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Hartmann-Hahn

The ID homonuclear Hartmann-Hahn (HOHAHA) experiment is an excellent way to determine complete coupled spin networks (18). The following pulse sequence is used ... [Pg.404]

Because of the complexity of the polyether antibiotics tittle progress has been made in stmcture determination by the chemical degradation route. X-ray methods were the techniques most successfully applied for the early stmcture elucidations. Monensin, X206, lasalocid, lysocellin, and salinomycin were included in nineteen distinct polyether x-ray analyses reported in 1983 (190). Use of mass spectrometry (191), and H (192) and nmr (141) are also reviewed. More recently, innovative developments in these latter techniques have resulted in increased applications for stmcture determinations. Eor example, heteronuclear multiple bond connectivity (hmbc) and homonuclear Hartmann-Hahn spectroscopy were used to solve the stmcture of portimicin (14) (193). East atom bombardment mass spectrometry was used in solving the stmctures of maduramicin alpha and co-factors (58). [Pg.172]

The transfer of magnetization from the proton spins to the carbon spins occurs now when the Hartmann-Hahn condition, Eq. (2), is fulfilled. [Pg.4]

Homonuclear Hartmann-Hahn Spectroscopy or Total Correlation Spectroscopy 267... [Pg.267]

HOMONUCLEAR HARTMANN-HAHN SPECTROSCOPY (HOHAHA), OR TOTAL CORRELATION SPECTROSCOPY (TOCSY)... [Pg.267]

We now want to turn to another experiment which, we must make clear at the start, does not have any relationship in theory to NOE experiments. In fact the theory is so complicated that we shall not say anything about it at all, but just refer you to one of the books in the Appendix. We are including this experiment because of its unique advantages when the spectrum has overlapping multiplets. It is called TOCSY, which stands for Total Correlation SpectroscopY (it has a second, more amusing name HOHAHA, standing for HOmonuclear HArtmann-HAhn), and is of particular use when oligosaccharides or peptides are under study. [Pg.19]

In addition, the technique of cross polarization introduced and developed by Pines, Gibby and Waugh (9) is used to increase the signal-to-noise ratio of the spectrum. The proton magnetization is spin-locked along the y axis with a spin-locking field % and the carbons subjected to an RF pulse chosen such that the two fields fulfill the Hartmann-Hahn condition (10), equation [3] (Figure 2). [Pg.387]

The first example, also being the example introducing optimal control to solid-state NMR [40] and further elaborated on later [161], is optimal control versions of the DCP experiment. This experiment was a natural choice for numerical improvements as it is widely used and it is well known that this experiment is sensitive to offsets, rf mismatch relative to the MAS-modified Hartmann-Hahn condition, and rf inhomogeneity. In particular the two latter effects may reduce significantly the performance of 15N to 13C transfers, severely complicate setup of such experiments, and render these critically sensitive to altered tuning/rf conditions in the course of potentially long experiments for biological samples. [Pg.38]

The spin-locking and CP behavior of the most commonly used SQ coherence (CT) in quadrupolar nuclei under static and MAS conditions has been described in detail by Vega using the fictitious spin-1/2 approximation [223]. In a static sample, the Hartmann-Hahn matching condition requires that co = nut where co ut is one of the nutation frequencies associated with the SQ coherence of the quadrupolar S spin (see Sect. 2.3.4). In the simple case of on-resonance SQ-CP this translates to [224]... [Pg.166]

Fig. 17 Efficiency of H — nB CPMAS in borax measured as a function of co (Hartmann-Hahn matching curve). The spectra were measured on-resonance at 9.4 T using = 6 kHz,... Fig. 17 Efficiency of H — nB CPMAS in borax measured as a function of co (Hartmann-Hahn matching curve). The spectra were measured on-resonance at 9.4 T using = 6 kHz,...
The Hartmann-Hahn MQ-CP transfer can be achieved when the rf frequency of spin I in the rotating frame is sufficiently close to one of the SQ or MQ nutation frequencies of spin S, co/ut = oJlf. In the case O/ > co/f, the nutation frequency for a symmetric MQ coherence of order p is given by [222, 229]... [Pg.169]

Under MAS, the Hartmann-Hahn condition for 3Q-CPMAS of spin-3/2 nuclei can be written as... [Pg.170]

The basic components of the solid state spectrometer are the same as the solution-phase instrument data system, pulse programmer, observe and decoupler transmitters, magnetic system, and probes. In addition, high-power amplifiers are required for the two transmitters and a pneumatic spinning unit to achieve the necessary spin rates for MAS. Normally, the observe transmitter for 13C work requires broadband amplification of approximately 400 W of power for a 5.87-T, 250-MHz instrument. The amplifier should have triggering capabilities so that only the radiofrequency (rf) pulse is amplified. This will minimize noise contributions to the measured spectrum. So that the Hartmann-Hahn condition may be achieved, the decoupler amplifier must produce an rf signal at one-fourth the power level of the observe channel for carbon work. [Pg.107]

Adamantane (C10H16) External referencing for 13C spectra, optimizing Hartmann-Hahn match, linewidth measurement, sensitivity measurement [30]... [Pg.112]

Hexamethylbenzene (Ci2H18) Optimizing Hartmann-Hahn match [30]... [Pg.112]

Hartmann-Hahn match, and cross-polarization mixing time are discussed in relation to obtaining quantitative NMR results. [Pg.118]

Homology modeling, 20 837 Homomenthyl salicylate, 22 16 physical properties of, 22 14t Homonuclear Hartmann-Hahn spectroscopy, 20 137 Homopolymerization, 10 183 of a-olelins, 16 110 ethene, 16 102-103 propene, 16 104-110 of VDC, 25 695-697 Homopolymers... [Pg.442]


See other pages where Hartmann-Hahn is mentioned: [Pg.482]    [Pg.67]    [Pg.176]    [Pg.267]    [Pg.268]    [Pg.268]    [Pg.268]    [Pg.567]    [Pg.212]    [Pg.8]    [Pg.66]    [Pg.166]    [Pg.167]    [Pg.168]    [Pg.168]    [Pg.170]    [Pg.205]    [Pg.105]    [Pg.116]    [Pg.118]    [Pg.105]    [Pg.309]    [Pg.85]   
See also in sourсe #XX -- [ Pg.223 ]




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Coupling constant, determination Hartmann-Hahn transfer experiments

Development of Hartmann-Hahn Mixing Sequences

HOHAHA Hartmann-Hahn spectroscopy

Hahne

Hartmann-Hahn Experiments

Hartmann-Hahn Transfer in Multispin Systems

Hartmann-Hahn condition

Hartmann-Hahn cross polarization

Hartmann-Hahn limit

Hartmann-Hahn match

Hartmann-Hahn match condition

Hartmann-Hahn matching

Hartmann-Hahn matching condition

Hartmann-Hahn matching experiment

Hartmann-Hahn mismatch

Hartmann-Hahn polarization transfer

Hartmann-Hahn spectroscopy

Hartmann-Hahn spectroscopy principle

Hartmann-Hahn transfer

Hartmann-Hahn transfer classification

Hartmann-Hahn transfer combination experiments

Hartmann-Hahn transfer coupling constant determination

Hartmann-Hahn transfer defined

Hartmann-Hahn transfer effective Hamiltonian

Hartmann-Hahn transfer effective coupling tensors

Hartmann-Hahn transfer evolution periods

Hartmann-Hahn transfer experiments

Hartmann-Hahn transfer frame

Hartmann-Hahn transfer mixing periods

Hartmann-Hahn transfer sequence

Heteronuclear Hartmann-Hahn Sequences

Heteronuclear Hartmann-Hahn Spectroscopy

Homonuclear Hartmann-Hahn

Homonuclear Hartmann-Hahn HOHAHA)

Homonuclear Hartmann-Hahn Sequences

Homonuclear Hartmann-Hahn principle

Homonuclear Hartmann-Hahn pulse sequence

Homonuclear Hartmann-Hahn spectroscopy

Homonuclear Hartmann-Hahn spectroscopy HOHAHA)

Homonuclear Hartmann-Hahn spectroscopy transfer

Practical Aspects of Hartmann-Hahn Experiments

Principle of Hartmann-Hahn Transfer

Selective Hartmann-Hahn coherence

Selective Hartmann-Hahn coherence transfer

Symmetry and Hartmann-Hahn Transfer

Total correlation spectroscopy homonuclear Hartmann-Hahn

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