Search results for "C-12"

showing 10 items of 16 documents

Self and N-2 collisional broadening of far-infrared methane lines measured at the SOLEIL synchrotron

2012

International audience; Following our recent study devoted to measurements of intensities of pure rotation lines of methane, room temperature far infrared spectra of methane diluted in nitrogen at five total pressures between 100 and 800 hPa have been recorded at the AILES beamline of the SOLEIL synchrotron. One hundred and five N-2 broadening coefficients of methane pure rotation lines have been measured in the 83-261 cm(-1) spectral range using multi-spectrum non-linear least squares fitting of Voigt profiles. Pressure-induced line shifts were not needed to fit the spectra to the noise level and line mixing effects were neglected. One hundred and seventy-six self broadening coefficients h…

Materials science010504 meteorology & atmospheric sciencesWIDTHSSynchrotron radiationchemistry.chemical_elementNU(4) BANDTRANSITIONS01 natural sciences7. Clean energySpectral lineMethanelaw.inventionsymbols.namesakechemistry.chemical_compoundFar infraredRETRIEVALSlaw0103 physical sciencesSPECTRAL REGION(CH4)-C-12010303 astronomy & astrophysicsTEMPERATURESpectroscopy0105 earth and related environmental sciences[PHYS.PHYS.PHYS-AO-PH]Physics [physics]/Physics [physics]/Atmospheric and Oceanic Physics [physics.ao-ph]RadiationDIODE-LASER SPECTROSCOPYCM(-1)NitrogenAtomic and Molecular Physics and OpticsSynchrotronBeamlinechemistry[ PHYS.PHYS.PHYS-AO-PH ] Physics [physics]/Physics [physics]/Atmospheric and Oceanic Physics [physics.ao-ph]13. Climate actionsymbolsSHIFT COEFFICIENTSAtomic physicsTitan (rocket family)
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The methane Raman spectrum from 1200 to 5500 cm(-1): A first step toward temperature diagnostic using methane as a probe molecule in combustion syste…

2005

International audience; We present a study of the spontaneous Raman spectra of (CH4)-C-12 from 1200 to 5500 cm(-1) at various temperatures. This study is of interest from a fundamental as well as from a practical point of view with regards to the temperature diagnostic in hydrocarbon combustion. The present investigation shows that the spontaneous (CH4)-C-12 Raman spectra are very sensitive to temperature and that the complexity of methane spectra is not an obstacle to use methane as a probe molecule in laser-diagnostic techniques. Our study consists in determining the polarisability parameters of methane (CH4)-C-12, unknown at the present time, from spontaneous Raman spectra recorded at pr…

Materials scienceAnalytical chemistry02 engineering and technologyCombustion01 natural sciences7. Clean energyTemperature measurementMethaneSpectral linesymbols.namesakechemistry.chemical_compoundNuclear magnetic resonance(CH4)-C-12Coherent anti-Stokes Raman spectroscopyPhysical and Theoretical ChemistryRamanSpectroscopyPropellant[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]methane010401 analytical chemistrypolarisability021001 nanoscience & nanotechnologyAtomic and Molecular Physics and Optics0104 chemical scienceschemistry13. Climate actionsymbolsCombustion chamber0210 nano-technologyRaman spectroscopytensorial formalismtemperature measurement
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CARS methane spectra: Experiments and simulations for temperature diagnostic purposes

2007

International audience; CARS laboratory experiments were done in the 2905-2925 cm(-1) range, in the vicinity of the v, band of the methane molecule, for pressures ranging from I to 50 bar, and temperatures up to 1100 K. These experiments were carried out in order to retrieve the pressure evolution of the CH4 spectrum, as well as to confirm its temperature dependance. After a brief recall on the theory used to compute pressure broadening coefficients and relaxation rates, we consider the v(3) and v(4) infrared bands of methane for benchmark calculations purposes. Next, we present recent experimental CARS spectra and calculated ones. Lastly, we discuss flame experiments as well as comparisons…

Materials scienceInfrared010402 general chemistryCombustion7. Clean energy01 natural sciencesTemperature measurementMethaneSpectral linechemistry.chemical_compoundsymbols.namesakeline-mixingNuclear magnetic resonancepressure broadening0103 physical sciences(CH4)-C-12CARSPhysical and Theoretical ChemistryRamanSpectroscopy[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]010304 chemical physicsmethaneRelaxation (NMR)Atomic and Molecular Physics and Optics0104 chemical sciencesComputational physicschemistry13. Climate actionsymbolsRaman spectroscopytemperature measurementBar (unit)combustion
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Measurement of the neutrino-oxygen neutral-current interaction cross section by observing nuclear deexcitation gamma rays

2014

We report the first measurement of the neutrino-oxygen neutral-current quasielastic (NCQE) cross section. It is obtained by observing nuclear deexcitation $\gamma$-rays which follow neutrino-oxygen interactions at the Super-Kamiokande water Cherenkov detector. We use T2K data corresponding to $3.01 \times 10^{20}$ protons on target. By selecting only events during the T2K beam window and with well-reconstructed vertices in the fiducial volume, the large background rate from natural radioactivity is dramatically reduced. We observe 43 events in the $4-30$ MeV reconstructed energy window, compared with an expectation of 51.0, which includes an estimated 16.2 background events. The background …

Nuclear and High Energy PhysicsCherenkov detectorPhysics::Instrumentation and DetectorsC-12FOS: Physical sciencesAstronomy & Astrophysicslaw.inventionHigh Energy Physics - ExperimentPhysics Particles & FieldsNuclear physicsSUPER-KAMIOKANDE DETECTORCross section (physics)High Energy Physics - Experiment (hep-ex)lawEXCITATIONABSORPTION[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]SCATTERINGO-16Nuclear ExperimentPhysicsCALIBRATIONScience & TechnologyNeutral currenthep-exPhysicsGamma rayT2K experimentFísica3. Good healthPhysical SciencesNeutrinoWEAKFiducial markerBeam (structure)
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Hypernuclear spectroscopy of products from Li-6 projectiles on a carbon target at 2 A GeV

2013

WOS: 000322848900009

Nuclear reaction(Li-6E=2 GeV/nucleonNuclear and High Energy PhysicsMaximum likelihoodWEAK DECAYFOS: Physical sciencesLIFETIMET-1/2. Compared with other datadeduced Lambda massC-12(LAMBDA)H-4)T-1/2measured Lambda H-3H-4 Lambda-hypernuclei invariant mass distribution T-1/2measured LambdaInvariant massNuclear Experiment (nucl-ex)LIGHT HYPERFRAGMENTSSpectroscopyNuclear ExperimentX)PhysicsH-4 Lambda-hypernuclei invariant mass distributionH-3ProjectileSignificance valueslifetime measurementdeduced Lambda mass H-3H-4 Lambda-hypernuclei mass T-1/2. Compared with other data lifetime measurementNUCLEAR REACTIONS C(Li-6Decay timeLAMBDA-HYPERNUCLEIAtomic physicst)NUCLEAR REACTIONS C(Li-6 X) (Li-6 t) (Li-6 H-4) E=2 GeV/nucleonH-4 Lambda-hypernuclei massHypertritonRELATIVISTIC HYPERNUCLEINuclear Physics A
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Testing charged current quasi-elastic and multinucleon interaction models in the NEUT neutrino interaction generator with published datasets from the…

2016

There has been a great deal of theoretical work on sophisticated charged current quasi-elastic (CCQE) neutrino interaction models in recent years, prompted by a number of experimental results that measured unexpectedly large CCQE cross sections on nuclear targets. As the dominant interaction mode at T2K energies, and the signal process in oscillation analyses, it is important for the T2K experiment to include realistic CCQE cross section uncertainties in T2K analyses. To this end, T2K’s Neutrino Interaction Working Group has implemented a number of recent models in NEUT, T2K’s primary neutrino interaction event generator. In this paper, we give an overview of the models implemented and pres…

Particle physicsPhysics::Instrumentation and DetectorsC-12Astronomy & AstrophysicsMASS7. Clean energy01 natural sciencesPhysics Particles & FieldsMiniBooNENuclear physics0103 physical sciencesMINERνAMuon neutrino010306 general physicsNeutrino oscillationEvent generatorPhysicsScience & TechnologyMuonDELTA010308 nuclear & particles physicsPhysicsT2K experimentNUCLEUS SCATTERINGPhysical SciencesSIMULATIONHigh Energy Physics::ExperimentNeutrino
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Properties of the 12C 10 MeV state determined through β-decay

2005

16 pages, 1 table, 10 figures.-- PACS nrs.: 23.40.-s; 26.20.+f; 27.20.+n.-- Printed version published Oct 3, 2005.

PhysicsNuclear and High Energy Physics[PACS] β decayDeduced spin and parity of levels in C-12[PACS] β decay; double β decay; electron and muon captureParity (physics)Alpha particleRadioactivity Be-12(β-) B-12(β(-)3α) [produced in Ta(p X)]Inelastic scatteringBeta decayelectron and muon captureParticle decayMeasured α-particle coincidencesR-matrix analysisdouble β decay6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Double-sided Si strip detectorDouble beta decay[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physics[PACS] Hydrostatic stellar nucleosynthesisExcitationCoincidence detection in neurobiologyNuclear Physics A
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CCDC 924267: Experimental Crystal Structure Determination

2013

Related Article: Ferenc Miklós, Zita Tóth, Mikko M. Hänninen, Reijo Sillanpää, Enikő Forró and Ferenc Fülöp|2013|Eur.J.Org.Chem.|2013|4887|doi:10.1002/ejoc.201300452

Space GroupCrystallographyCrystal System8-Methyl-7-(4-methylphenyl)-38-diazatetracyclo[9.2.1.0^210^.0^37^]tetradec-12-ene-49-dioneCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 1508564: Experimental Crystal Structure Determination

2017

Related Article: Beáta Fekete, Márta Palkó, Matti Haukka, Ferenc Fülöp|2017|Molecules|22|613|doi:10.3390/molecules22040613

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters8-methoxy-7-methyl-38-diazatetracyclo[9.2.1.0210.037]tetradec-12-ene-49-dioneExperimental 3D Coordinates
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CCDC 1508563: Experimental Crystal Structure Determination

2017

Related Article: Beáta Fekete, Márta Palkó, Matti Haukka, Ferenc Fülöp|2017|Molecules|22|613|doi:10.3390/molecules22040613

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parametersmethyl 8-methoxy-49-dioxo-38-diazatetracyclo[9.2.1.0210.037]tetradec-12-ene-7-carboxylateExperimental 3D Coordinates
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