Use of phased array coils for a determination of absolute metabolite concentrations

This work describes the use of phased array coils for a quantification of absolute metabolite concentrations. The method is demonstrated for single‐voxel localized proton MRS of human brain with an eight‐element receive‐only head coil. It is based on the transmitter reference amplitude of the body coil used for RF transmission. A relative sensitivity of every element of the phased array coil is derived from a combination of two reference scans without water suppression that correspond to either the body coil in transmit‐receive mode or the phased array coil in conjunction with body coil excitation. Experimental results were obtained at 2.9 T for both phantoms and 12 human subjects in different locations of gray and white matter. The data demonstrate that the procedure is technically robust and without a penalty in measuring time. Moreover, it takes full advantage of the signal‐to‐noise gain for quantitative proton MRS and may be extended to other phased array coils without the need for a recalibration. Magn Reson Med 53:3–8, 2005. © 2004 Wiley‐Liss, Inc.

[1]  van der Klink JJ The NMR reciprocity theorem for arbitrary probe geometry. , 2001, Journal of magnetic resonance.

[2]  Jürgen Gieseke,et al.  1H metabolite relaxation times at 3.0 tesla: Measurements of T1 and T2 values in normal brain and determination of regional differences in transverse relaxation , 2004, Journal of magnetic resonance imaging : JMRI.

[3]  G Helms,et al.  Analysis of 1.5 Tesla proton MR spectra of human brain using LCModel and an imported basis set. , 1999, Magnetic resonance imaging.

[4]  Jens Frahm,et al.  Regional Age Dependence of Human Brain Metabolites from Infancy to Adulthood as Detected by Quantitative Localized Proton MRS , 1999, Pediatric Research.

[5]  B J Soher,et al.  Quantitation of proton NMR spectra of the human brain using tissue water as an internal concentration reference , 1993, NMR in biomedicine.

[6]  B D Ross,et al.  Absolute Quantitation of Water and Metabolites in the Human Brain. I. Compartments and Water , 1993 .

[7]  L. Wald,et al.  Theory and application of array coils in MR spectroscopy , 1997, NMR in biomedicine.

[8]  J. Frahm,et al.  Absolute concentrations of metabolites in the adult human brain in vivo: quantification of localized proton MR spectra. , 1993, Radiology.

[9]  D J Collins,et al.  An algorithm for the optimum combination of data from arbitrary magnetic resonance phased array probes. , 2002, Physics in medicine and biology.

[10]  B. Ross,et al.  Three methods of calibration in quantitative proton MR spectroscopy. , 1995, Journal of magnetic resonance. Series B.

[11]  J. J. Van Der Klink The NMR reciprocity theorem for arbitrary probe geometry. , 2001 .

[12]  P. Barker,et al.  Single‐voxel proton MRS of the human brain at 1.5T and 3.0T , 2001, Magnetic resonance in medicine.

[13]  O Henriksen,et al.  Absolute quantitative proton NMR spectroscopy based on the amplitude of the local water suppression pulse. Quantification of brain water and metabolites , 1994, NMR in biomedicine.

[14]  B J Soher,et al.  Quantitation of automated single‐voxel proton MRS using cerebral water as an internal reference , 1996, Magnetic resonance in medicine.

[15]  S. Provencher Estimation of metabolite concentrations from localized in vivo proton NMR spectra , 1993, Magnetic resonance in medicine.

[16]  R. B. Kingsley,et al.  WET, a T1- and B1-insensitive water-suppression method for in vivo localized 1H NMR spectroscopy. , 1994, Journal of magnetic resonance. Series B.

[17]  J. Frahm,et al.  Regional metabolite concentrations in human brain as determined by quantitative localized proton MRS , 1998, Magnetic resonance in medicine.

[18]  L L Wald,et al.  Proton spectroscopic imaging of the human brain using phased array detectors , 1995, Magnetic resonance in medicine.

[19]  U. Klose In vivo proton spectroscopy in presence of eddy currents , 1990, Magnetic resonance in medicine.