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N bands

In general, electron-releasing substituents cause a bathochromic shift of the n band... [Pg.65]

Infrared spectral evidence indicates that indazol 3-one probably exists in the oxo form (cf. 77). 4-Monosubstituted-l,3-diphenylpyrazol-5-ones have been assigned an oxo structure (cf. 78) on the basis of infrared (presence of a v C=N band) and ultraviolet spectral data. The structure of certain iV-acylated pyrazolones has been discussed on the basis of their infrared spectra, but in these cases the possibility of acyl migration is a complicating factor. [Pg.46]

Band, m. volume binding.—n. band ribbon, tape, strap, strip, belt, hoop hinge bond, tie, ligament, -achst, m. banded agate, ribbon agate. [Pg.56]

Streifen, m. band, strip, stripe, stria streak, vein (in marble, etc.) strap, -gefiige, n. banded structure, -kohle, /. banded coal, -spektrum, n. band spectrum. [Pg.432]

Similar isomerizations have been noted for a number of complexes. As with metal nitrosyls, IR spectra can be used to indicate the manner of bonding, but there is an overlap region around 2080-2100 cm-1 where i/(C-N) is found for both N- and S-bonded thiocyanates (additionally, S-bonded thiocyanates usually give a much sharper i (C-N) band). 14N NQR has been shown to be a reliable discriminator, but X-ray diffraction is ultimately the most reliable method. [Pg.231]

Conjugated polymers are generally poor conductors unless they have been doped (oxidized or reduced) to generate mobile charge carriers. This can be explained by the schematic band diagrams shown in Fig. I.23 Polymerization causes the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) of the monomer to split into n and n bands. In solid-state terminology these are the valence and conduction bands, respectively. In the neutral forms shown in Structures 1-4, the valence band is filled, the conduction band is empty, and the band gap (Eg) is typically 2-3 eV.24 There is therefore little intrinsic conductivity. [Pg.551]

Figure 1. n band edges for neutral CnHn+2- The right hand side points correspond to an infinite polymer (CH)n. [Pg.151]

The one-dimensional chain of hydrogen atoms is merely a model. Flowever, compounds do exist to which the same kind of considerations are applicable and have been confirmed experimentally. These include polyene chains such as poly acetylene. The p orbitals of the C atoms take the place of the lx functions of the H atoms they form one bonding and one antibonding n band. Due to the Peierls distortion the polyacetylene chain is only stable with alternate short and long C-C bonds, that is, in the sense of the valence bond formula with alternate single and double bonds ... [Pg.95]

The outer most levels in C60 are due to rc orbitals . These are formed by 2p electrons which have their orbitals oriented along the radius of the molecule. The different environment inside and outside the spherical molecule causes the double-peaked structure in the momentum densities. In graphite the n band is formed by 2p orbitals oriented perpendicular to the sheets of carbon atoms. Using single-crystal graphite films we have a unique opportunity to study the effects of the orientation of these 2p orbitals in detail. [Pg.215]

Figure 8. In the top left panel we show the band structure in the repeated zone scheme for the T -M direction. In the lower left panel we show the top half of the graphite Brillouin zone. The measurement presented in the central and right panel are for the T-M and A-L directions. Darker shading corresponds to larger intensities. Note that the n band is visible in the latter but absent in the first. Figure 8. In the top left panel we show the band structure in the repeated zone scheme for the T -M direction. In the lower left panel we show the top half of the graphite Brillouin zone. The measurement presented in the central and right panel are for the T-M and A-L directions. Darker shading corresponds to larger intensities. Note that the n band is visible in the latter but absent in the first.
A comparison of the band structure diagram and these two measurements shows that experimentally the main measured intensity is constrained to a few of the bands present. In the first Brillouin zone the ct, band is found to be occupied, in the second zone 02. No sign of o, or the % band is found for the T M measurement. For the A-L measurement the same bands as for the T-M measurement contribute but in addition the n band is observed, mainly in the first Brillouin zone. These experiments are a beautiful, direct observation of the nodal plane of the % electrons in momentum space. [Pg.216]

The material balance is consistent with the results obtained by OSA (S2+S4 in g/100 g). For oil A, the coke zone is very narrow and the coke content is very low (Table III). On the contrary, for all the other oils, the coke content reaches higher values such as 4.3 g/ 100 g (oil B), 2.3 g/ioo g (oil C), 2.5 g/ioo g (oil D), 2.4/100 g (oil E). These organic residues have been studied by infrared spectroscopy and elemental analysis to compare their compositions. The areas of the bands characteristic of C-H bands (3000-2720 cm-1), C=C bands (1820-1500 cm j have been measured. Examples of results are given in Fig. 4 and 5 for oils A and B. An increase of the temperature in the porous medium induces a decrease in the atomic H/C ratio, which is always lower than 1.1, whatever the oil (Table III). Similar values have been obtained in pyrolysis studies (4) Simultaneously to the H/C ratio decrease, the bands characteristics of CH and CH- groups progressively disappear. The absorbance of the aromatic C-n bands also decreases. This reflects the transformation by pyrolysis of the heavy residue into an aromatic product which becomes more and more condensed. Depending on the oxygen consumption at the combustion front, the atomic 0/C ratio may be comprised between 0.1 and 0.3 ... [Pg.415]

The He(l) photoelectron spectra <1997JMT(392)21> of ATQ and TATCD were measured and interpreted by means of ab initio outer valence Green function calculations (OVGF). These gave an overall consistent agreement with the main features in the spectra, in particular of the n (N) bands. [Pg.641]

The high energy metal carbonyl band would be consistent with a Ti(IV) cationic complex, while the C=N bands correspond closely to those of the (TCNE)2 dianion at 2160 and 2095 cm-1 and also to those in (PPh3)2-(CO)IrN=C=C(CN)C(CN)=C=NIr(CO)(PPh3)2. [Pg.365]

Thus the weak n — n band in a saturated carbonyl compound is shifted from below 300 nm to above 300 nm with an increase in s. Conjugation of additional chromophoric groups moves mx progressively... [Pg.367]

The direction of the potential shift of the surface C-N band is the same as for the C-O band on Pt and the shift rates are ca. 30 cm 1/V for Ag and Au (22,23,25) and ca. 45 cm-1/V for Cu (33). The measurement for copper is less accurate due to formation of ion complexes with large absorption crossections and the relatively weak signal from the surface species itself. [Pg.329]

Figure 7. The dependence of the C—N bands of the adsorbed 12CN and 13CN- on the isotopic composition based on the data of Figure 4. (Reprinted from ref. 25. Copyright 1988 American Chemical Society.)... Figure 7. The dependence of the C—N bands of the adsorbed 12CN and 13CN- on the isotopic composition based on the data of Figure 4. (Reprinted from ref. 25. Copyright 1988 American Chemical Society.)...
To solve (12) uniquely, we must impose the initial conditions which arise from the original state of the system (r = — oo)>. Considering a case where, initially, the valence orbital 0> of the atom is empty, then d>(— oo)> must represent a situation where the n band orbitals of lowest energy are doubly occupied by electrons, i.e. [Pg.342]


See other pages where N bands is mentioned: [Pg.1148]    [Pg.2400]    [Pg.19]    [Pg.19]    [Pg.202]    [Pg.321]    [Pg.46]    [Pg.243]    [Pg.395]    [Pg.721]    [Pg.24]    [Pg.341]    [Pg.173]    [Pg.488]    [Pg.150]    [Pg.739]    [Pg.216]    [Pg.231]    [Pg.156]    [Pg.41]    [Pg.279]    [Pg.133]    [Pg.39]    [Pg.214]    [Pg.60]    [Pg.349]    [Pg.158]    [Pg.218]    [Pg.65]    [Pg.45]    [Pg.509]    [Pg.57]   
See also in sourсe #XX -- [ Pg.89 ]

See also in sourсe #XX -- [ Pg.554 , Pg.555 ]




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C—N Bands

Hoechst and N-banding

Metal Nanoparticles with the Associates of Donor Defects in Wide-Band-Gap n-type Semiconductors

N-H combination band from primary amides

N—H Bending Vibrations (Amide II Band)

N—H absorption bands

The n-electron energy band

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