A quadrature transmit/receive coil for proton-decoupled An ideal coil configuration for in vivo proton-decoupled NMR spectroscopy requires a highly sensitive 13 C coil as 13 C or 31 P spectroscopy half-volume applications, which retains optimal performance on the 1 H frequency, was built. well as an efficient proton-decoupling coil. Ideally, those coils have very similar areas of sensitivity, yet show no Specifically, no RF field profile distortions due to coil interactions were observed. This and the quadrature 1 H coil de-significant electromagnetic interaction or degenerated field patterns. Both aims are especially difficult to achieve sign resulted in a fourfold improvement in the power requirements over conventional, linear-polarized designs. A single for 13 C applications, since the quarter wavelength of 13 C is very close to the 1 H wavelength. In addition, since the lowpass filter of 00.1 dB insertion loss was sufficient for broadband proton decoupling experiments on a 4 T whole-power absorption increases with B 2 0 , the proton-coil effibody system. Images and spectra show excellent sensitivity ciency may determine the feasibility of decoupling within at both frequencies. Broadband decoupling depicting narrow the FDA guidelines ( 2 -7 ) . metabolite resonances from glutamate, taurine, and creatine Several surface-coil configurations have been used for in the human leg and human brain was possible within FDA broadband-decoupled 13 C MRS in humans (4,(8)(9)(10)(11)(12)(13). Many guidelines for power absorption.applications successfully used two concentric circular surProton decoupling is a necessary requirement to achieve face coils (8-10). A serious drawback of such a configuraoptimal sensitivity for 13 C MR spectroscopy (MRS) and tion is the inherent 1 H flux blockage of the inner 13 C coil, may provide substantial improvements for 31 P MRS. NOE since the 13 C coil is almost short-circuited at the 1 H frequency generation can enhance sensitivity up to threefold for 13 C (9). Consequently the proton-coil performance is rather poor MRS. To a lesser extend, the same holds true for 31 P MRS, adjacent to the 13 C coil, resulting in excessive power requirements for proton decoupling. Despite these drawbacks, conin that 1 H decoupling can increase spectral resolution, especially in the PME and PDE resonances at low magnetic centric coil design was not prohibitive for some clinical applications using small coils at 4.7 T (14) as well as at fields (1), and improved signal-to-noise ratio (SNR) can be obtained by NOE generation. These heteronuclear tech-1.5-2.1 T (15, 16). However, for the volumes needed for human applications at 4 T, we found that the performance niques use relatively long and intense RF irradiation at the 1 H frequency, which can make it difficult to achieve decou-of the proton coil in a double concentric arrangement was not sufficient for decoupling within FDA guidelines. pling in humans within FDA guidelines for power absorption. Both NOE generation and proton decoupling perform Alternatively,...