Search results for "Sect"

showing 10 items of 10622 documents

"Table 4" of "Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2020

Inclusive $e^+e^-$ cross section in p-Pb collisions at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $0.5 < m_{\rm ee} < 1.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

5020.0P PB --> E+ E- XDSIG/DPTEEDielectron cross section
researchProduct

"Table 12" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.0…

2021

Interpolated $p_{\mathrm{T}}$-differential cross section for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of its transverse momentum (Figure 6).

5020.0Proton-Proton ScatteringP P --> UPSI(1S) < MU+ MU- > XD2SIG/DYRAP/DPTNuclear TheoryHigh Energy Physics::ExperimentUpsilonCross SectionNuclear ExperimentTransverse Momentum Dependence
researchProduct

"Table 13" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.0…

2021

Interpolated rapidity-differential cross section for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of rapidity (Figure 7).

5020.0Proton-Proton ScatteringP P --> UPSI(1S) < MU+ MU- > XRapidity DependenceNuclear TheoryHigh Energy Physics::ExperimentUpsilonDSIG/DYRAPCross SectionNuclear Experiment
researchProduct

"Table 14" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.0…

2021

Interpolated rapidity-differential cross section for $\Upsilon(2\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(2\mathrm{S})$ as a function of rapidity (Figure 7).

5020.0Proton-Proton ScatteringP P --> UPSI(2S) < MU+ MU- > XRapidity DependenceNuclear TheoryHigh Energy Physics::ExperimentUpsilonDSIG/DYRAPCross SectionNuclear Experiment
researchProduct

"Table 11" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.0…

2021

Interpolated production cross sections and cross-section ratio for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ and $\Upsilon(2\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions, integrated over the rapidity interval 2.5–4.0 and $p_{\mathrm{T}} <$ 15 GeV/$c$. Results used for the determination of the integrated nuclear modification factors and of the nuclear modification factors as a function of centrality (Figures 4 and 5 (right)).

5020.0RATIOProton-Proton ScatteringP P --> UPSI(1S) < MU+ MU- > XP P --> UPSI(2S) < MU+ MU- > XHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentUpsilonNuclear ExperimentSIG
researchProduct

"Table 6" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

2014

Forward to backward ratio RFB of inclusive UPSI(1S) yields in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.

5020.0SIG/SIGIntegrated Cross SectionCross Section
researchProduct

"Table 7" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

2014

Ratios of the cross sections of UPSI(2S)->MU+MU- to UPSI(1S)->MU+MU- in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.

5020.0SIG/SIGIntegrated Cross SectionCross Section
researchProduct

"Table 1" of "First measurement of the ${\mathbf{|\textit t|}}$-dependence of coherent $\mathbf{\rm{J/\psi}}$ photonuclear production"

2021

t-dependence of coherent J/psi photonuclear production cross section in Pb-Pb UPC.

5020.0Single Differential Cross SectionDi-Muon ProductionPhotoproductionPhysics::Medical PhysicsNuclear TheoryDSIG/DTMomentum Transfer DependenceHigh Energy Physics::ExperimentPB PB --> PB PB J/PSI(1S)Nuclear ExperimentJ/Psi
researchProduct

"Table 1" of "Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}…

2020

HFe cross section in pp

5023.01/(Nev*2*PI*PT)*D2(N)/DPT/DYRAPSemileptonic Heavy-Flavour Hadron DecaysCross Section
researchProduct

Gap perception in bumblebees

2018

ABSTRACT A number of insects fly over long distances below the natural canopy, where the physical environment is highly cluttered consisting of obstacles of varying shape, size and texture. While navigating within such environments, animals need to perceive and disambiguate environmental features that might obstruct their flight. The most elemental aspect of aerial navigation through such environments is gap identification and ‘passability’ evaluation. We used bumblebees to seek insights into the mechanisms used for gap identification when confronted with an obstacle in their flight path and behavioral compensations employed to assess gap properties. Initially, bumblebee foragers were train…

570PhysiologyAcousticsmedia_common.quotation_subjectOptic FlowAquatic Science03 medical and health sciences0302 clinical medicineSalience (neuroscience)PerceptionAnimalsMolecular BiologyEcology Evolution Behavior and Systematics030304 developmental biologymedia_common0303 health sciencesSensorimotor systemBeesLateral displacementLateral velocityFlight AnimalInsect ScienceObstacleAnimal Science and Zoology030217 neurology & neurosurgeryGeology
researchProduct