Heterogeneous fluorescence decay of (4. fwdarw. 6)-and (4. fwdarw. 8

Feb 27, 1987 - about 0.01% of the main peak, but it does not interferewith minor component detection at the 0.01% level because of the broad flat-topp...
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6614

J . Am. Chem. SOC.1987, 109, 6614-6619

In this study, the integrated intensity of spinning sidebands was one. In this paper we have used I3C N M R of samples of natural minimized by careful magnet homogeneity adjustments," and then isotopic composition, a low-sensitivity technique. Each spectrum the height of the sidebands was further diminished by modulation of Figure 2 required less than 4 min signal averaging time, because of vs,15 in the range 10-20 Hz. The resulting spinning sidebands the proportion of the minor component (2) was 20.4% of that of have a flat-top shape. The one at +vs is barely visible in Figure the major one (l),but about 1 week of instrument time was used 1A as a base line rise in the 10-20 Hz range. It has a height of to observe 0.01% of 2 (Figure 1). However, detection of minor about 0.01% of the main peak, but it does not interfere with minor components at the 0.01% level by natural-abundance 13CN M R component detection at the 0.01% level because of the broad can be achieved with just overnight data accumulation if the flat-topped shape. molecules are much larger than 1 and 2, so that they have T I Cyclic sidebands caused by WALTZ- 16 proton d e ~ o u p l i n g ~ ~ ~ ~values * shorter than 1 s44 instead of the 20 s T I of 1, because then were detected, outside the spectral range shown in Figure 1. They the acquisition time per scan can be diminished from the 5 5 s used had a peak height less than 0.1% of that of the main resonance. in this paper to 5 s or less. The resulting loss in digital resolution Other spurious peaks occurred a t frequencies related to that of is not a problem because Wo > 0.32 Hz when T , < 1 s. Furthe main resonance ( y o ) , defined here as the difference between thermore, the signal-to-noiseratio per scan can be greatly increased the resonance frequency and the phase detection carrier frequency, by going from our low magnetic field (50-MHz I3C and 200-MHz and the Nyquist frequency (vN),equal to half of the full spectral 'H resonance frequencies) to high-field instruments (1 25-MHz width when quadrature detection is used. We observed small I3C and 500-MHz 'H resonance frequencies), which should yield (