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V-mode

Two other examples will sufhce. Methane physisorbs on NaCl(lOO) and an early study showed that the symmetrical, IR-inactive v mode could now be observed [97]. In more recent work, polarized FTIR rehection spectroscopy was used to determine that on being adsorbed, the three-fold degeneracies of the vs and v modes were partially removed [98]. This hnding allowed consideration of possible adsorbate-adsorbent geometries one was that of a tripod with three of the methane hydrogens on the surface. The systems were at between 4 and 40 K so that the equilibrium pressure was very low, about 10 atm. [Pg.635]

The Bloeh equations for the motion of the v andy magnetizations (usually ealled the u- and v-mode signals), in the presenee of a weak radiofteqiieney (RF) field, fi, are given in equation (B2.4.2) ). [Pg.2094]

According to the solution of the Bloch equations (Chapter 5), the magnetic resonance absorption, sometimes called the v-mode signal , v, is given by eqn (1.10). [Pg.12]

There are two components of the transverse nuclear magnetization one in phase with the field H, and one ir/2 out of phase with Hi. The former is known as the dispersion mode or u mode magnetization, and the latter as the absorption mode or v mode magnetization. That is, referring to Fig. 2, will lag or lead Hi as the resonance is traversed. The magnetic radiofrequency susceptibilities are defined by... [Pg.39]

In summary, the assignments favored by us for these single hydride-bridged-carbonyl anions are ca. 1700 cm-1 for 3, ca. 850 cm-1 for v2, and <150 cm-1 for v. Alternatively, the v mode can be near that of v2 in the 900-700 cm-1 region. However, we do not favor this assignment because it does not provide a ready explanation for the high frequency modes, which cannot be explained as overtones. Further confirmation of our preferred assignments can be obtained from normal mode calculations. [Pg.250]

Due to the quadratic form of eq. (1.37), the magnitude spectrum is phase independent, and a manipulated signal noise improvement relative to the pure u and v modes is attained (Fig. 2.14). If only magnitude information is desired, phase correction is not necessary, and P(v) can be computed immediately after Fourier transformation. [Pg.36]

Watanabe T, Suzuki T, Izaki K (1991) New Polyenic Antibiotics Active Against Gram-Positive and Gram-Negative Bacteria V. Mode of Action of Enacyloxin Ila. J Antibiot 44 1457... [Pg.418]

Fig. 5.6. Principal block diagram of the electronic unit. (1) Signal generation, (2) amplification of /photo, (3) controller for CC mode, (4) dc voltage sweep for I/V mode and (5) communication interface. Fig. 5.6. Principal block diagram of the electronic unit. (1) Signal generation, (2) amplification of /photo, (3) controller for CC mode, (4) dc voltage sweep for I/V mode and (5) communication interface.
Fig. 4. The emission and excitation spectra of the luminescence of Cs2NaYCl6 Bi3+ at 5 K. The zero-phonon line (0-0) and the progression in the v, mode are indicated at the top. See also Table 1. After A.C. van der Steen, thesis, Utrecht (1980)... Fig. 4. The emission and excitation spectra of the luminescence of Cs2NaYCl6 Bi3+ at 5 K. The zero-phonon line (0-0) and the progression in the v, mode are indicated at the top. See also Table 1. After A.C. van der Steen, thesis, Utrecht (1980)...
Given the illustrations of the normal modes of a molecule, it is possible to identify their symmetry species from the character table. Each non-degenerate normal mode can be regarded as a basis, and the effects of all symmetry operations of the molecular point group on it are to be considered. For instance, the v mode of XeF4 is invariant to all symmetry operations, i.e. R(v 1) = (l)vj for all values of R. Since the characters are all equal to 1, v belongs to symmetry species Aig. For V2, the symmetry operation C4 leads to a character of -1, as shown below ... [Pg.243]

It must, however, be borne in mind that minor shifts and weak splittings of the IR bands may arise on account of lowering of site symmetry because of strong lattice effects or of coupling of vibrations between perchlorate groups or from a purely isotopic effect within the group (15, 16). For example, the broad and strong band due to the v mode of ionic perchlorate is often split because of lattice effects. Despite these limitations, with a little care and caution, coordinated and noncoordinated perchlorate(s) are conveniently identified by IR spectroscopy. [Pg.258]

An experimental demonstration is depicted in Fig. 8 for the v mode of neat bromochloromethane (45). Part of the data of Fig. 5b are replotted in Fig. 8a with an enlarged ordinate scale. We recall that the anisotropic component (dotted line in Fig. 5b) is negligible for the special case here,... [Pg.35]

Measurements of the concentration dependence allow one to uniquely separate the dephasing contribution via concentration fluctuations in the solvation layer of the vibrating CH3I molecule, the time scale of which is determined to be 3.2-1.1 ps in the temperature range 242-374 K. Striking deviations from simple exponential relaxation dynamics are reported for the v, mode with correlation times rc > 1 ps, indicating the intermediate case for this relaxation mechanism (46). [Pg.40]

The amide V mode is largely an NH out-of-plane bend with some CN torsion. [Pg.238]

Fig. 4. Calculated intensity distribution of the light scattering by liquid crystalline solution of PBLG. kill = 200, bfIS = 0.45 u> = 0 . Upper, the V, mode lower, the Hh mode. Direction of the orientation horizontal... Fig. 4. Calculated intensity distribution of the light scattering by liquid crystalline solution of PBLG. kill = 200, bfIS = 0.45 u> = 0 . Upper, the V, mode lower, the Hh mode. Direction of the orientation horizontal...
In PBLG-chloroform preparation, the V, mode often shows the (f —90 pattern under no external field, showing that the maximum polarizabili direction of the molecular cluster is at 45° with respect to the cluster axis (see Section II). Even in such a case, this pattern turns to the 45 pattern in external lds the 45 Vn pattern is often seen in liquid crystalline solutions when shearing stresses are suspected to have operated on the solutioiL... [Pg.97]

Table 4.5-1 finally provides some information concerning the LO-TO behavior of the bands. It ranges from as little as several cm in the case of nearly non-polar modes such as Vi, to about 150 cm" in the case of the highly polar v mode in both crystalline phases. [Pg.322]

The patterns of intensities can be understood on the basis of how much a given vibrational motion changes the molecular dipole moment. The donor bend, for example, acquires its high intensity because it turns the HF molecule with its large molecular moment in such a way as to give the complex a nonzero moment perpendicular to the H-bond axis. In contrast, the stretch of the two subunits away from each other in the v mode does little to... [Pg.151]

Anharmonicity corrections can be quite large in complexes of this type, up to several hundred cm k In FH- NHj and CIH—NH3, for example, the anharmonic v, frequency is lower than the harmonic value by about 400 cm . It is interesting also that whereas correlation lowers the v frequency, it has the opposite effect of increasing v. Nor can one expect cancellation to occur between anharmonic and correlation effects in some cases, the two can be additive. Mechanical anharmonicity leads to a progressively smaller spacing between successive overtones of the v mode as the quantum number increases. [Pg.199]

Fig. 1 Normal vibrational modes for Hj. The totally symmetric v, mode (3178.3 cm" ) is Raman active and infrared inactive. The degenerate mode (2521.3 cm" ) is infrared active. Fig. 1 Normal vibrational modes for Hj. The totally symmetric v, mode (3178.3 cm" ) is Raman active and infrared inactive. The degenerate mode (2521.3 cm" ) is infrared active.
Other substances whose Raman spectra have been interpreted in terms of the v, modes are listed in Table 3-XXIII. [Pg.135]

F. G. Baglin, U. Zimmerman, and H. Versmold. Higher-order collision induced Raman scattering from the dipole forbidden v, mode of ethane. Molec. Phys., 52 877-890 (1984). [Pg.497]

The doubly degenerate nontotally symmetric v, mode (411.3cm ) is modeled using two one-dimensional modes which have the same wavenumber for the ground electronic state and by two inverted harmonic oscillator surfaces for the excited electronic state. A value of 190 cm is used for the inverted harmonic oscillator in this calculation. [Pg.195]

Fig. 2.3 HREELS spectra after NO dosing (in Langmuir (L)) on the (3 2 x V2) R45° Sn/Pt(100) alloy at 100 K [34]. After low NO exposures, a Vj peak at 1666 cm was observed from bent-atop NO. Higher NO exposure led to the appearance of a very broad peak at 1816 cmwhich can be decomposed into two peaks centered at 1821 and 1698 cmas shown in the inset. These two peaks were assigned to a surface dinitrosyl complex. Formation of adsorbed N O from the reaction of adsorbed NO, via a dinitrosyl intermediate, occurs at 100 K, as evidenced by the peaks at 580, 1234, and 2238 cm, which are assignments for the three normal modes of linear N O molecules N-N-0 bending N-N-O stretching (v ), and N-N stretching (v ) modes, respectively. Fig. 2.3 HREELS spectra after NO dosing (in Langmuir (L)) on the (3 2 x V2) R45° Sn/Pt(100) alloy at 100 K [34]. After low NO exposures, a Vj peak at 1666 cm was observed from bent-atop NO. Higher NO exposure led to the appearance of a very broad peak at 1816 cmwhich can be decomposed into two peaks centered at 1821 and 1698 cmas shown in the inset. These two peaks were assigned to a surface dinitrosyl complex. Formation of adsorbed N O from the reaction of adsorbed NO, via a dinitrosyl intermediate, occurs at 100 K, as evidenced by the peaks at 580, 1234, and 2238 cm, which are assignments for the three normal modes of linear N O molecules N-N-0 bending N-N-O stretching (v ), and N-N stretching (v ) modes, respectively.
Corrosion rate values were calculated from the mass loss of each test presenting a statistical array and indicating corrosion rate ordered array average value v, mode value vmode, median value vmediam and standard deviation s. [Pg.122]

A parameter that has been widely used in the study of the structure and thermal properties of solid organic materials (13-16) and particularly coals (14-16) is the NMR second moment. To compute such a parameter from our solid echo data requires its Fourier transformation from the time domain to obtain a complex frequency domain NMR spectrum, i.e. g (v) u (v) + iv (v). The quadrature components of this spectrum represent linear combinations of the pure absorptive (u(v)) and dispersive (v(v)) modes of the true spectrum, i.e,... [Pg.361]

For Zn(phen)(H20)V206 and Ti(bipy)V207, IR spectra gave assignments to vV=0 and vV-O-V modes.136,137 The IR spectra of V16Nb0.4O5 and Vo 3Nb1705 show that the number of V=0 bands decreases with increased addition of Nb.138 The IR spectra of MxOy+, where M = V, Nb or Ta, x = 3, 4 or 6, show that for M = V, the bands are 20 10 cm-1 lower than for M = Nb or Ta (which show very similar wavenumbers).139... [Pg.260]


See other pages where V-mode is mentioned: [Pg.96]    [Pg.148]    [Pg.272]    [Pg.14]    [Pg.35]    [Pg.42]    [Pg.77]    [Pg.155]    [Pg.35]    [Pg.134]    [Pg.98]    [Pg.784]    [Pg.217]    [Pg.99]    [Pg.168]    [Pg.184]    [Pg.338]    [Pg.397]    [Pg.391]    [Pg.193]    [Pg.134]    [Pg.258]   
See also in sourсe #XX -- [ Pg.14 ]




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