Search results for "Cross Section"

showing 10 items of 3111 documents

"Table 8" of "Cross-sections and leptonic forward-backward asymmetries from the Z0 running of LEP."

2000

Cross section and forward-backward asymmetry in the MU+ MU- channel for the1994 data. The polar angle is 20 to 160 degrees. Additional systematic error for cross section of 0.26 PCT (efficiencies and backgrounds) and 0.14 PCT (absolute luminosity). Additional systematic error for the asymmetry of 0.0005.

Asymmetry MeasurementE+ E- --> MU+ MU-E+ E- ScatteringIntegrated Cross SectionExclusive91.2Cross SectionSIGMuon productionASYM
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"Table 7" of "Measurement of electroweak parameters from Z decays into Fermion pairs"

1990

No description provided.

Asymmetry MeasurementE+ E- --> Z0E+ E- ScatteringIntegrated Cross SectionExclusiveE+ E- --> LEPTON+ LEPTON-88.227-94.278Cross SectionSIGASYM
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"Table 2" of "Measurement and Interpretation of Fermion-Pair Production at LEP Energies of 183 and 189 GeV"

2003

No description provided.

Asymmetry MeasurementE+ E- ScatteringIntegrated Cross SectionE+ E- --> TAU- TAU+ (GAMMAS)ExclusiveE+ E- --> MU- MU+ (GAMMAS)Cross SectionTau production183.0-189.0SIGMuon productionASYM
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ATLAS measurements of the properties of jets for boosted particle searches

2012

Measurements are presented of the properties of high transverse momentum jets, produced in proton-proton collisions at a center-of-mass energy of √s=7  TeV. The data correspond to an integrated luminosity of 35  pb−1 and were collected with the ATLAS detector in 2010. Jet mass, width, eccentricity, planar flow and angularity are measured for jets reconstructed using the anti-kt algorithm with distance parameters R=0.6 and 1.0, with transverse momentum pT>300  GeV and pseudorapidity |η|<2. The measurements are compared to the expectations of Monte Carlo generators that match leading-logarithmic parton showers to leading-order, or next-to-leading-order, matrix elements. The generators describ…

Atlas detectorMonte Carlo methodParton7. Clean energy01 natural sciencesNucleonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentNUCLEONATLAS; jets; boostedQCDetectors de radiacióQuantum chromodynamicsPhysicsLarge Hadron ColliderAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleATLASINCLUSIVE JET CROSS SECTIONLarge Hadron ColliderPseudorapidityTransverse momentumComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCFRAGMENTATIONNucleonParticle Physics - ExperimentjetsNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas530 PhysicsAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Proton-proton collisionsNuclear physics0103 physical sciencesddc:530High Energy Physics010306 general physicsCiencias ExactasScience & TechnologyATLAS detector010308 nuclear & particles physicsFísicaMODELHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)PARTON DISTRIBUTIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentModel
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"Table 2" of "Search for exclusive charmless B meson decays with the DELPHI detector at LEP"

1995

Three body decay modes. Upper limits at 90% CL.

B- --&gt; P PBAR PI-SIG/SIGStrange productionE+ E- ScatteringB- --&gt; K- K+ K-Integrated Cross SectionB- --&gt; K- PI+ PI-E+ E- --&gt; ZExclusiveCross SectionB- --&gt; PI- PI+ PI-
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A model for the γN → ππN reaction

1995

We have studied the γN→ππN reaction using a model which includes N, Δ(1232), N*(1440) and N*(1520) intermediate baryonic states and the ρ-meson as intermediate ππ resonance. The model reproduces fairly well experimental cross sections below E γ = 800 MeV and invariant-mass distributions even at higher energies. One of the interesting findings of the study is that the γ N →N*(1520) → Δπ process is very important and interferes strongly with the dominant Δ-Kroll-Ruderman term to produce the experimental peak of the cross section.

BaryonPhysicsCross section (physics)symbols.namesakesymbolsIntermediate stateFeynman diagramAtomic physicsResonance (particle physics)Simulation
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The alanine detector in BNCT dosimetry: Dose response in thermal and epithermal neutron fields

2014

Purpose: The response of alanine solid state dosimeters to ionizing radiation strongly depends on particle type and energy. Due to nuclear interactions, neutron fields usually also consist of secondary particles such as photons and protons of diverse energies. Various experiments have been carried out in three different neutron beams to explore the alanine dose response behavior and to validate model predictions. Additionally, application in medical neutron fields for boron neutron capture therapy is discussed. Methods: Alanine detectors have been irradiated in the thermal neutron field of the research reactor TRIGA Mainz, Germany, in five experimental conditions, generating different secon…

Bonner sphereMaterials sciencebusiness.industryPhysics::Medical Physicstechnology industry and agricultureGeneral MedicineNeutron temperatureNuclear physicsNeutron captureAbsorbed doseNeutron cross sectionDosimetryNeutron sourceNeutronNuclear medicinebusinessMedical Physics
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Neutron fluence spectrometry using disk activation

2009

Abstract A simple and robust detector for spectrometry of environmental neutrons has been developed. The technique is based on neutron activation of a series of different metal disks followed by low-level gamma-ray spectrometry of the activated disks and subsequent neutron spectrum unfolding. The technique is similar to foil activation but here the applied neutron fluence rates are much lower than usually in the case of foil activation. The detector has been tested in quasi mono-energetic neutron fields with fluence rates in the order of 1000–10000 cm −2  s −1 , where the obtained spectra showed good agreement with spectra measured using a Bonner sphere spectrometer. The detector has also b…

Bonner spherePhysicsRadiationSpectrometerPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFluenceNuclear physicsNeutron fluxNeutron cross sectionNeutron detectionNeutronAtomic physicsNuclear ExperimentInstrumentationNeutron activationRadiation Measurements
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&lt;title&gt;Iodine and bromine resonance lamps in atmospheric research&lt;/title&gt;

2003

For the first time previously developed iodine resonance spectra source has been tested in flash photolysis experiment. Quantitative measurements of concentration kinetics of iodine atomic species in a I2+O3 system are possible. The 183.038 nm resonance absorption transition of I(2P3/2) in previously developed EDL has been studied; dependence of self-absorption and self-reversal on iodine partial pressure in the discharge volume has been measured. The search for optimal conditions for an iodine EDL with minimized self-absorption and sufficient intensity were made. In condition of flash photolysis with previously described method it is possible to determine the emission temperature, oscillat…

BromineAbsorption spectroscopyOscillator strengthChemistryAnalytical chemistryAbsorption cross sectionFlash photolysisResonancechemistry.chemical_elementAbsorption (electromagnetic radiation)SpectroscopySPIE Proceedings
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Study of heavy meson production in p-Pb collisions at $\sqrt{S}$=5.02 TeV in the general-mass variable-flavour-number scheme

2017

Nuclear physics / B 925, 415 - 430 (2017). doi:10.1016/j.nuclphysb.2017.10.016

CMSnucleusFOS: Physical sciencesinitial-state interaction530High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CERN LHC CollALICEproduction [bottom]heavy [meson]ddc:530High Energy Physics::Experimentcross section [p p]Nuclear Experimentnumerical calculationscharmproduction [meson]1 [higher-order]
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