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Difference decoupling

One of the most useful proton nuclear magnetic resonance ( H-NMR) one-dimensional (a single-frequency axis) techniques to be applied in structure determination is difference spectroscopy. This approach involves subtracting a spectrum obtained under the conditions of some perturbation from a normal, unperturbed spectrum. The resulting difference spectrum reveals the spectral changes caused by the perturbation, whereas those signals that remain unaffected are nulled. The perturbation can be a decoupling irradiation, a nuclear Overhauser enhancement, or even a population transfer experiment (135, 328). [Pg.60]

12-H decoupled peaks in Fig. 2.26C shows that 1.53t is due to axial 11)8-H and the 1.94 dd is due to equatorial lla-H. It is clear that such results could not have been obtained from straight decoupling experiments. [Pg.61]


Within a software design, the different levels of refinement are generally associated with different, decoupled layers in the software. We can see this, for example, in the conventional separation into business and GUI layers. We can also see it in communications protocols, from the individual bits up through to the secure movement of files and Web pages. [Pg.276]

ASM3 A variant of ASMl with a different, decoupled hydrolysis mechanism... [Pg.203]

Adding blocks of separately acquired FID.s together is recommended when studying unstable compounds or when using difference techniques (NOE-difference, decoupling difference). In the former case, coaddition of blocks of data allows snapshots to be taken of the sample decomposing whilst in the latter case it minimizes effects caused by spectrometer instability and so improves the visibility of the very small difference effects. [Pg.172]

With modern Bruker spectrometers the selective ID NOE experiment is usually performed in a pseudo 2D mode. The raw data is obtained as a 2D matrix with the individual rows (FIDs) corresponding to the different decoupler frequencies used for the selective perturbation plus one row where the decoupler frequency is set well away from any resonance line (reference FID). Consequently this 2D data matrix must first be decomposed into the individual 1D FIDs before the difference FIDs can be calculated. [Pg.199]

The Orbital Picture of Resonances from different Decouplings of the Dilated Electron Propagator... [Pg.224]

The 2P shape resonance in e-Be scattering has served as the test case for almost all the theoretical approaches to the treatment of electron scattering resonances and the earliest applications of the dilated electron propagator have also focused on this system /21,26,40/. Theta trajectories from different decouplings of the bi-orthogonal dilated electron propagator are displayed in fig. 4. The optimal value of a = 0.75 has been determined through a separate a-trajectory /26/. [Pg.244]

Figure 7. Resonant trajectories from different decouplings for JVj using the (a) (5s 4p 2d) and (h) (4s 9p) bases. The resonance energy from the decouplings devoid of orbital relaxation (E°, E3, it almost same but markedly different from that given by the... Figure 7. Resonant trajectories from different decouplings for JVj using the (a) (5s 4p 2d) and (h) (4s 9p) bases. The resonance energy from the decouplings devoid of orbital relaxation (E°, E3, it almost same but markedly different from that given by the...
The resonant -trajectories from different decouplings are displayed in figs. 8a and 8b where it is seen that optimal value of the radial scale factor a is different for the methods with (E2 and E2ph TDA) and without (E°, E2, E2ph TDA) orbital relaxation. [Pg.256]

Figure S. Resonant trajectories from different decouplings for CO. The radial scale factor required to unmask the resonance using the E°, Ej and decouplings (a) is different... Figure S. Resonant trajectories from different decouplings for CO. The radial scale factor required to unmask the resonance using the E°, Ej and decouplings (a) is different...
The value for resonance energy calculated using the bi-orthogonal dilated electron propagator is quite reasonable but the width of the 2II CO- using different decouplings is close only to that from the boomerang model. The... [Pg.257]

Figure 9. Resonant trajectories from different decouplings for CiH+. The lowering of LUMO energy by the decouplings incorporating orbital relaxation (3Ca and E1pi -tda) seen for this system as well. Figure 9. Resonant trajectories from different decouplings for CiH+. The lowering of LUMO energy by the decouplings incorporating orbital relaxation (3Ca and E1pi -tda) seen for this system as well.
Figure 14 Radial charge density plot from the orhital/Feynman-Dyson (FD) amplitude for the Ss orbital in Be from zeroth order (SCF ), the second order (E2 A) and diagonal 2ph-TDA decouplings /EJph-TDA ). On the scale employed in the main plot, distinguishing the orbital/FD amplitudes from different decouplings is not possible but in the inset the difference between radial charge densities from the second and zeroth order (bi-variaiional SCF) decouplings clearly reveals the role of correlation and relaxation effects in changing the ionization potential from 8.44 cV at the SCF level to 8.79 eV at second order. The maximum in the electron density is at imu = 2.1 a.u. Figure 14 Radial charge density plot from the orhital/Feynman-Dyson (FD) amplitude for the Ss orbital in Be from zeroth order (SCF ), the second order (E2 A) and diagonal 2ph-TDA decouplings /EJph-TDA ). On the scale employed in the main plot, distinguishing the orbital/FD amplitudes from different decouplings is not possible but in the inset the difference between radial charge densities from the second and zeroth order (bi-variaiional SCF) decouplings clearly reveals the role of correlation and relaxation effects in changing the ionization potential from 8.44 cV at the SCF level to 8.79 eV at second order. The maximum in the electron density is at imu = 2.1 a.u.
Figure 7 31P CP spectra for O-phospho-L-threonine spun at 60 kHz and recorded employing different decoupling sequences (A) cw (B) tppm (C) spinal and (D) xix. Figure 7 31P CP spectra for O-phospho-L-threonine spun at 60 kHz and recorded employing different decoupling sequences (A) cw (B) tppm (C) spinal and (D) xix.
The CP can be used with different decoupling sequences during the acquisition (these should also be optimized). [Pg.6190]

Before discussing the different decoupling pulse sequences, we should comment on the two following aspects. Let us first consider the zero-order effective Hamiltonian. Because fe// solely determined by the scaled isotropic chemical... [Pg.74]

Then, the absolute price decrease for the organic product is similar to the price decrease for the conventional product, but revenue reductions will generally be lower in organic than in conventional farming due to the yield difference. Decoupled compensatory payments will increase the relative competitiveness of organic farming. This is also the case if an organically produced product is sold conventionally. [Pg.332]

Fig. 9.8 Different manufacturing strategies related to different decoupling points, following Naylor et al. (1999)... Fig. 9.8 Different manufacturing strategies related to different decoupling points, following Naylor et al. (1999)...

See other pages where Difference decoupling is mentioned: [Pg.839]    [Pg.153]    [Pg.184]    [Pg.226]    [Pg.253]    [Pg.257]    [Pg.259]    [Pg.268]    [Pg.43]    [Pg.393]    [Pg.145]    [Pg.74]    [Pg.300]    [Pg.42]    [Pg.191]    [Pg.212]    [Pg.300]    [Pg.561]    [Pg.196]    [Pg.60]    [Pg.60]    [Pg.61]    [Pg.84]    [Pg.561]    [Pg.79]   
See also in sourсe #XX -- [ Pg.145 ]




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