiative transitionHigh Energy Physics::ExperimentInvariant massCenter of massAtomic physicsNuclear Experiment010306 general physicsStorage ringPhysical Review Letters
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