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In-phase mode

For 2D spectra to be displayed in phased mode, choose the Manual phase correction option from the Process pull-down menu of 2D WIN-NMR. This will also change the info field of the button panel and disable some of the panel buttons (Fig. 5.7). [Pg.163]

Figure 27. Dipolar coupling of asymmetric stretching in side-by-side C02 dimer. For this configuration, unfavorable electrostatic interaction shifts the intense in-phase mode of a degenerate pair (a) to higher frequency. At the same time, the weak out-of-phase mode (b) shifts to lower frequency. From Ref. 87 with permission from Elsevier Science Publishers. Figure 27. Dipolar coupling of asymmetric stretching in side-by-side C02 dimer. For this configuration, unfavorable electrostatic interaction shifts the intense in-phase mode of a degenerate pair (a) to higher frequency. At the same time, the weak out-of-phase mode (b) shifts to lower frequency. From Ref. 87 with permission from Elsevier Science Publishers.
For the three smallest islands - containing 7, 19 and 37 CO molecules - the full vibrational eigen value problem was solved to yield dipole shifts relative to the singleton of 12, 17 and 20 cm-1 respectively. In addition, it was found that for these small islands certain vibrational modes other than the fully in-phase mode have non-zero intensity, and in each case bands having an intensity of a few percent of the major band s appear at lower frequency. [Pg.70]

In Fig.3 the energy of the in-phase mode is normalized to the Big phonon energy in order to cancel uncertainties in the amount of 160 substituted by 180. It is clear that the in-phase phonon shows a decreasing amount of anharmonicity for x>6.5 and the anharmonicity disappears completely at optimal doping. On the other hand, there is anharmonicity at lower oxygen concentrations, which may originate from the coexistence of chain-ordering phases... [Pg.121]

In the most simple case where only a pair of adsorbed CO s are considered, dipole-dipole interactions would lead to coupling and produce an in-phase mode 0 0, and an out-of-phase mode, 0 0. The... [Pg.188]

The restriction that any new unit must be operated in the same manner for all products is removed An operating mode different from an existing mode can be considered Introduction of the "group" concept the out-of-phase mode and the in-phase mode operations are merged into a generalized superstructure... [Pg.232]

Fig. 102. Upper part oxygen content vs. Ca%. Lower part comparison of the relative intensity of the Raman in-phase modes 429/(429+439) vs. Ca% with the A-B transitions of the oxygen content. The 439 cm" mode is a new mode appearing with the Ca doping however, it does not scale with Ca and it seems to scale with O. After Palles (2000) and Palles et al. (2000b). Fig. 102. Upper part oxygen content vs. Ca%. Lower part comparison of the relative intensity of the Raman in-phase modes 429/(429+439) vs. Ca% with the A-B transitions of the oxygen content. The 439 cm" mode is a new mode appearing with the Ca doping however, it does not scale with Ca and it seems to scale with O. After Palles (2000) and Palles et al. (2000b).
Figure 106 shows that the relative intensity of the Raman in-phase mode ratio 429/(429-h439) (cf fig. 102) scales well with T 2, indicating that the splitting of the... [Pg.158]

Phase imaging In phase mode imaging, the phase shift of the oscillating cantilever relative to the driving signal is measured. This phase shift can be correlated with specific material properties that affect sample-tip interaction. The phase shift can be used to differentiate areas on a sample with such differing properties as friction, adhesion, and viscoelasticity. Because the technique can be used simultaneously with DFM, topography can also be measured. [Pg.241]

Figure 23.2. Scheme of the function of the SCORIM procedure along with the three basic inodes of operations (A, B and C) - Mode A the pistons are activated 180° out of phase Mode B the pistons are activated in phase Mode C the pistons are held down at a constant pressure [15]... [Pg.742]

GTG defect. CH2 wagging. -CH2(G)-CH2(T)-CH2(G )-. This defect introduces two wagging modes because the two CHt groups are joined by a bond in trans conformation and are partly decoupled from the host lattice by the gauche bonds. The intra-defect coupling generates out-of-phase and in-phase modes calculated (and observed) near 1375 and 1306 cm . [Pg.143]

Since dispersion curves have been clearly discussed in Sections 3.5 and 3.6, the concepts which form the grounds of LAM spectroscopy can be easily defined. Let us consider an a -trans polymethylene chain and focus our attention on the branch cu8 of the phonon dispersion curve. The branch starts as mostly C-C stretching and ends as CCC bending. For a finite chain of N chemical units we expect to locate on this branch a band progression of N vibrational modes characterized by the phase coupling pj = jn/N. The most in-phase mode occurs at very small frequencies its frequency approaches zero when the chain tends to be of infinite length. Let 1,2,3. .. N label the components of the band progression of the modes which lie on the co% branch. [Pg.161]

In the out-of-phase deformation mode, the matrix is loaded in tension and compression, in the in-phase mode, it is sheared. Because of this, the modes are sometimes called extension mode and shear mode. Except at small volume fractions of the fibre, the strength of the composite is smaller in in-phase deformation which is thus the mode of interest. If a purely elastic deformation of the matrix is assumed, the calculated strength values for the composite are very large, but the observed values are usually much smaller. In metal and polymer matrix composites, the matrix deforms plastically in the in-phase mode. If we make the simplifying assumption that the matrix is perfectly plastic with a yield strength of the compressive strength is [122]... [Pg.314]

Figure 20.4 AFM image in phase mode of the self-assembled lamellar structure of PS-b-PGA block copolymers. (Reprinted with permission from J. Babin, D. Taton, M. Brinkmann and S. Lecommandoux, Synthesis and self-assembly in bulk of linear and mikto-arm star block copolymers based on polystyrene and poly(glutamic acid), Macromolecules, 41, 4, 1384-1392, 2008. 2008 American Chemical Society.)... Figure 20.4 AFM image in phase mode of the self-assembled lamellar structure of PS-b-PGA block copolymers. (Reprinted with permission from J. Babin, D. Taton, M. Brinkmann and S. Lecommandoux, Synthesis and self-assembly in bulk of linear and mikto-arm star block copolymers based on polystyrene and poly(glutamic acid), Macromolecules, 41, 4, 1384-1392, 2008. 2008 American Chemical Society.)...
The out-of-plane C—H bends are weakly coupled and largely C—X insensitive. Inasmuch as the all-in-phase mode is modestly sensitive only to the number of C H oscillators mutually adjacent, it is often possible to establish the substitution pattern of a ring system simply by the assignment of this mode alone. [Pg.123]


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See also in sourсe #XX -- [ Pg.152 ]




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Ferroelectric modes in chiral smectic C* phase

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