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Spectroscopy satellite

Physical background. MAS will narrow the inliomogeneously broadened satellite transitions to give a series of sharp sidebands whose intensity envelopes closely follow the static powder pattern so that the quadnipole interaction can be deduced. The work of Samoson [25] gave real impetus to satellite transition spectroscopy by showing that both the second-order quadnipolar linewidths and isotropic shifts are fiinctions of / and Some combinations of / and produce smaller second-order quadnipolar effects on the satellite lines than... [Pg.1485]

All have zero nuclear spin except (33.8% abundance) which has a nuclear spin quantum number this isotope finds much use in nmr spectroscopy both via direct observation of the Pt resonance and even more by the observation of Pt satellites . Thus, a given nucleus coupled to Pt will be split into a doublet symmetrically placed about the central unsplit resonance arising from those species containing any of the other 5 isotopes of Pt. The relative intensity of the three resonances will be (i X 33.8) 66.2 ( x 33.8), i.e. 1 4 1. [Pg.1148]

Kohei Uosaki received his B.Eng. and M.Eng. degrees from Osaka University and his Ph.D. in Physical Chemistry from flinders University of South Australia. He vas a Research Chemist at Mitsubishi Petrochemical Co. Ltd. from 1971 to 1978 and a Research Officer at Inorganic Chemistry Laboratory, Oxford University, U.K. bet veen 1978 and 1980 before joining Hokkaido University in 1980 as Assistant Professor in the Department of Chemistry. He vas promoted to Associate Professor in 1981 and Professor in 1990. He is also a Principal Investigator of International Center for Materials Nanoarchitectonics (MANA) Satellite, National Institute for Materials Science (NIMS) since 2008. His scientific interests include photoelectrochemistry of semiconductor electrodes, surface electrochemistry of single crystalline metal electrodes, electrocatalysis, modification of solid surfaces by molecular layers, and non-linear optical spectroscopy at interfaces. [Pg.337]

How then, can one recover some quantity that scales with the local charge on the metal atoms if their valence electrons are inherently delocalized Beyond the asymmetric lineshape of the metal 2p3/2 peak, there is also a distinct satellite structure seen in the spectra for CoP and elemental Co. From reflection electron energy loss spectroscopy (REELS), we have determined that this satellite structure originates from plasmon loss events (instead of a two-core-hole final state effect as previously thought [67,68]) in which exiting photoelectrons lose some of their energy to valence electrons of atoms near the surface of the solid [58]. The intensity of these satellite peaks (relative to the main peak) is weaker in CoP than in elemental Co. This implies that the Co atoms have fewer valence electrons in CoP than in elemental Co, that is, they are definitely cationic, notwithstanding the lack of a BE shift. For the other compounds in the MP (M = Cr, Mn, Fe) series, the satellite structure is probably too weak to be observed, but solid solutions Coi -xMxl> and CoAs i yPv do show this feature (vide infra) [60,61]. [Pg.116]

The thermally induced interconversion of two oxides, e.g., C03O4 and CoO, and CU2O and CuO, has been followed by electron spectroscopy 15, 67). In both cases the shake-up satellites associated with the Co(2piy2)... [Pg.90]

Gan, Z. (2001) Satellite transition magic-angle spinning nuclear magnetic resonance spectroscopy of half-integer... [Pg.168]

Ashbrook, S.E. and Wimperis, S. (2002) High-resolubon NMR spectroscopy of quadrupolar nuclei in solids satellite-transibon MAS with self-compensabon for magic-angle misset. J. Am. Chem. Soc., 124,11602. [Pg.169]

Beyond the violet, France is present in all areas of astrophysics, from UV through X to gamma rays. Just mentioning the main items devoted to spectroscopy, France is involved in the satellites FUSE, XMM and INTEGRAL. [Pg.47]

The energy involved in this excitation is easily obtainable from atomic spectroscopy (see Chapt. A) and is found to be about 6eV i.e. coinciding with the energy position of the satellite. [Pg.217]

The crucial experiment to identify whether this satellite structure is due to a localized 5 f hole, is claimed to be photoemission spectroscopy, in which the excitation (provided by synchrotron radiation) is tuned through the 5d-5f threshold energy . At the threshold energy an empty 5 f state just beyond Ep becomes occupied... [Pg.228]

Measurements either from the ground or from satellites have been a major contribution to this effort, and satellite instruments such as LIMS (Limb Infrared Monitor of the Stratosphere) on the Nimbus 7 satellite (I) in 1979 and ATMOS (Atmospheric Trace Molecular Spectroscopy instrument), a Fourier transform infrared spectrometer aboard Spacelab 3 (2) in 1987, have produced valuable data sets that still challenge our models. But these remote techniques are not always adequate for resolving photochemistry on the small scale, particularly in the lower stratosphere. In some cases, the altitude resolution provided by remote techniques has been insufficient to provide unambiguous concentrations of trace gas species at specific altitudes. Insufficient altitude resolution is a handicap particularly for those trace species with large gradients in either altitude or latitude. Often only the most abundant species can be measured. Many of the reactive trace gases, the key species in most chemical transformations, have small abundances that are difficult to detect accurately from remote platforms. [Pg.145]

Thermal emission spectroscopy can be used in middle- and far-infrared spectral regions to make stratospheric measurements, and it has been applied to a number of important molecules with balloon-borne and satellite-based detection systems. In this approach, the molecules of interest are promoted to excited states through collisions with other molecules. The return to the ground state is accompanied by the release of a photon with energy equal to the difference between the quantum states of the molecule. Therefore, the emission spectrum is characteristic of a given molecule. Calculation of the concentration can be complicated because the emission may have originated from a number of stratospheric altitudes, and this situation may necessitate the use of computer-based inversion techniques (24-27) to retrieve a concentration profile. [Pg.306]

Satellites - [ALUMINUMAND ALUMINUM ALLOYS] (Vol 2) -batteries for [BATTERIES - SECOND ARYCELLS - ALKALINE] (Vol 3) -hydrazine fuel for [HYDRAZINE AND ITS DERIVATIVES] (Vol 13) -infrared remote sensing from [INFRARED TECHNOLOGY AND RAMAN SPECTROSCOPY - INFRAREDTECHNOLOGY] (Vol 14) -synthetic quartz crystals for [SILICA - SYNTHETIC QUARTZ CRYSTALS] (Vol 21) -thermoelectric power supplies for [THERMOELECTRIC ENERGY CONVERSION] (Vol 23)... [Pg.870]

Chance, K., J.P. Burrows, D. Pettier and W. Schneider (1997) Satellite measurements of atmospheric ozone profiles, including tropospheric ozone from UV/visible measurements in the nadir geometry a potential method to retrieve tropospheric ozone. Journal Quantitative Spectroscopy and Radiative Transfer 57 467-476. [Pg.325]


See other pages where Spectroscopy satellite is mentioned: [Pg.1478]    [Pg.1484]    [Pg.151]    [Pg.39]    [Pg.50]    [Pg.589]    [Pg.14]    [Pg.272]    [Pg.91]    [Pg.121]    [Pg.142]    [Pg.113]    [Pg.401]    [Pg.18]    [Pg.391]    [Pg.144]    [Pg.189]    [Pg.96]    [Pg.15]    [Pg.753]    [Pg.686]    [Pg.18]    [Pg.246]    [Pg.107]    [Pg.199]    [Pg.279]    [Pg.60]    [Pg.42]    [Pg.173]    [Pg.564]    [Pg.399]    [Pg.266]    [Pg.150]    [Pg.959]    [Pg.42]   


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