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Lee-Goldburg

In the solid, dynamics occurring within the kHz frequency scale can be examined by line-shape analysis of 2H or 13C (or 15N) NMR spectra by respective quadrupolar and CSA interactions, isotropic peaks16,59-62 or dipolar couplings based on dipolar chemical shift correlation experiments.63-65 In the former, tyrosine or phenylalanine dynamics of Leu-enkephalin are examined at frequencies of 103-104 Hz by 2H NMR of deuterated samples and at 1.3 x 102 Hz by 13C CPMAS, respectively.60-62 In the latter, dipolar interactions between the 1H-1H and 1H-13C (or 3H-15N) pairs are determined by a 2D-MAS SLF technique such as wide-line separation (WISE)63 and dipolar chemical shift separation (DIP-SHIFT)64,65 or Lee-Goldburg CP (LGCP) NMR,66 respectively. In the WISE experiment, the XH wide-line spectrum of the blend polymers consists of a rather featureless superposition of components with different dipolar widths which can be separated in the second frequency dimension and related to structural units according to their 13C chemical shifts.63... [Pg.15]

A. Bielecki, A.C. Kolbert, H.J.M. de Groot, R.G. Griffin, and M.H. Levitt. Frequency-Switched Lee-Goldburg Sequences in Solids. In W. S. Warren, editor, Adv. Magn. Reson., volume 14, pages 111-124. Academic Press, New York, 1990. [Pg.279]

Frequency-switched Lee-Goldburg (FSLG) 13C-1H heteronuclear correlation (HETCOR) experiments... [Pg.41]

Fig. 18. The pulse sequence for measuring the 2D heteronuclear correlation NMR spectrum with frequency-switched Lee-Goldburg irradiation during the evolution. Fig. 18. The pulse sequence for measuring the 2D heteronuclear correlation NMR spectrum with frequency-switched Lee-Goldburg irradiation during the evolution.
Figure 13 Pulse sequence for the solid-state 31P—1H frequency-switched Lee-Goldburg (FSLG) experiment. Proton-proton homonuclear decoupling was performed by using the FSLG decoupling sequence. Quadrature detection in Wi was achieved by using the TPPI method. During the acquisition period, TPPM heteronuclear decoupling was applied. Figure 13 Pulse sequence for the solid-state 31P—1H frequency-switched Lee-Goldburg (FSLG) experiment. Proton-proton homonuclear decoupling was performed by using the FSLG decoupling sequence. Quadrature detection in Wi was achieved by using the TPPI method. During the acquisition period, TPPM heteronuclear decoupling was applied.
The Lee-Goldburg (LG) irradiation scheme achieves spin-space averaging by an off-resonance irradiation, such that the spins rotate in the off-resonance rotating frame around a direction inclined at an angle Om = 54.7° with respect to the direction of the external magnetic field. In effect, the same angle is achieved... [Pg.42]

Recently, Vega and co-workers have presented a phase-modulated Lee-Goldburg experiment (PMLG) experiment, in which only the phase of a series of adjacent pulses is changed, i.e., a i remains constant.76 77 In an ingenious reinterpretation of the LG concept, the zero-order term in the average Hamiltonian can be shown to vanish when the modulation of the pulse phase described by... [Pg.430]

Using Lee-Goldburg based decoupling methods, a fwhmh of 150—170 Hz has been reported for the aliphatic H resonances in L-alanine78—this is demonstrated in part c of Figure 5, where, for comparison, the (a) static and (b) MAS (pr = 30 kHz) spectra are also shown. The spectrum in Figure 5c was recorded... [Pg.430]

E. Vinogradov. P. K. Madhu and S. Vega, Proton spectroscopy in solid state nuclear magnetic resonance with windowed phase modulated Lee-Goldburg decoupling sequences. Chem. Phys. Lett., 2002, 354, 193-202. [Pg.291]

Fig. 5. (A) Vector picture describing the relationship between the rf field strength and offset frequency in off-resonance experiments such as LGCP and PISEMA. (B) A simple pulse sequence (called LGCP or FFLGCP) to set-up the Lee-Goldburg condition. As explained in the text, this sequence can be used to determine the S-spin-lock field strength that matches ileff./for the effective spin exchange between / and S spins. Fig. 5. (A) Vector picture describing the relationship between the rf field strength and offset frequency in off-resonance experiments such as LGCP and PISEMA. (B) A simple pulse sequence (called LGCP or FFLGCP) to set-up the Lee-Goldburg condition. As explained in the text, this sequence can be used to determine the S-spin-lock field strength that matches ileff./for the effective spin exchange between / and S spins.
Fig. 18. Proton-detected ID PISEMA spectra of a powder sample of A-acetyl- A-D,L-valine obtained using the pulse sequence shown in Fig. 17 under static condition. The experiments were performed with a H Lee-Goldburg spin-lock RF power of... Fig. 18. Proton-detected ID PISEMA spectra of a powder sample of A-acetyl- A-D,L-valine obtained using the pulse sequence shown in Fig. 17 under static condition. The experiments were performed with a H Lee-Goldburg spin-lock RF power of...
A new 3D experiment that allows direct probing of proton spin-diffusion process between resolved proton spectra obtained under Lee-Goldburg homo-nuclear decoupling has been reported. It is anticipated that this class of experiments will soon be used to study poorly crystalline hybrid materials as well as finely divided or porous inorganic materials. [Pg.231]


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See also in sourсe #XX -- [ Pg.35 ]




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Frequency-switched Lee-Goldburg

Frequency-switched Lee-Goldburg decoupling

Lee and Goldburg

Lee-Goldburg experiment

Lee—Goldburg cross-polarization

Phase-modulated Lee-Goldburg

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