Search results for "Hadrons"

showing 10 items of 502 documents

Alma Mater

2015

Jauno mūzikas grupu konkurss studentiem «Hadrons» – platforma jauniešiem ceļā uz lielo skatuviERASMUS+ prakses iespējas studentiemzinātnē viens nav karotājs [Neirozinātniece Inga Kadiša]Mālu mīcīšana 40 gadu garumāNākotnes materiāli. Epoksīda sveķu uzlabošana ar oglekļa nanopildvielāmRakstīt ir tikpat dabiski kā ēst gulēt un mazgātiessaules enerģija jaunajiem izgudrotājiem [«Saules kauss 2015»]Studiju programmas Latvijas Universitātē 2015./2016. akadēmiskajā gadārektora stāsts [Latvijas Universitāte – kad globālais satiekas ar lokālo]«Mans hobijs ir cilvēki» [Mateo Frejs no Šveices]
researchProduct

Alma Mater: 2013/ Vasara

2013

Jauno mūzikas grupu konkurss «Hadrons 2013»Fizikas un matemātikas fakultātes jauktais koris "Aura"Latvijas Universitātes Botāniskais dārzsProfesors Viktors FreibergsKaspars AdijānsProjekts «Atbalsts Latvijas Universitātes starptautiskās sadarbības projektiem un citiem starptautiskās sadarbības pasākumiem zinātnē un tehnoloģijās»Studiju kvalitāte -- Latvijas UniversitāteDiriģents Edgars VītolsLatvijas Universitātes basketbola komandaLatvijas Universitātes Studentu padome -- Projektu konkursiStarptautiskais kognitīvo zinātņu loģikas un komunikācijas simpozijs «Uztvere un koncepti»Aktuālie notikumi Latvijas UniversitātēCouple Learning programme
researchProduct

Differential branching fraction and angular analysis of the decay $B^{0} \to K^{*0} \mu^{+}\mu^{-}$

2013

The angular distribution and differential branching fraction of the decay B-0 -> K*(0)mu(+)mu(-) are studied using a data sample, collected by the LHCb experiment in pp collisions at root s = 7 TeV, corresponding to an integrated luminosity of 1.0 fb(-1). Several angular observables are measured in bins of the dimuon invariant mass squared, q(2). A first measurement of the zero-crossing point of the forward-backward asymmetry of the dimuon system is also presented. The zero-crossing point is measured to be q(0)(2) = 4.9 +/- 0.9 GeV2/c(4), where the uncertainty is the sum of statistical and systematic uncertainties. The results are consistent with the Standard Model predictions.

K-ASTERISK-L(+)L(-)12.15.Mm01 natural sciencesB physicsLuminositydecayHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNeutral currentFlavor physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massQCDetectors de radiaciómedia_commonPhysicsB0 mesonHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronObservableCP violationFIS/01 - FISICA SPERIMENTALENuclear countersLeptonic semileptonic and radiative decays of bottom mesonsFísica nuclearLHCB physics; Flavor physics; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decayParticle Physics - ExperimentParticle physicsNuclear and High Energy Physicsmedia_common.quotation_subject14.40.NdFlavour Changing Neutral CurrentsHadronsAsymmetryPartícules (Física nuclear)Standard ModelB physics; Flavor physics; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decay; Nuclear and High Energy PhysicsNeutral currentsAngular distributionASYMMETRIES0103 physical sciencesLeptonic semileptonic and radiative decays of bottom mesonLHC flavour physics010306 general physicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronsB0 meson; decay; LHCb; LHCHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionCromodinàmica quànticaLHCbRare decay13.20.HeBottom mesons (|B|>0); Leptonic semileptonic and radiative decays of bottom mesons; Hadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadrons; Neutral currents; 14.40.Nd; 13.20.He; 13.85.Ni; 12.15.Mm;Bottom mesons (|B|>0)High Energy Physics::Experiment13.85.NiDifferential (mathematics)FIS/04 - FISICA NUCLEARE E SUBNUCLEAREQuantum chromodynamicsexperimental results
researchProduct

"Table 3" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Moments of the Thrust Minor distributions at cm energies 133, 161, 172 and 183 GeV.

MINOR133.0-183.0E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringExclusiveVARIANCENAME=MINORJet ProductionSKEWNESSNAME=MINOR
researchProduct

"Table 28" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distribution of the Heavy Jet Masses (MH**2/EVIS**2) at cm energy 183 GeV.

Mathematics::ProbabilityDN/DMHEAVY-JETAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentSingle Differential DistributionJet ProductionNuclear Experiment183.0
researchProduct

"Table 30" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distribution of the Light Jet Masses (ML**2/EVIS**2) at cm energy 183 GeV.

Mathematics::ProbabilityDN/DMLIGHT-JETAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentSingle Differential DistributionJet ProductionNuclear Experiment183.0
researchProduct

Complete Measurement of the Λ Electromagnetic Form Factors.

2019

The exclusive process e+e−→ΛΛ¯, with Λ→pπ− and Λ¯→p¯π+, has been studied at s=2.396 GeV for measurement of the timelike Λ electric and magnetic form factors, GE and GM. A data sample, corresponding to an integrated luminosity of 66.9 pb−1, was collected with the BESIII detector for this purpose. A multidimensional analysis with a complete decomposition of the spin structure of the reaction enables a determination of the modulus of the ratio R=|GE/GM| and, for the first time for any baryon, the relative phase ΔΦ=ΦE−ΦM. The resulting values are R=0.96±0.14(stat)±0.02(syst) and ΔΦ=37°±12°(stat)±6°(syst), respectively. These are obtained using the recently established and most precise value of …

Multi-dimensional analysisElectron–positron annihilationRelative phaseHadronAnalytical chemistryGeneral Physics and AstronomyHadronsOBSERVABLESLambdaBaryon01 natural sciencesArticleNOHigh Energy Physics - ExperimentSubatomär fysikGermanium compoundsElectromagnetic form factorsSubatomic Physics0103 physical sciencesMagnetic form factorTwo-photon exchangePiddc:530010306 general physicsAsymmetry parameterProton Scattering; Nucleons; HydrogenPhysicsIntegrated luminosityDecompositionPhysicsHigh Energy Physics::PhenomenologyApproximation theoryPhysics multidisciplinaryPhotonHigh Energy Physics - Experiment; High Energy Physics - ExperimentBaryonLuminanceSpin structuresHigh Energy Physics::ExperimentMagnetic form factorMulti dimensional analysisBar (unit)Physical review letters
researchProduct

Direct X(3872) production in e+e- collisions

2014

Direct production of the charmonium-like state $X(3872)$ in $e^+e^-$ collisions is considered in the framework of the vector meson dominance model. An order-of-magnitude estimate for the width $\Gamma(X\to e^+e^-)$ is found to be $\gtrsim$0.03 eV. The same approach applied to the $\chi_{c1}$ charmonium decay predicts the corresponding width of the order 0.1 eV in agreement with earlier estimates. Experimental perspectives for the direct production of the $1^{++}$ charmonia in $e^+e^-$ collisions are briefly discussed.

Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Nuclear TheoryExotic hadronsFOS: Physical sciencesHigh Energy Physics::Experimentddc:530Charmoniumlcsh:Physicslcsh:QC1-999High Energy Physics - Experiment
researchProduct

Precision Measurement of the Mass and Lifetime of the Ξ[0 over b] Baryon

2014

Using a proton-proton collision data sample corresponding to an integrated luminosity of 3 fb$^{-1}$ collected by LHCb at center-of-mass energies of 7 and 8 TeV, about 3800 $\Xi_b^0\to\Xi_c^+\pi^-$, $\Xi_c^+\to pK^-\pi^+$ signal decays are reconstructed. From this sample, the first measurement of the $\Xi_b^0$ baryon lifetime is made, relative to that of the $\Lambda_b^0$ baryon. The mass differences $M(\Xi_b^0)-M(\Lambda_b^0)$ and $M(\Xi_c^+)-M(\Lambda_c^+)$ are also measured with precision more than four times better than the current world averages. The resulting values are $\frac{\tau_{\Xi_b^0}}{\tau_{\Lambda_b^0}} = 1.006\pm0.018\pm0.010$, $M(\Xi_b^0) - M(\Lambda_b^0) = 172.44\pm0.39\pm…

Nuclear TheoryAnalytical chemistryGeneral Physics and Astronomyinclusive weak decays; discarding 1/N(C); beaty; charm; ruleLambdaHigh Energy Physics - Experimenthigh energy physicsSettore FIS/04 - Fisica Nucleare e Subnucleare[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]INCLUSIVE WEAK DECAYS; DISCARDING 1/N(C); BEAUTY; CHARM; RULENuclear ExperimentQCPhysicsprecision measurementPhysicsintegrated luminosityParticle physicsBEAUTYtransverse momentaPseudorapidityPhysical SciencesTransverse momentumINCLUSIVE WEAK DECAYSFísica nuclearLHC13.30.Egtellurium compoundsParticle Physics - Experiment530 PhysicsAstrophysics::High Energy Astrophysical PhenomenaPhysics MultidisciplinarypseudorapiditiesPhysics InstituteLHCb - Abteilung HofmannAstrophysics::Cosmology and Extragalactic AstrophysicsCHARMNuclear physicsPhysics and Astronomy (all)Pi14.20.MrScience & Technologycenter-of-mass energiesmass differencetransverse momenta; precision measurement; center-of-mass energies; tellurium compounds; production rates; pseudorapidities; high energy physics; integrated luminosity; hadrons; mass difference; proton proton collisionsDISCARDING 1/N(C)BaryonLHCbproton proton collisionshadronsHadronic decays of baryonBottom baryons (|B|>0)Physics::Accelerator Physicsproduction ratesFísica de partículesExperimentsRULE
researchProduct

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
researchProduct