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Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing

In EPI‐fMRI acquisitions, various readout bandwidth (BW) values are used as a function of gradients' characteristics of the MR scanner system. Echo spacing (ES) is another fundamental parameter of EPI‐fMRI sequences, but the employed ES value is not usually reported in fMRI studies. Nyquist gho...

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Autores principales: Giannelli, Marco, Diciotti, Stefano, Tessa, Carlo, Mascalchi, Mario
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2010
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5720418/
https://www.ncbi.nlm.nih.gov/pubmed/21081879
http://dx.doi.org/10.1120/jacmp.v11i4.3237
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author Giannelli, Marco
Diciotti, Stefano
Tessa, Carlo
Mascalchi, Mario
author_facet Giannelli, Marco
Diciotti, Stefano
Tessa, Carlo
Mascalchi, Mario
author_sort Giannelli, Marco
collection PubMed
description In EPI‐fMRI acquisitions, various readout bandwidth (BW) values are used as a function of gradients' characteristics of the MR scanner system. Echo spacing (ES) is another fundamental parameter of EPI‐fMRI sequences, but the employed ES value is not usually reported in fMRI studies. Nyquist ghost is a typical EPI artifact that can degrade the overall quality of fMRI time series. In this work, the authors assessed the basic effect of BW and ES for two clinical 1.5 T MR scanner systems (scanner‐A, scanner‐B) on Nyquist ghost of gradient‐echo EPI‐fMRI sequences. BW range was: scanner‐A, 1953‐3906 Hz/pixel; scanner‐B, 1220‐2894 Hz/pixel. ES range was: scanner‐A, scanner‐B: 0.75‐1.33 ms. The ghost‐to‐signal ratio of time series acquisition [Formula: see text] and drift of ghost‐to‐signal ratio [Formula: see text] were measured in a water phantom. For both scanner‐A (93% of variation) and scanner‐B (102% of variation) the mean [Formula: see text] significantly increased with increasing BW. [Formula: see text] values of scanner‐A did not significantly depended on ES. On the other hand, [Formula: see text] values of scanner‐B significantly varied with ES, showing a downward trend (81% of variation) with increasing ES. In addition, a [Formula: see text] spike point at [Formula: see text] indicating a potential resonant effect was revealed. For both scanners, no significant effect of ES on [Formula: see text] was revealed. [Formula: see text] values of scanner‐B did not significantly vary with BW, whereas [Formula: see text] values of scanner‐A significantly depended on BW showing an upward trend from negative to positive values with increasing BW. [Formula: see text] and [Formula: see text] can significantly vary with BW and ES, and the specific pattern of variation may depend on gradients performances, EPI sequence calibrations and functional design of radiofrequency coil. Thus, each MR scanner system should be separately characterized. In general, the employment of low BW values seems to reduce the intensity and temporal variation of Nyquist ghost in EPI‐fMRI time series. On the other hand, the use of minimum ES value might not be entirely advantageous when the MR scanner is characterized by gradients with low performances and suboptimal EPI sequence calibration. PACS numbers: 87.61.‐c, 87.61.Qr, 87.61.Hk
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spelling pubmed-57204182018-04-02 Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing Giannelli, Marco Diciotti, Stefano Tessa, Carlo Mascalchi, Mario J Appl Clin Med Phys Medical Imaging In EPI‐fMRI acquisitions, various readout bandwidth (BW) values are used as a function of gradients' characteristics of the MR scanner system. Echo spacing (ES) is another fundamental parameter of EPI‐fMRI sequences, but the employed ES value is not usually reported in fMRI studies. Nyquist ghost is a typical EPI artifact that can degrade the overall quality of fMRI time series. In this work, the authors assessed the basic effect of BW and ES for two clinical 1.5 T MR scanner systems (scanner‐A, scanner‐B) on Nyquist ghost of gradient‐echo EPI‐fMRI sequences. BW range was: scanner‐A, 1953‐3906 Hz/pixel; scanner‐B, 1220‐2894 Hz/pixel. ES range was: scanner‐A, scanner‐B: 0.75‐1.33 ms. The ghost‐to‐signal ratio of time series acquisition [Formula: see text] and drift of ghost‐to‐signal ratio [Formula: see text] were measured in a water phantom. For both scanner‐A (93% of variation) and scanner‐B (102% of variation) the mean [Formula: see text] significantly increased with increasing BW. [Formula: see text] values of scanner‐A did not significantly depended on ES. On the other hand, [Formula: see text] values of scanner‐B significantly varied with ES, showing a downward trend (81% of variation) with increasing ES. In addition, a [Formula: see text] spike point at [Formula: see text] indicating a potential resonant effect was revealed. For both scanners, no significant effect of ES on [Formula: see text] was revealed. [Formula: see text] values of scanner‐B did not significantly vary with BW, whereas [Formula: see text] values of scanner‐A significantly depended on BW showing an upward trend from negative to positive values with increasing BW. [Formula: see text] and [Formula: see text] can significantly vary with BW and ES, and the specific pattern of variation may depend on gradients performances, EPI sequence calibrations and functional design of radiofrequency coil. Thus, each MR scanner system should be separately characterized. In general, the employment of low BW values seems to reduce the intensity and temporal variation of Nyquist ghost in EPI‐fMRI time series. On the other hand, the use of minimum ES value might not be entirely advantageous when the MR scanner is characterized by gradients with low performances and suboptimal EPI sequence calibration. PACS numbers: 87.61.‐c, 87.61.Qr, 87.61.Hk John Wiley and Sons Inc. 2010-07-12 /pmc/articles/PMC5720418/ /pubmed/21081879 http://dx.doi.org/10.1120/jacmp.v11i4.3237 Text en © 2010 The Authors. This is an open access article under the terms of the Creative Commons Attribution (http://creativecommons.org/licenses/by/3.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Medical Imaging
Giannelli, Marco
Diciotti, Stefano
Tessa, Carlo
Mascalchi, Mario
Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing
title Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing
title_full Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing
title_fullStr Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing
title_full_unstemmed Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing
title_short Characterization of Nyquist ghost in EPI‐fMRI acquisition sequences implemented on two clinical 1.5 T MR scanner systems: effect of readout bandwidth and echo spacing
title_sort characterization of nyquist ghost in epi‐fmri acquisition sequences implemented on two clinical 1.5 t mr scanner systems: effect of readout bandwidth and echo spacing
topic Medical Imaging
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5720418/
https://www.ncbi.nlm.nih.gov/pubmed/21081879
http://dx.doi.org/10.1120/jacmp.v11i4.3237
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