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Half-time reversible system

For the excitation of DQC under MAS, the interference with the sample rotation must be considered, as was the case for the CRAMPS experiment discussed in the previous section. In particular, if a sequence designed for a static MQ experiment is used without modification, the excitation (and reconversion) time is limited to ttr/2, since the rotor modulation causes the action of the pulse sequence in the second half of the rotor period to be the time reversal of that which occurred in the first half of the rotor period. Starting with the suggestion of Meier and Earl,89,90 who simply proposed the phase switching of the static sequences used by Baum et al.,47,48 every half rotor period to prevent the process of self-time-reversal, many different approaches have been presented that allow excitation (and reconversion) times of one or more rotor periods. Such pulse sequences that counteract the effect of MAS are referred to as recoupling methods,1112 examples that have been used in homonuclear DQ MAS NMR spectroscopy include BABA,91 C7,92 DRAMA,93 DRAWS,94 and HORROR.95 We note that Levitt and co-workers have recently introduced a very helpful classification system, based on symmetry principles, which covers such sequences.96,97... [Pg.432]

Degradation and evaporation seem to be the major pathways for acrolein loss in water smaller amounts are lost through absorption and uptake by aquatic organisms and sediments. The half-time persistence of acrolein in freshwater is 38 h at pH 8.6, and 50 h at pH 6.6 degradation is more rapid when initial acrolein concentrations are less than 3000.0 pg/L. Acrolein has a half-time persistence of 2.9-11.3 h at initial nominal concentrations of 20.0 pg/L, and 27.1-27.8h at 101.0pg/L. At pH 5, acrolein reacts by reversible hydrolysis to produce an equilibrium mixture with 92% beta-hydroxypropionaldehyde and 8% acrolein in alkali, the primary reaction is consistent with a polycondensation reaction. Microbial degradation plays a major role in the ttans-formation of aaolein in aquatic systems. In natural waters, acrolein degradation proceeds to carboxylic acid via a microbial pathway beta-hydroxypropionaldehyde is readily biotransformed in about 17.4 days. [Pg.5]

There are well-defined criteria for this "reversible" system in terms of peak separation, wave shape, etc. and the maximum current scales inversely with the square root of the scan rate. The half-wave potential of a "reversible" redox process may readily be obtained from the voltammogram. If, however, the electron transfer produces a species that is chemically reactive on the experimental time scale, then the return wave is missing and the peak potential shifts as a function of the kinetics of the follow-up processes. The peak is not as well defined, and without a proper return wave it is now not straightforward to obtain thermodynamic half-wave potentials from the trace of such an irreversible system. Furthermore, if a disk electrode is used of micrometer-dimensions, then hemispherical diffusion now takes place and a sigmoidal current-potential curve is obtained [Fig. 4(b)]. [Pg.271]

For a system with fermion symmetry—that is, half-integer spin— the wave function cannot therefore be invariant under time reversal. Further, the time-reversed wave function cannot be a simple multiple of the original. [Pg.96]


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See also in sourсe #XX -- [ Pg.7 ]




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Half-time

Reverse system

Reverse-time

Time reversal

Time-reverse system

Time-reversibility

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