2004
DOI: 10.1002/mrm.20244
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Time‐domain combination of MR spectroscopy data acquired using phased‐array coils

Abstract: A new method for efficiently processing MRS data acquired with phased-array coils is presented. The method consists of performing phase compensation (i.e., redefining the signal phase relative to a common reference) of the signals in the time domain prior to combining the signals. The resulting spectra are equivalent to those obtained by previously published methods for phased-array spectral data processing (i.e., processing the signals individually and then combining them in the frequency domain). The method … Show more

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Cited by 88 publications
(142 citation statements)
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“…Briefly, the 8-channel phased-array coil data recorded were combined into single regular time-domain free-induction decay signals, using a C-language computer program that implemented a previously published algorithm (Brown, 2004), with the unsuppressed voxel tissue water signal from each receiver coil element providing the required relative array coil sensitivities. The two resulting free-induction decay signals for the editing pulses on/off scans were subtracted in the time domain to yield the difference signal, which was filtered with an exponential multiplication function corresponding to a 5-Hz linebroadening and then Fourier-transformed to obtain the GABA and Glx spectra (Figure 1b).…”
Section: H Mrs Data Processing and Quantificationmentioning
confidence: 99%
“…Briefly, the 8-channel phased-array coil data recorded were combined into single regular time-domain free-induction decay signals, using a C-language computer program that implemented a previously published algorithm (Brown, 2004), with the unsuppressed voxel tissue water signal from each receiver coil element providing the required relative array coil sensitivities. The two resulting free-induction decay signals for the editing pulses on/off scans were subtracted in the time domain to yield the difference signal, which was filtered with an exponential multiplication function corresponding to a 5-Hz linebroadening and then Fourier-transformed to obtain the GABA and Glx spectra (Figure 1b).…”
Section: H Mrs Data Processing and Quantificationmentioning
confidence: 99%
“…24 A comparison of the performance of many of these CSI methods has been provided by Pohmann et al 43 Barker and Lin 26 have an excellent discussion of methods that use multireceiver arrays (e.g., an eightchannel head array) to accelerate CSI acquisitions, similar to the methods used in parallel imaging. An added complication is that, although there have been descriptions of algorithms 44,45 used in combining CSI spectra obtained from each individual coil element, few of these are routinely available on commercial whole-body clinical scanners. This situation is in contrast to multicoil MR imaging and parallel imaging, in which this combination (or acceleration, or both) is performed routinely.…”
Section: Spatial Localizationmentioning
confidence: 99%
“…Better results are obtained by weighting the spectra according to the reference peak amplitudes (3) or SNRs (7), which approximate a matched filter. When performing 1 H spectroscopy in vivo, particularly reliable reference peak data are obtained by repeating the experiment without water suppression since tissue contains water at $40 M concentration (8)(9)(10)(11). Alternatively, one can use the whole chemical shift range of the spectra.…”
Section: Existing Approaches To Receive Array Mr Spectroscopymentioning
confidence: 99%
“…Alternatively, one can use the whole chemical shift range of the spectra. Brown (8) suggested scaling and phasing each spectrum by the first point in its FID, i.e., by the mean value of the spectrum. The singular value decomposition (SVD) also uses the whole spectra for combination (9).…”
Section: Existing Approaches To Receive Array Mr Spectroscopymentioning
confidence: 99%
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