Getting the phase consistent: The importance of phase description in balanced steady‐state free precession MRI of multi‐compartment systems
Purpose Determine the correct mathematical phase description for balanced steady‐state free precession (bSSFP) signals in multi‐compartment systems. Theory and Methods Based on published bSSFP signal models, different phase descriptions can be formulated: one predicting the presence and the other pr...
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Published in | Magnetic resonance in medicine Vol. 92; no. 1; pp. 215 - 225 |
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Main Authors | , , , , , , |
Format | Journal Article |
Language | English |
Published |
United States
Wiley Subscription Services, Inc
01.07.2024
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Subjects | |
Online Access | Get full text |
ISSN | 0740-3194 1522-2594 1522-2594 |
DOI | 10.1002/mrm.30033 |
Cover
Abstract | Purpose
Determine the correct mathematical phase description for balanced steady‐state free precession (bSSFP) signals in multi‐compartment systems.
Theory and Methods
Based on published bSSFP signal models, different phase descriptions can be formulated: one predicting the presence and the other predicting the absence of destructive interference effects in multi‐compartment systems. Numerical simulations of bSSFP signals of water and acetone were performed to evaluate the predictions of these different phase descriptions. For experimental validation, bSSFP profiles were measured at 3T using phase‐cycled bSSFP acquisitions performed in a phantom containing mixtures of water and acetone, which replicates a system with two signal components. Localized single voxel MRS was performed at 7T to determine the relative chemical shift of the acetone‐water mixtures.
Results
Based on the choice of phase description, the simulated bSSFP profiles of water‐acetone mixtures varied significantly, either displaying or lacking destructive interference effects, as predicted theoretically. In phantom experiments, destructive interference was consistently observed in the measured bSSFP profiles of water‐acetone mixtures, supporting the theoretical description that predicts such interference effects. The connection between the choice of phase description and predicted observation enables unambiguous experimental identification of the correct phase description for multi‐compartment bSSFP profiles, which is consistent with the Bloch equations.
Conclusion
The study emphasizes that consistent phase descriptions are crucial for accurately describing multi‐compartment bSSFP signals, as incorrect phase descriptions result in erroneous predictions. |
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AbstractList | Determine the correct mathematical phase description for balanced steady-state free precession (bSSFP) signals in multi-compartment systems.PURPOSEDetermine the correct mathematical phase description for balanced steady-state free precession (bSSFP) signals in multi-compartment systems.Based on published bSSFP signal models, different phase descriptions can be formulated: one predicting the presence and the other predicting the absence of destructive interference effects in multi-compartment systems. Numerical simulations of bSSFP signals of water and acetone were performed to evaluate the predictions of these different phase descriptions. For experimental validation, bSSFP profiles were measured at 3T using phase-cycled bSSFP acquisitions performed in a phantom containing mixtures of water and acetone, which replicates a system with two signal components. Localized single voxel MRS was performed at 7T to determine the relative chemical shift of the acetone-water mixtures.THEORY AND METHODSBased on published bSSFP signal models, different phase descriptions can be formulated: one predicting the presence and the other predicting the absence of destructive interference effects in multi-compartment systems. Numerical simulations of bSSFP signals of water and acetone were performed to evaluate the predictions of these different phase descriptions. For experimental validation, bSSFP profiles were measured at 3T using phase-cycled bSSFP acquisitions performed in a phantom containing mixtures of water and acetone, which replicates a system with two signal components. Localized single voxel MRS was performed at 7T to determine the relative chemical shift of the acetone-water mixtures.Based on the choice of phase description, the simulated bSSFP profiles of water-acetone mixtures varied significantly, either displaying or lacking destructive interference effects, as predicted theoretically. In phantom experiments, destructive interference was consistently observed in the measured bSSFP profiles of water-acetone mixtures, supporting the theoretical description that predicts such interference effects. The connection between the choice of phase description and predicted observation enables unambiguous experimental identification of the correct phase description for multi-compartment bSSFP profiles, which is consistent with the Bloch equations.RESULTSBased on the choice of phase description, the simulated bSSFP profiles of water-acetone mixtures varied significantly, either displaying or lacking destructive interference effects, as predicted theoretically. In phantom experiments, destructive interference was consistently observed in the measured bSSFP profiles of water-acetone mixtures, supporting the theoretical description that predicts such interference effects. The connection between the choice of phase description and predicted observation enables unambiguous experimental identification of the correct phase description for multi-compartment bSSFP profiles, which is consistent with the Bloch equations.The study emphasizes that consistent phase descriptions are crucial for accurately describing multi-compartment bSSFP signals, as incorrect phase descriptions result in erroneous predictions.CONCLUSIONThe study emphasizes that consistent phase descriptions are crucial for accurately describing multi-compartment bSSFP signals, as incorrect phase descriptions result in erroneous predictions. Purpose Determine the correct mathematical phase description for balanced steady‐state free precession (bSSFP) signals in multi‐compartment systems. Theory and Methods Based on published bSSFP signal models, different phase descriptions can be formulated: one predicting the presence and the other predicting the absence of destructive interference effects in multi‐compartment systems. Numerical simulations of bSSFP signals of water and acetone were performed to evaluate the predictions of these different phase descriptions. For experimental validation, bSSFP profiles were measured at 3T using phase‐cycled bSSFP acquisitions performed in a phantom containing mixtures of water and acetone, which replicates a system with two signal components. Localized single voxel MRS was performed at 7T to determine the relative chemical shift of the acetone‐water mixtures. Results Based on the choice of phase description, the simulated bSSFP profiles of water‐acetone mixtures varied significantly, either displaying or lacking destructive interference effects, as predicted theoretically. In phantom experiments, destructive interference was consistently observed in the measured bSSFP profiles of water‐acetone mixtures, supporting the theoretical description that predicts such interference effects. The connection between the choice of phase description and predicted observation enables unambiguous experimental identification of the correct phase description for multi‐compartment bSSFP profiles, which is consistent with the Bloch equations. Conclusion The study emphasizes that consistent phase descriptions are crucial for accurately describing multi‐compartment bSSFP signals, as incorrect phase descriptions result in erroneous predictions. Determine the correct mathematical phase description for balanced steady-state free precession (bSSFP) signals in multi-compartment systems. Based on published bSSFP signal models, different phase descriptions can be formulated: one predicting the presence and the other predicting the absence of destructive interference effects in multi-compartment systems. Numerical simulations of bSSFP signals of water and acetone were performed to evaluate the predictions of these different phase descriptions. For experimental validation, bSSFP profiles were measured at 3T using phase-cycled bSSFP acquisitions performed in a phantom containing mixtures of water and acetone, which replicates a system with two signal components. Localized single voxel MRS was performed at 7T to determine the relative chemical shift of the acetone-water mixtures. Based on the choice of phase description, the simulated bSSFP profiles of water-acetone mixtures varied significantly, either displaying or lacking destructive interference effects, as predicted theoretically. In phantom experiments, destructive interference was consistently observed in the measured bSSFP profiles of water-acetone mixtures, supporting the theoretical description that predicts such interference effects. The connection between the choice of phase description and predicted observation enables unambiguous experimental identification of the correct phase description for multi-compartment bSSFP profiles, which is consistent with the Bloch equations. The study emphasizes that consistent phase descriptions are crucial for accurately describing multi-compartment bSSFP signals, as incorrect phase descriptions result in erroneous predictions. PurposeDetermine the correct mathematical phase description for balanced steady‐state free precession (bSSFP) signals in multi‐compartment systems.Theory and MethodsBased on published bSSFP signal models, different phase descriptions can be formulated: one predicting the presence and the other predicting the absence of destructive interference effects in multi‐compartment systems. Numerical simulations of bSSFP signals of water and acetone were performed to evaluate the predictions of these different phase descriptions. For experimental validation, bSSFP profiles were measured at 3T using phase‐cycled bSSFP acquisitions performed in a phantom containing mixtures of water and acetone, which replicates a system with two signal components. Localized single voxel MRS was performed at 7T to determine the relative chemical shift of the acetone‐water mixtures.ResultsBased on the choice of phase description, the simulated bSSFP profiles of water‐acetone mixtures varied significantly, either displaying or lacking destructive interference effects, as predicted theoretically. In phantom experiments, destructive interference was consistently observed in the measured bSSFP profiles of water‐acetone mixtures, supporting the theoretical description that predicts such interference effects. The connection between the choice of phase description and predicted observation enables unambiguous experimental identification of the correct phase description for multi‐compartment bSSFP profiles, which is consistent with the Bloch equations.ConclusionThe study emphasizes that consistent phase descriptions are crucial for accurately describing multi‐compartment bSSFP signals, as incorrect phase descriptions result in erroneous predictions. |
Author | Peper, Eva S. Kreis, Roland Açikgöz, Berk C. Ganter, Carl Bastiaansen, Jessica A. M. Plähn, Nils M. J. Poli, Simone |
Author_xml | – sequence: 1 givenname: Nils M. J. orcidid: 0009-0002-2624-5412 surname: Plähn fullname: Plähn, Nils M. J. organization: University of Bern – sequence: 2 givenname: Simone surname: Poli fullname: Poli, Simone organization: University of Bern – sequence: 3 givenname: Eva S. surname: Peper fullname: Peper, Eva S. organization: Swiss Institute for Translational and Entrepreneurial Medicine – sequence: 4 givenname: Berk C. surname: Açikgöz fullname: Açikgöz, Berk C. organization: University of Bern – sequence: 5 givenname: Roland orcidid: 0000-0002-8618-6875 surname: Kreis fullname: Kreis, Roland organization: University of Bern – sequence: 6 givenname: Carl orcidid: 0000-0002-6735-7448 surname: Ganter fullname: Ganter, Carl organization: TUM School of Medicine and Health, Klinikum rechts der Isar, Technical University of Munich – sequence: 7 givenname: Jessica A. M. orcidid: 0000-0002-5485-1308 surname: Bastiaansen fullname: Bastiaansen, Jessica A. M. email: jbastiaansen.mri@gmail.com organization: Swiss Institute for Translational and Entrepreneurial Medicine |
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Determine the correct mathematical phase description for balanced steady‐state free precession (bSSFP) signals in multi‐compartment systems.
Theory and... Determine the correct mathematical phase description for balanced steady-state free precession (bSSFP) signals in multi-compartment systems. Based on published... PurposeDetermine the correct mathematical phase description for balanced steady‐state free precession (bSSFP) signals in multi‐compartment systems.Theory and... Determine the correct mathematical phase description for balanced steady-state free precession (bSSFP) signals in multi-compartment systems.PURPOSEDetermine... |
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SubjectTerms | Acetone asymmetries balanced steady‐state free precession Chemical equilibrium Descriptions Interference Mathematical models Mixtures multi‐compartment phase definition phase‐cycled bSSFP Precession signal model |
Title | Getting the phase consistent: The importance of phase description in balanced steady‐state free precession MRI of multi‐compartment systems |
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