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showing 10 items of 7176 documents

Layer-Specific Refinement of Sensory Coding in Developing Mouse Barrel Cortex

2017

Rodent rhythmic whisking behavior matures during a critical period around 2 weeks after birth. The functional adaptations of neocortical circuitry during this developmental period remain poorly understood. Here, we characterized stimulus-evoked neuronal activity across all layers of mouse barrel cortex before, during, and after the onset of whisking behavior. Employing multi-electrode recordings and 2-photon calcium imaging in anesthetized mice, we tested responses to rostro-caudal whisker deflections, axial "tapping" stimuli, and their combination from postnatal day 10 (P10) to P28. Within this period, whisker-evoked activity of neurons displayed a general decrease in layer 2/3 (L2/3) and …

2805 Cognitive NeuroscienceMale0301 basic medicineNeurogenesisCognitive NeurosciencePeriod (gene)2804 Cellular and Molecular Neuroscience610 Medicine & healthSensory systemStimulationBiologySomatosensory system03 medical and health sciencesCellular and Molecular Neuroscience0302 clinical medicineCalcium imagingPhysical StimulationAnimalsPremovement neuronal activityNeuronsAfferent PathwaysNeuronal Plasticity10242 Brain Research InstituteWhisking in animalsSomatosensory CortexBarrel cortexMice Inbred C57BL030104 developmental biologyAnimals NewbornVibrissae570 Life sciences; biologyFemaleSensory DeprivationNeuroscience030217 neurology & neurosurgery
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"Table 12: Cross-section limits lepton specific tanb 1" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the lepton specific, tanbeta 1, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For lepton specific only gluon-gluon fusion is used and the nb=2 category only.

2HDMHIGGS --> BQ BQBAR13000.0CLSHigh Energy Physics::Phenomenologycross section limitsZ0 --> MU+ MU-Z0 --> E+ E-P P --> HIGGSgluon-gluon fusionHigh Energy Physics::ExperimentHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 14: Cross-section limits lepton specific tanb 3" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the lepton specific, tanbeta 3, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For lepton specific only gluon-gluon fusion is used and the nb=2 category only.

2HDMHIGGS --> BQ BQBAR13000.0CLSHigh Energy Physics::Phenomenologycross section limitsZ0 --> MU+ MU-Z0 --> E+ E-P P --> HIGGSgluon-gluon fusionHigh Energy Physics::ExperimentHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 13: Cross-section limits lepton specific tanb 2" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the lepton specific, tanbeta 2, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For lepton specific only gluon-gluon fusion is used and the nb=2 category only.

2HDMHIGGS --> BQ BQBAR13000.0CLSHigh Energy Physics::Phenomenologycross section limitsZ0 --> MU+ MU-Z0 --> E+ E-P P --> HIGGSgluon-gluon fusionHigh Energy Physics::ExperimentHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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UAV and GPR Data Integration in Glacier Geometry Reconstruction: A Case Study from Irenebreen, Svalbard

2022

Although measurements of thickness and internal structure of glaciers are substantial for the understanding of their evolution and response to climate change, detailed data about polythermal glaciers, are scarce. Here, we present the first ground-penetrating radar (GPR) measurement data of Irenebreen, and high-resolution DEM and orthomosaic, obtained from unmanned aerial vehicle (UAV) photogrammetry. A combination of GPR and UAV data allowed for the reconstruction of the glacier geometry including thermal structure. We compare different methods of GPR signal propagation speed determination and argue that a common midpoint method (CMP) should be used if possible. Our observations reveal that…

3D modelSvalbardground-penetrating radarcommon midpoint methodScienceQglaciologyunmanned aerial vehicleGeneral Earth and Planetary Sciencestemperate icephotogrammetrythermal structureRemote Sensing
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Soil moisture variations from boreal forests to the tundra

2023

Soil moisture has a profound influence on life on Earth, and this vital water resource varies across space and time. Here, we explored soil moisture variations in boreal forest and tundra environments, where comprehensive soil moisture datasets are scarce. We installed soil moisture sensors up to 14 cm depth at 503 measurement sites within seven study areas across northern Europe. We recorded 6,138,528 measurements to capture soil moisture variations of the snowless season from April to September 2020. We described the spatio-temporal patterns of soil moisture, and test how these patterns are linked to topography and how these links vary in space and time. We found large spatial variation a…

4112 ForestrymaaperäkosteusSoil waterWetlandSoil wetnessSubarcticAlpinemetsätWater Science and Technologymittausmenetelmät
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La caduta dell'impero d'Occidente (455-476 d.C.)

2008

Le vicende degli anni 455-476, dalla morte di Valentiniano III alla caduta della pars Occidentis dell’impero, mostrano l’indebolirsi della figura imperiale e l’emergere del potere di Ricimero, magister militum barbarico, figura centrale di Kaisermacher che domina lo scenario politico del periodo.

476 d.C.RicimerostoriografiaTarda AntichitàSettore L-ANT/03 - Storia Romanabarbari
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"Table 3" of "Charm-quark fragmentation fractions and production cross section at midrapidity in pp collisions at the LHC"

2022

Production cross section of charm-anticharm quark pairs per unity of rapidity at midrapidity $\mathrm{d}\sigma^{\mathrm{c\overline{c}}}/\mathrm{d}y|_{|y| < 0.5}$ in pp collisions at $\sqrt{s} = 2.76$, $5.02$, and $7$ TeV.

5020.0$\mathrm{d}\sigma^{\mathrm{ccbar}}/\mathrm{d}y|_{|y| < 0.5}$pp -> $\mathrm{ccbar}$ + X2760.0High Energy Physics::Phenomenology7000.0High Energy Physics::ExperimentNuclear Experiment
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"Table 6" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2021

$p_{T}$-distributions of protons ($p+pbar$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

5020.0InclusiveAstrophysics::High Energy Astrophysical PhenomenaP P --> P XP P --> PBAR XPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentTransverse Momentum DependenceDifferential DistributionDN/DPT
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"Table 5" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2021

$p_{T}$-distributions of protons ($p+pbar$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

5020.0InclusivePB PB --> PBAR XPB PB --> P XPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentTransverse Momentum DependenceDifferential DistributionDN/DPT
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