Search results for "Rubidium"

showing 10 items of 103 documents

CCDC 1425268: Experimental Crystal Structure Determination

2016

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

Space GroupCrystallographyCrystal SystemCrystal Structurebis(11'-(2356891112-Octahydro-1471013-benzopentaoxacyclopentadecine-1516-diyl)bis(3-(4-nitrophenyl)urea))-rubidium chloride methanol solvate hydrateCell ParametersExperimental 3D Coordinates
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CCDC 1425267: Experimental Crystal Structure Determination

2016

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

Space GroupCrystallographyCrystal SystemCrystal Structurebis(11'-(2356891112-Octahydro-1471013-benzopentaoxacyclopentadecine-1516-diyl)bis(3-(4-nitrophenyl)urea))-rubidium fluoride diethyl ether methanol solvateCell ParametersExperimental 3D Coordinates
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CCDC 1478711: 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

Space GroupCrystallographyCrystal SystemCrystal Structurecatena-[(mu-11'1''-(17-(((4-(oxy(oxido)-azanyl)phenyl)carbamoyl)amino)-67910121320212324-decahydrodibenzo[bk][14710131619]heptaoxacyclohenicosine-2316-triyl)tris(3-(4-nitrophenyl)urea))-rubidium hemikis(carbonate) NN-dimethylformamide methanol solvate]Cell ParametersExperimental 3D Coordinates
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CCDC 1439194: Experimental Crystal Structure Determination

2016

Related Article: Toni Mäkelä, Miia-Elina Minkkinen, and Kari Rissanen|2016|Inorg.Chem.|55|1339|doi:10.1021/acs.inorgchem.5b02780

Space GroupCrystallographyCrystal Systemcatena-[(mu2-Chloro)-(mu2-1819-bis((2-oxidobenzylidene)amino)-23568911121415-decahydro-147101316-benzohexaoxacyclooctadecine)-dioxo-rubidium-uranium acetonitrile solvate]Crystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 288487: Experimental Crystal Structure Determination

2006

Related Article: A.Ahmen, M.Nissinen|2006|Chem.Commun.||1209|doi:10.1039/b515143k

Space GroupCrystallographycatena-((mu~3~-eta^6^-281420-Tetramethyl-456101112161718222324-dodecahydroxycalix(4)arene)-chloro-rubidium methanol solvate hemihydrate)Crystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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<title>High-frequency electrodeless light sources for application</title>

2001

The high-frequency electrodes light sources (HFELS) are widely used as bright radiators of narrow and intensive spectral lines covering spectral region from VUV to IR. In this work we shall give a short overview of our experience in preparation of HFELS, containing He, H, Rb, Hg, Zn, Pb, As, Sb, Bi, Tl, Hg-Cd, Hg-Zn, Hg-Cd-Zn, Se-Te for different applications. Special attention would be paid for HFELS use in Zeeman mercury analyzer, in Atomic absorption analyzer and Angle and glass refractive index measurement system.© (2001) COPYRIGHT SPIE--The International Society for Optical Engineering. Downloading of the abstract is permitted for personal use only.

Spectrum analyzerZeeman effectInfraredbusiness.industryChemistryOptical engineeringchemistry.chemical_elementSpectral linelaw.inventionRubidiumsymbols.namesakeOpticslawsymbolsOptoelectronicsAtomic absorption spectroscopybusinessRefractive indexSPIE Proceedings
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Saturated absorption spectroscopy: elimination of crossover resonances by use of a nanocell

2007

It is demonstrated that velocity selective optical pumping/saturation resonances of reduced absorption in a Rb vapor nanocell with thickness \textit{L=} $\lambda $, 2$\lambda $, and 3$\lambda $ (resonant wavelength $\lambda $ = 780 nm) allow the complete elimination of crossover (CO) resonances. We observe well pronounced resonances corresponding to the F$_{g}=3$ $\to $ F$_{e}=2,3,4$ hyperfine transitions of the $^{85}$Rb D$_{2}$ line with linewidths close to the natural width. A small CO resonance located midway between F$_{g}=3$ $\to $ F$_{e}=3$ and F$_{g}=3$ $\to$ F$_{e}=4$ transitions appears only for \textit{L} = 4$\lambda $. The D$_{2}$ line ($\lambda $ = 852 nm) in a Cs nanocell exhi…

StandardsOptical pumping[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Saturated absorption spectroscopyFOS: Physical sciencesPhysics - Classical PhysicsLambda01 natural sciencesIndustrial and Manufacturing Engineering010309 opticssymbols.namesakeAbsorption spectroscopy[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciencesFrequency measurementLine widthsRubidium 85Physics::Atomic Physics010306 general physicsInstrumentationHyperfine structure[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]PhysicsZeeman effectResonanceClassical Physics (physics.class-ph)Zeeman effectNanocellCondensed Matter PhysicsAtomic and Molecular Physics and Optics3. Good healthMagnetic fieldWavelengthHyperfine transitionsymbolsRubidium AtomsMagnetic field effectsAtomic physicsOptical saturation
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Calculation of modification of alkali metal atomic transition probability in strong external magnetic field and its application

2010

International audience; Interaction of alkali atoms with external magnetic field induced a splitting and a shift of their energy levels. We have study this interaction for external field from 0 to 5000 Gauss when the alkali vapor is confined in submicron thin vapor cell with thickness L = λ/2. Rubidium and Sodium vapors have been studied. The Hamiltonian can be expressed as the sum of the unperturbated atomic Hamiltonian and the so-called Zeeman Hamiltonian. The probability of a transition, induced by the laser electric field is proportional to the square of the transfer coefficients modified by the presence of the magnetic field. We will show that the strong nonlinearity of the transition …

Strong Magnetic FieldTransition Probability[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]SodiumPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsRubidiumNanocells[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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PECULIARITIES OF RESONANT ABSORPTION AND FLUORESCENCE IN EXTREMELY THIN CELL FILLED WITH Rb AND BUFFER GAS.

2010

Recently unique extremely thin cells (ETC) containing atomic vapour of alkali metals with the column thickness L of an order and much less than optical light wavelength λ have been developed. It has been demonstrated that these ETC are a very promising tool for a fundamental study of atom-light, atom-atom, atom-surface and atom-external magnetic field interactions. Particularly, a dramatically different behaviour of resonant absorption, fluorescence and resonant magneto-optical processes compared to that obtained with the help of cm-long ordinary cells has been demonstrated. Possible applications based on ETC are described, such as magnetometers with nanometric spatial resolution and tunabl…

Strong Magnetic Field[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]RubidiumNanocells[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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QUANTITATIVE SPECTROSCOPY OF Rb ATOMS IN STRONG MAGNETIC FIELD BASED ON SUBMICRON THIN VAPOUR.

2010

The energy levels of atoms placed in an external magnetic field undergo frequency shifts and changes in their transition probabilities. It is demonstrated that using fluorescence spectra from a submicron thin vapour cell (STC) with the thickness L = λ/2, it is possible to efficiently study the above mentioned changes (“half-λ Zeeman technique” (HLZT)). The circularly polarized beam of extended-cavity diode laser (λ = 794 nm, laser bandwidth γL < 1 MHz) resonant with 87Rb D1 transition, after passing through Faraday isolator is directed onto the Rb STC with the thickness L = λ/2. The temperature of the STC is 120 °C, corresponding to N ~ 1013 atom/cm3. STC was provided by a special oven with…

Strong Magnetic Field[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph][ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]RubidiumNanocells[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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