Search results for "Rubidium"

showing 10 items of 103 documents

Spectrochemical Rubidium-Strontium Method for Geological Age Determination

1960

The age values of lepidolites from South Africa and from Varutrask as well as that of a microcline from Varutrask have been determined and are discussed in connection with determination according to the potassium-argon method, applied to the same materials A method is suggested which allows the spectrochemical determination of Rb and Sr with sufficient accuracy. The isotopic composition is determined by means of a Fabry-Perot etalon and hollow-cathode excitation, investigating the hyper-fine structure of the Sr line at 4078 A.

StrontiumMicrocline010401 analytical chemistryAnalytical chemistrychemistry.chemical_elementMineralogyengineering.material01 natural sciencesIsotopic composition0104 chemical sciencesRubidium010309 opticschemistryAge values0103 physical sciencesengineeringInstrumentationSpectroscopyFabry–Pérot interferometerApplied Spectroscopy
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Influence of sample pan on the thermal behaviour of KSCN measured with TG

2003

Abstract In this study, the influence of the sample pan on the thermal behaviour of potassium thiocyanate (KSCN) was investigated. The measurements were performed with thermogravimetry (TG) and the two sample pans used were a platinum pan and a ceramic crucible. The samples were heated to 400–950 °C and the thermal products were identified by powder diffraction. The thermal behaviour of KSCN was found to be dependent on the sample pan used. With the platinum sample pan KSCN reacted in the first step into a mixture of K 2 SO 4 and potassium tetracyanoplatinate (K 2 Pt(CN) 4 ). In the second step, the mixture reacted further to pure K 2 SO 4 . In the ceramic sample crucible, however, the reac…

ThiocyanateAnalytical chemistrychemistry.chemical_elementCondensed Matter PhysicsAlkali metalRubidiumThermogravimetrychemistry.chemical_compoundchemistryPotassium thiocyanateSample preparationPhysical and Theoretical ChemistryPlatinumThermal analysisInstrumentationThermochimica Acta
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Rubidium dimers in paraffin-coated cells

2010

Measurements were made to determine the density of rubidium dimer vapor in paraffin-coated cells. The number density of dimers and atoms in similar paraffin-coated and uncoated cells was measured by optical spectroscopy. Due to the relatively low melting point of paraffin, a limited temperature range of 43-80 deg C was explored, with the lower end corresponding to a dimer density of less than 10^7 cm^(-3). With one-minute integration time, a sensitivity to dimer number density of better than 10^6 cm^(-3) was achieved. No significant difference in dimer density was observed between the cells.

Time delay and integrationPhysicsQuantum PhysicsNumber densityAtomic Physics (physics.atom-ph)DimerSignificant differenceAnalytical chemistryGeneral Physics and Astronomychemistry.chemical_elementLow melting pointFOS: Physical sciences02 engineering and technologyAtmospheric temperature range021001 nanoscience & nanotechnology01 natural sciencesPhysics - Atomic PhysicsRubidiumchemistry.chemical_compoundchemistry0103 physical sciences010306 general physics0210 nano-technologySpectroscopyQuantum Physics (quant-ph)
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Total Absorption Spectroscopy of Fission Fragments Relevant for Reactor Antineutrino Spectra and Decay Heat Calculations

2015

Volume: 111 Host publication title: WONDER-2015 Host publication sub-title: 4TH INTERNATIONAL WORKSHOP ON NUCLEAR DATA EVALUATION FOR REACTOR APPLICATIONS Isbn(print): 978-2-7598-1970-6 Beta decay of fission products is at the origin of decay heat and antineutrino emission in nuclear reactors. Decay heat represents about 7% of the reactor power during operation and strongly impacts reactor safety. Reactor antineutrino detection is used in several fundamental neutrino physics experiments and it can also be used for reactor monitoring and non-proliferation purposes. Rb-92,Rb-93 are two fission products of importance in reactor antineutrino spectra and decay heat, but their beta-decay properti…

Total absorption spectroscopyFissionQC1-999[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciences7. Clean energy01 natural sciencesPhysics::GeophysicsNuclear physicsrubidium0103 physical sciencesfission productsDecay heatNuclear Experiment010306 general physicsFission productsDecay schemeta114010308 nuclear & particles physicsChemistryPhysicsXenon-135Beta decay13. Climate actiondecay heatHigh Energy Physics::Experimentbeta decayantineutrino emissionNeutrinoEPJ Web of Conferences
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Tests of atomic charge-exchange cells for collinear laser spectroscopy

2012

Abstract The performance characteristics of two charge-exchange cells (CECs) with horizontal and vertical cell configurations were determined by neutralizing a 10-keV rubidium ion beam in a potassium vapor. The neutralization efficiency and the fluorescence line shape of the 5s 2 S 1 / 2 ↔ 5 p 2P3/2 (D2) transition in neutral 85Rb were investigated as a function of the reservoir temperature used to control the potassium vapor density. The CECs exhibited similar neutralization performance and at neutralization efficiencies greater than 25–50% an asymmetric line shape of the rubidium D2 fluorescent signal was observed. The asymmetry was attributed to inelastic channels in the charge-exchange …

Voigt profilePhysicsNuclear and High Energy PhysicsIon beamchemistry.chemical_elementResonanceIsotopes of rubidiumSpectral lineRubidiumIonchemistryAtomic physicsSpectroscopyInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Hyperfine Paschen-Back regime realized in Rb nanocell

2012

A simple and efficient scheme based on one-dimensional nanometric thin cell filled with Rb and strong permanent ring magnets allowed direct observation of hyperfine Paschen-Back regime on D1 line in 0.5 - 0.7 T magnetic field. Experimental results are perfectly consistent with the theory. In particular, with sigma+ laser excitation, the slopes of B-field dependence of frequency shift for all the 10 individual transitions of 85,87Rb are the same and equal to 18.6 MHz/mT. Possible applications for magnetometry with submicron spatial resolution and tunable atomic frequency references are discussed.

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Atomic Physics (physics.atom-ph)MagnetometerFOS: Physical sciences01 natural sciencesPhysics - Atomic Physicslaw.invention010309 optics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]law0103 physical sciencesOCIS codes: 020.1335 300.6360010306 general physicsHyperfine structure[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]Line (formation)PhysicsNanocellLaserRubidiumAtomic and Molecular Physics and OpticsMagnetic fieldnanocellMagnetHyperfineAtomic physicsPaschen-BackExcitation
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Study of optical and magneto-optical processes in cesium, rubidium and potassium micro- and nano-metric thin atomic layers

2016

It has been investigated the D1 line transitions of 39K atoms in external magnetic fields using nanocells for the cases of sigma+ and pi polarizations of laser radiation. For the first time it is demonstrated the decoupling of electronic total angular momentum J and nuclear momentum I (complete hyperfine Paschen-Back regime) in external magnetic field. For 39K the decoupling takes place at B >> 165 G. In the case of linear polarization it is shown that for B > 400 G the transmission spectrum consists of 2 groups of transitions and each group contains of one so-called "Guiding transition" (GT). The GT indicates the asymptotic value of all transitions probabilities in the group and the freque…

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics]Nano-cellule de rubidiumNano-cell of rubidiumRégime Paschen-BackSpectroscopieZeeman effectPaschen-Back RegimeEffet ZeemanSpectroscopy
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ATOM-WALL COLLISIONS INFLUENCE ON DARKLINE ATOMIC RESONANCES IN SUBMICRON THIN VAPOUR CELLS.

2010

Recently it was demonstrated that miniaturization of alkali cells, i.e. the use of an extremely thin cell (ETC) for the applications using the electromagnetically induced transparency (EIT) effect, despite to intuitive expectation, does not cause a strong broadening of the dark-line (DL) linewidth. Here we present the conditions when a strong broadening of DL linewidth (more than by 10 times) can be easily observed due to atom-wall collisions influence and this could be a convenient and robust tool for atomwall (i.e. ETC's window material/temperature) collisions study. We present experimental and theoretical results on EIT realized in a Λ- system of 85Rb, D2 line, 5S-5P-5S for a Rb vapour c…

[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]EIT[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]CollisionsRubidiumNanocells[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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CCDC 1425269: Experimental Crystal Structure Determination

2016

Related Article: T. Mäkelä, K. Rissanen|2016|Dalton Trans.|45|6481|doi:10.1039/C6DT00414H

bis(11'-(2356891112-Octahydro-1471013-benzopentaoxacyclopentadecine-1516-diyl)bis(3-(4-nitrophenyl)urea))-rubidium iodide dimethylformamide solvateSpace GroupCrystallographyCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 1478713: Experimental Crystal Structure Determination

2016

Related Article: Toni Mäkelä, Anniina Kiesilä, Elina Kalenius and Kari Rissanen|2016|Chem.-Eur.J.|22|14264|doi:10.1002/chem.201602362

catena-[11'1''-(17-(((4-(oxy(oxido)-azanyl)phenyl)carbamoyl)amino)-679101213202123242627-dodecahydrodibenzo[bn][1471013161922]octaoxacyclotetracosine-2316-triyl)tris(3-(4-nitrophenyl)urea)-rubidium iodide chloroform solvate]Space GroupCrystallographyCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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