Search results for " Spectra"

showing 10 items of 709 documents

Structural characterization of β-2′-pyridylaminocrotonoyl-2-pyridylamide by ESI-MS, NMR, single crystal X-ray analysis and ab initio methods

2003

Abstract In contradiction with earlier reports 1H, 13C and 15N NMR spectra show that β-2′-pyridylaminocrotonoyl-2-pyridylamide is the only form present in chloroform solution. According to the X-ray data the same tautomer exists also in the crystal state. The studied amide has a dimeric form where the monomer molecules are held together by two intermolecular hydrogen bonds. The NMR spectral data show that there is also an intramolecular hydrogen bond in each monomer subunit. The dilution experiments and variable-temperature 1H NMR runs show that β-2′-pyridylaminocrotonoyl-2-pyridylamide tends to form the dimers also in chloroform solution at higher concentrations. The ESI-TOF MS measurement…

Hydrogen bondChemistryOrganic ChemistryIntermolecular forceAb initioTautomerAnalytical ChemistryInorganic ChemistryNMR spectra databaseCrystallographyMolecular geometryIntramolecular forceProton NMRSpectroscopyJournal of Molecular Structure
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Structural and spectroscopic characterisation of 2-(2'-hydroxybenzoyl)pyrrole and its O-methyl derivative

2004

Abstract Density functional theory calculations on the tautomeric and conformational equilibria of 2-(2′-hydroxybenzoyl)pyrrole (HBP) and 2-(2′-methoxybenzoyl)pyrrole (MBP) were performed. Moreover, the experimental IR and UV spectra of the same compounds were recorded and compared with the theoretical data. The presence of an intramolecular hydrogen bond in HBP can be related to the biological activities of some of its derivatives.

Hydrogen bondMethyl derivativeCondensed Matter PhysicsBiochemistryTautomerSettore CHIM/08 - Chimica Farmaceuticachemistry.chemical_compoundUv spectrachemistryComputational chemistryIntramolecular forceDensity functional theoryPhysical and Theoretical ChemistryDFT calculations2-(2′-Hydroxybenzoyl)pyrrole2-(2′-Methoxybenzoyl)pyrrolePyrrole
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15N NMR: Substituent effect analysis inpara-andmeta-substituted phenylhydrazines

1994

15N NMR spectra of phenylhydrazine and of 14 para- and meta-substituted phenylhydrazines were measured at natural isotope abundance in DMSO-d6 solution. The substituent present exerts a larger influence on the chemical shift of the nitrogen atom directly bound to the aromatic ring (N-1) than on the second one (N-2), which shows an attenuated and inverted trend. The chemical shifts of N-1 and N-2 give a good cross correlation in both series of compounds if p-NO2 and m-F derivatives are excluded from the correlations of para- and meta-substituted phenylhydrazines, respectively. Moreover, N-1 SCS values show good linear correlations with Hammett substituent constants, with SCSs of directly bou…

HydrogenStereochemistryChemical shiftPhenylhydrazinesSubstituentchemistry.chemical_elementGeneral ChemistryRing (chemistry)Medicinal chemistryNMR spectra databasechemistry.chemical_compoundAnilinechemistryGeneral Materials SciencePhenylhydrazineMagnetic Resonance in Chemistry
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Application of 61Ni Mössbauer spectroscopy to chemical problems

1996

Using the possibility to produce 61Co sources at the MAinz MIcrotron, 61Ni Mossbauer spectroscopy was applied to different kinds of chemical problems. Measurements of isomer shifts and V zz values in some common compounds and compounds with unusual chemical bonding for comparison with band structure calculations, measurement of 61Ni Mossbauer parameters in model compounds for hydrogenase and dehydrogenase with an active [NiS4] centre, and study of novel binary NiF3 compounds at helium temperature are presented.

HydrogenaseMaterials scienceNuclear magnetic resonanceChemical bondMössbauer spectroscopyGeneral Physics and AstronomyPhysical chemistryMossbauer spectraElectronic band structureMicrotronHelium temperatureIl Nuovo Cimento D
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Temperature dependence of the E2h phonon mode of wurtzite GaN/AlN quantum dots

2008

Raman scattering has been used to study the temperature dependence of the frequency and linewidth of the E2h phonon mode of GaN/AlN quantum dot stacks grown on 6H-SiC. The evolution of the nonpolar phonon mode was analyzed in the temperature range from 80 to 655 K for both quantum dots and barrier materials. The experimental results are interpreted by comparison with a model that takes into account symmetric phonon decay and the different thermal expansions of the constituents of the heterostructure. We find a small increase in the anharmonic parameters of the phonon modes in the heterostructure with respect to bulk. jorbumar@alumni.uv.es Alberto.Garcia@uv.es Ana.Cros@uv.es

III-V semiconductorsMaterials scienceCondensed matter physicsPhononUNESCO::FÍSICAGallium compoundsGeneral Physics and AstronomyHeterojunctionAluminium compounds ; Gallium compounds ; III-V semiconductors ; Phonons ; Raman spectra ; Semiconductor quantum dots ; Thermal expansionAtmospheric temperature rangeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter::Materials Sciencesymbols.namesakeLaser linewidth:FÍSICA [UNESCO]Quantum dotsymbolsPhononsSemiconductor quantum dotsRaman spectraThermal expansionRaman spectroscopyAluminium compoundsRaman scatteringWurtzite crystal structureJournal of Applied Physics
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Raman study of self-assembled InAs/InP quantum wire stacks with varying spacer thickness

2008

http://link.aip.org/link/?JAPIAU/104/033523/1

III-V semiconductorsMaterials sciencePhononAnnealing (metallurgy)General Physics and AstronomyCritical pointsDielectricAnnealingCondensed Matter::Materials Sciencesymbols.namesake:FÍSICA [UNESCO]Indium compoundsCondensed matter physicsQuantum wireUNESCO::FÍSICAAnnealing ; Critical points ; III-V semiconductors ; Indium compounds ; Phonons ; Raman spectra ; Self-assembly ; Semiconductor quantum wiresSelf-assemblyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectMolecular vibrationSemiconductor quantum wiressymbolsPhononsRaman spectraRaman spectroscopyExcitationRaman scatteringJournal of Applied Physics
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Oscillator strength reduction induced by external electric fields in self-assembled quantum dots and rings

2007

We have carried out continuous wave and time resolved photoluminescence experiments in self-assembled In(Ga)As quantum dots and quantum rings embedded in field effect structure devices. In both kinds of nanostructures, we find a noticeable increase of the exciton radiative lifetime with the external voltage bias that must be attributed to the field-induced polarizability of the confined electron hole pair. The interplay between the exciton radiative recombination and the electronic carrier tunneling in the presence of a stationary electric field is therefore investigated and compared with a numerical calculation based on the effective mass approximation.

III-V semiconductorsOscillator strengthRadiative lifetimesTime resolved spectraTunnellingSelf assembledCondensed Matter::Materials ScienceGallium arsenideIndium compoundsElectric fieldQuantum mechanicsSemiconductor quantum dotsNetwork of excellenceEuropean commissionPhotoluminescenceQuantum tunnellingPhysicsSelf-assemblyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsQuantum dotEffective massElectron hole recombinationElectron-hole recombinationPhysical Review B
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Correlation between optical properties and barrier composition in InxGa1−xP/GaAs quantum wells

1998

9 páginas, 11 figuras.

III-V semiconductorsPhotoluminescenceMaterials scienceBand gapExcitonAlloyGeneral Physics and Astronomyengineering.materialGallium arsenideSpectral line broadeningchemistry.chemical_compoundCondensed Matter::Materials ScienceGallium arsenideIndium compounds:FÍSICA [UNESCO]Optical constantsInterface structureFluctuationsSemiconductor quantum wellsPhotoluminescenceQuantum wellCondensed matter physicsCondensed Matter::OtherGallium compoundsUNESCO::FÍSICAHeterojunctionInterface statesCondensed Matter::Mesoscopic Systems and Quantum Hall EffectStoichiometryEnergy gapchemistryIndium compounds ; Gallium compounds ; III-V semiconductors ; Gallium arsenide ; Semiconductor quantum wells ; Interface structure ; Photoluminescence ; Excitons ; Interface states ; Fluctuations ; Stoichiometry ; Spectral line broadening ; Energy gap ; Optical constantsengineeringExcitonsMolecular beam epitaxy
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Vibrational Sum Frequency Generation Spectroscopy of the Water Liquid–Vapor Interface from Density Functional Theory-Based Molecular Dynamics Simulat…

2013

International audience; The vibrational sum frequency generation (VSFG) spectrum of the water liquid-vapor (LV) interface is calculated using density functional theory-based molecular dynamics simulations. The real and imaginary parts of the spectrum are in good agreement with the experimental data, and we provide an assignment of the SFG bands according to the dipole orientation of the interfacial water molecules. We use an instantaneous definition of the surface, which is more adapted to the study of interfacial phenomena than the Gibbs dividing surface. By calculating the vibrational (infrared, Raman) properties for interfaces of varying thickness, we show that the bulk spectra signature…

InfraredBulk spectra02 engineering and technologyMolecular dynamicsVibrational sum-frequency generations010402 general chemistry01 natural sciencesMolecular physicsSpectral lineInterfacial phenomenaLiquid-vapor interfaceMolecular dynamicssymbols.namesakeDipole orientationComputational chemistryGeneral Materials SciencePhysical and Theoretical ChemistryDividing surfacesDensity functionalsSum-frequency generationMolecular dynamics simulationsChemistryInterfacial water moleculesThin layers021001 nanoscience & nanotechnologyLiquid-vapor0104 chemical sciencesDipoleImaginary partsDensity functional theoryVaporssymbolsDensity functional theory[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]0210 nano-technologyRaman spectroscopyVarying thicknessSum frequency generation spectroscopyThe Journal of Physical Chemistry Letters
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Über gemischte bindungen in der IV. Hauptgruppe

1984

Abstract The reaction of Ph 3 PbLi with Ph 3 SnCl or Ph 3 GeCl gives Ph 3 PbSnPh 3 and Ph 2 PbGePh 3 , respectively; there is no reaction with Ph 3 SiCl. Ph 3 SiLi reacts with Ph 3 PbCl to form a regular 1 : 1 Pb 2 Ph 6 · Si 2 Ph 6 phase. The compounds have been investigated by mass, NMR and vibrational spectra: 207 Pb NMR chemical shifts with respect to PbMe 2 −79.8 (Pb 2 Ph 6 ), −256.5 (Ph 3 PbSnPh 3 ), −271.5 ppm (Ph 3 PbGePh 3 ); stretching vibrations 112 (PbPb), 125 (PbSn), 138 cm −1 (PbGe). The crystal structures have been determined and refined to R = 0.061 (Ph 3 PbSnPh 3 , −40°C), 0.053 (Ph 3 PbGePh 3 , −50°C), 0.068 (Pb 2 Ph 6 · Si 2 Ph 6 , 20°C); bond lengths 285 (PbPb),…

Inorganic ChemistryBond lengthStereochemistryChemistryChemical shiftPhase (matter)Organic ChemistryMaterials ChemistryPhysical chemistryCrystal structurePhysical and Theoretical ChemistryBiochemistryVibrational spectraJournal of Organometallic Chemistry
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