The biological applications of 13C magnetic resonance spectroscopy are well known ( 1-5). Recently, there was evidence (6-9) suggesting that the citrate peak in the 13C spectrum may be useful as a marker for human prostate cancer. It was found in human prostate that the citrate concentration is small in the normal gland, negligible in ma lignant tumors (8)) and increased markedly in tissues with benign prostatic hypertrophy (BPH) (8, 9). Wh ile this evidence suggests citrate as possibly a specific marker for ma lignant prostatic tumor and BPH, it also underscores the problem in applying NMR spectroscopic techniques without localization under in vivo conditions where prostatic ma lignancy is often, if not always, accompanied by BPH. There are two possible solutions to the above problem. One is through mu ltidimensional chemical-shift imaging ( 10, I I ) and the other, localized spectroscopy. For carbon, either one of these two approaches presents many challenging problems. F irst, one must deal with the problem of low sensitivity and long T1. Second, because carbon has a low y, one needs four times as much gradient strength in imaging or localization of carbon as that of hydrogen. Third, since carbon has large chemical shifts, it is often difficult to separate the spatial from the spectral information. By using polarization transfer techniques, such as INEPT ( 12,13) or DEPT ( 14,15), the problems associated with low y nuclei, such as carbon, are converted into those of protons which are much easier to solve. Recently this idea was exploited by Norris et al. ( 16)) who applied a one-dimensional ISIS sequence ( 17) on the protons for the localization of carbon. In this Communication, we will demonstrate an alternative technique of carbon selection based on the idea ment ioned above and the conventional p lane excitation method commonly used in proton imaging. In this scheme, plane selection of carbon is obtained by selective proton enhancement. We will also demonstrate that one can gain a similar type of enhancement in carbon imaging by applying phase encoding on the proton, instead of the carbon, polarization. We shall call this an indirect spinwarp method. F igure 1 shows the method of localization of carbon by selective enhancement through excitation of hydrogen. The RF section of the pulse sequence in F ig. 1 is a DEPT sequence with a shaped proton 7r/2 pulse. Since the phase-cycl ing scheme of the DEPT sequence is so designed that only the proton-enhanced nuclei are observed
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