Related Experiment Video
Updated: Jun 13, 2025

09:30
Quantitative Magnetic Resonance Imaging of Skeletal Muscle Disease
Published on: December 18, 2016
19.5K
Towards accurate MRF T2 in structured material at 0.55T using MT-suppressed excitations
Zhibo Zhu1, Nam G Lee2, Krishna S Nayak3
1Ming Hsieh Department of Electrical and Computer Engineering, University of Southern California, Los Angeles, CA, United States.
Magnetic Resonance Imaging
|June 11, 2025
Summary
This study introduces a new 0.55 Tesla Fast Imaging with Steady-state Free Precession-Magnetic Resonance Fingerprinting (FISP-MRF) method. It significantly improves T2 mapping accuracy in white matter by reducing artifacts.
Area of Science:
- Biomedical Engineering
- Magnetic Resonance Imaging
- Neuroimaging
Background:
- Accurate T2 mapping is crucial for characterizing biological tissues.
- Structured materials like white matter present challenges for conventional MR imaging due to complex magnetic properties.
- Existing Magnetic Resonance Fingerprinting (MRF) methods can suffer from artifacts, particularly at lower field strengths.
Purpose of the Study:
- To develop a novel 0.55 Tesla Fast Imaging with Steady-state Free Precession-Magnetic Resonance Fingerprinting (FISP-MRF) technique.
- To enhance the accuracy of T2 quantification in structured biological tissues, such as white matter.
- To mitigate artifacts caused by off-resonance Magnetization Transfer (MT) effects.
Main Methods:
- Implementation of non-selective, low-bandwidth excitation pulses to minimize on-resonance MT effects.
- Simulation of MRF dictionaries using a conventional single-pool model.
- Comparison of T2 maps generated by the novel non-selective approach against conventional slab-selective MRF and slow, reference-based measurements.
Main Results:
- The proposed non-selective approach significantly reduced T2 underestimation in white matter from approximately 40% to below 10%.
- The precision of T2 measurements was maintained without compromise.
- The method demonstrated improved accuracy at 0.55 Tesla.
Conclusions:
- Non-selective, low-bandwidth excitations effectively reduce MT effects in 0.55T FISP-MRF.
- This advancement enables the use of a simplified single-pool model for T2 quantification.
- The developed technique is particularly valuable for MRF applications at low field strengths and in challenging materials like white matter.
Related Concept Videos
NMR Spectrometers: Resolution and Error Correction
678
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
678
Magnetic Resonance Imaging
5.0K
Magnetic resonance imaging (MRI) is a noninvasive medical imaging technique based on a phenomenon of nuclear physics discovered in the 1930s, in which matter exposed to magnetic fields and radio waves was found to emit radio signals. In 1970, a physician and researcher named Raymond Damadian noticed that malignant (cancerous) tissue gave off different signals than normal body tissue. He applied for a patent for the first MRI scanning device in clinical use by the early 1980s. The early MRI...
5.0K
Two-Dimensional (2D) NMR: Overview
632
The 1D NMR spectrum of large and complex molecules like natural products has complicated splitting patterns and overlapping signals, which can be easily interpreted using 2-dimensional (2D) NMR. Unlike 1D NMR, 2D NMR has two frequency axes that provide the coupling information between the nucleus A and nucleus B in a molecule. The process from which 2D spectra are obtained has four steps.
The first step is the preparation period, during which nucleus A is excited with a radiofrequency pulse....
The first step is the preparation period, during which nucleus A is excited with a radiofrequency pulse....
632

