Search results for "GASES"

showing 10 items of 1098 documents

"Table 22" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0W Production
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"Table 24" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0W Production
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"Table 25" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0W Production
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"Table 11" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XHigh Energy Physics::ExperimentDSIG/DETARAPJet Production1960.0W Production
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"Table 9" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XHigh Energy Physics::ExperimentDSIG/DETARAPJet Production1960.0W Production
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"Table 12" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XHigh Energy Physics::ExperimentDSIG/DETARAPJet Production1960.0W Production
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"Table 2" of "Measurement of the shape of the boson transverse momentum distribution in p anti-p ---> Z / gamma* ---> e+ e- + X events produced…

2008

Correlation matrix for all rapidity Z bosons for the 12 bins used for PT < 30.

Condensed Matter::Quantum GasesInclusiveZ ProductionElectron productionPBAR P --> E+ E- XCORRHigh Energy Physics::PhenomenologyPBAR P --> GAMMA* XAstrophysics::Cosmology and Extragalactic AstrophysicsPhysics::Data Analysis; Statistics and ProbabilityPBAR P --> Z0 X
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FTICR analysis of the magnetic trapping mode of the electron beam ion trap

1996

Abstract An electron beam ion trap is used to produce and confine highly-charged atomic ions in an energetic electron beam (electron trapping mode). After switching off the electron beam the ions remain trapped due to the external magnetic and electric fields. We have investigated the properties of this magnetic trapping mode by use of Fourier transform ion cyclotron resonance mass spectrometry. We found that the number of highly charged ions and the relative species abundance is nearly the same just before and just after turning off the electron beam. The electron trapping mode thus represents an ideal method for filling the trap in situ without the losses associated with transferring the …

Condensed Matter::Quantum GasesIon beam depositionChemistryElectric fieldTrappingIon trapAtomic physicsSpectroscopyFourier transform ion cyclotron resonanceIon cyclotron resonanceElectron beam ion trapIonInternational Journal of Mass Spectrometry and Ion Processes
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Direct observation of second-order atom tunnelling

2007

Tunnelling of material particles through a classically impenetrable barrier constitutes one of the hallmark effects of quantum physics. When interactions between the particles compete with their mobility through a tunnel junction, intriguing novel dynamical behaviour can arise where particles do not tunnel independently. In single-electron or Bloch transistors, for example, the tunnelling of an electron or Cooper pair can be enabled or suppressed by the presence of a second charge carrier due to Coulomb blockade. Here we report on the first direct and time-resolved observation of correlated tunnelling of two interacting atoms through a barrier in a double well potential. We show that for we…

Condensed Matter::Quantum GasesJosephson effectQuantum PhysicsMultidisciplinaryCondensed matter physicsChemistryFOS: Physical sciencesCoulomb blockadeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter - Other Condensed MatterTunnel effectTunnel ionizationUltracold atomTunnel junctionCondensed Matter::SuperconductivityCooper pairQuantum Physics (quant-ph)Quantum tunnellingOther Condensed Matter (cond-mat.other)Nature
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Observation of the Kibble-Zurek scaling law for defect formation in ion crystals

2013

Traversal of a symmetry-breaking phase transition at finite rates can lead to causally separated regions with incompatible symmetries and the formation of defects at their boundaries, which has a crucial role in quantum and statistical mechanics, cosmology and condensed matter physics. This mechanism is conjectured to follow universal scaling laws prescribed by the Kibble-Zurek mechanism. Here we determine the scaling law for defect formation in a crystal of 16 laser-cooled trapped ions, which are conducive to the precise control of structural phases and the detection of defects. The experiment reveals an exponential scaling of defect formation γ(β), where γ is the rate of traversal of the …

Condensed Matter::Quantum GasesKibble-Zurek mechanismPhysicsScaling lawQuantum PhysicsMultidisciplinaryCondensed matter physicsCoulomb crystalsFOS: Physical sciencesGeneral Physics and AstronomyGeneral ChemistryMeasure (mathematics)General Biochemistry Genetics and Molecular BiologyIonCondensed Matter - Other Condensed MatterClassical mechanicsQuantum Physics (quant-ph)Other Condensed Matter (cond-mat.other)
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