METHOD OF DOUBLE-CONTRAST MAGNETIC RESONANCE FINGERPRINTING
20250237726 ยท 2025-07-24
Inventors
Cpc classification
G01R33/5601
PHYSICS
International classification
G01R33/58
PHYSICS
G01R33/561
PHYSICS
Abstract
A method of double-contrast magnetic resonance fingerprinting including: optimizing, using Cramr-Rao lower bound (CRLB) via a computer system, radiofrequency (RF) pulse parameters in an MRF sequence; loading, via the computer system, the RF pulse parameters optimized into an MRI scanner; and capturing raw k-space data by selecting different signal contrast modules for dual-contrast encoding at varying repetition times (TR); reconstructing, via the computer system, at least one image including a plurality of pixels; defining, via the computer system, a dynamic range and step size for tissue parameters; and creating, via the computer system, a dictionary based on Bloch equations, the dynamic range, and the step size; and comparing, via the computer system, signal evolution for each of the plurality of pixels in the at least one image to the dictionary to determine quantitative parameters for each of the plurality of pixels, and generating a quantitative parameter map.
Claims
1. A method of double-contrast magnetic resonance fingerprinting, comprising: S1. optimizing, using Cramr-Rao lower bound (CRLB) via a computer system, radiofrequency (RF) pulse parameters in an MRF sequence; wherein, the MRF sequence comprises a Fast Imaging with Steady-State Precession (FISP) contrast module and a Reversed Fast Imaging with Steady-State Precession (PSIF) contrast module; S2. loading, via the computer system, the RF pulse parameters optimized into an MRI scanner; and capturing, using the MRI scanner, raw k-space data by selecting different signal contrast modules for dual-contrast encoding at varying repetition times (TR); S3. reconstructing, via the computer system, at least one image comprising a plurality of pixels, by processing the raw k-space data using a reconstruction algorithm; S4. defining, via the computer system, a dynamic range and step size for tissue parameters; and creating, via the computer system, a dictionary based on Bloch equations, the dynamic range, and the step size; and S5. comparing, via the computer system, signal evolution for each of the plurality of pixels in the at least one image to the dictionary to determine quantitative parameters for each of the plurality of pixels, and generating a quantitative parameter map.
2. The method of claim 1, wherein in S1, the RF pulse parameters comprise flip angle (FA), repetition time (TR), selection (SE), and flip angle multiplier (AM).
3. The method of claim 1, wherein in S1, the FISP contrast module is configured to capture FISP signals, and the PSIF contrast module is configured to capture PSIF signals; the flip angle for the FISP contrast module is defined as FA, and the flip angle for the PSIF contrast module is defined as AM.Math.FA; the SE parameter is introduced to determine, for each repetition time (TR), whether to select the FISP contrast module or the PSIF contrast module for capturing the MRF signal.
4. The method of claim 3, wherein optimizing RF pulse parameters comprises: setting longitudinal relaxation time (T.sub.1) and transverse relaxation time (T.sub.2) of the tissue parameters and the RF pulse parameters FA, TR, SE, and AM; inputting the tissue parameters and the RF pulse parameters into the Bloch equations to simulate the MRF signal; calculating, using the simulated MRF signal, a Fisher Information matrix; processing, using generalized inverse, the Fisher Information Matrix to compute a Cramr-Rao matrix; and creating a weighing matrix based on the tissue parameters T.sub.1 and T.sub.2; multiplying the weighing matrix with the Cramer-Rao matrix to produce a new matrix; and calculating a trace of the new matrix to derive an optimization objective function:
5. The method of claim 1, wherein in S3, when the raw k-space data is collected from receiver coils, a parallel imaging method or a compressed sensing method is adopted to optimize the reconstruction of the at least one image.
6. The method of claim 1, wherein in S4, creating a dictionary based on Bloch equations comprises: defining the dynamic range and step size for the tissue parameters T.sub.1 and T.sub.2; modeling, using the Bloch equations, the MRF signal for each unique combination of T.sub.1 and T.sub.2; and generating the dictionary; wherein, the dictionary comprises a plurality of entries; each of the plurality of entries corresponds to a unique combination of T.sub.1 and T.sub.2; the signal evolution for each of the plurality of entries is defined as a time-series response of the MRF signal modeled using the Bloch equations for the assigned tissue parameters T.sub.1 and T.sub.2; and the signal evolution is defined as follows:
7. The method of claim 1, wherein in S5, comparing signal evolution for each of the plurality of pixels in the at least one image to the dictionary comprises: inverting PSIF signals; for each of the plurality of pixels, computing an inner product between the signal evolution of the pixel and the signal evolution for each of the plurality of entries in the dictionary; summing all of absolute values of the computed inner products for each of the plurality of pixels; and selecting, for each of the plurality of pixels, an entry with the highest sum of absolute inner products as the best matching entry; and assigning the tissue parameters corresponding to a best entry as physical parameters of each of the plurality of pixels.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION
[0038] To further illustrate the disclosure, embodiments detailing the method of double-contrast magnetic resonance fingerprinting are described below. It should be noted that the following embodiments are intended to describe and not to limit the disclosure.
[0039] As shown in
1. Sequence Optimization
[0040] As shown in
[0041] A. The FISP contrast module emits the RF pulse to excite the hydrogen nuclei in the tissues. The nuclei relax and release energy. The energy is captured by the FISP contrast module as an FID signal.
[0042] B. In the PSIF contrast module, a rewinder gradient is applied at the end. A readout gradient in the PSIF contrast module is the time-reversed form of a readout gradient in the FISP contrast module. The signal from the previous contrast module is reemitted and refocused by the RF pulse in the current PSIF contrast module, resulting in an echo signal.
[0043] C. Different flip angles are used in the two contrast modules to obtain different echo signals. When alternatively using the two contrast modules, the echo signals are divided into two branches, one from each contrast module. The alternation usage of the two contrast modules is determined by introducing the SE parameter. The SE parameter is initialized using a trigonometric function to facilitate Cramr-Rao lower bound (CRLB) optimization. The trigonometric function can be expressed as follows:
[0044] The known values of the tissue parameters (T.sub.1 and T.sub.2) and the RF pulse parameters (FA, TR, SE, and AM) are input into the Bloch equations. The Bloch equations generate a simulated MRF signal that represents the expected MRF response of the tissue. The simulated MRF signal is configured to compute the Fisher Information matrix. The Fisher Information Matrix is configured to calculate the CRLB matrix. The CRLB matrix is configured to calculate an optimization objective function.
[0045] The Cramer-Rao Lower Bound (CRLB) is a theoretical limit that defines the minimum variance achievable by unbiased estimator when estimating a parameter. The CRLB matrix provide information that the variance of any unbiased estimator must be greater than or equal to the CRLB value. The variance of any unbiased estimator can be expressed as follows:
[0047] In the CRLB optimization, upper bounds and lower bounds for the RF pulse parameters are defined as follows: FA.sub.n.sup.max, FA.sub.n.sup.min=10, TR.sub.n.sup.maxms, TR.sub.n.sup.min=16 ms, SE.sub.n.sup.max, SE.sub.n.sup.min=0, AM.sub.n.sup.max, AM.sub.n.sup.min=0. FA is the flip angle used in the FISP module; TR is the repetition time; SE is a parameter that determines the switching between the FISP and PSIF modules during the MRF sequence; and AM is the multiple of the flip angle used in the PSIF module compared to the FISP module.
[0048] Additionally, to ensure the smoothness of the signal evolution, a smoothing constraint is added to the CRLB optimization process: F A.sup.max=1. The smoothing constraint helps avoid irregular or erratic behavior in the signal evolution, particularly when the data is undersampled.
[0049] The optimization objective function is defined as follows:
[0051]
2. Data Acquisition and Processing
[0052] A. The optimization results from
[0053] C. The basic principle of magnetic resonance fingerprinting (MRF) is to build a dictionary of fingerprints that represent all possible MRF signals, which are generated based on various tissue properties and parameters. The MRF signals in the dictionary are then compared with the actual MRF signals collected during an MRI scan. By identifying the fingerprint in the dictionary that most closely matches the collected MRF signal, the corresponding tissue physiological parameters, such as relaxation times (T.sub.1 and T.sub.2), can be determined. The process enables the creation of quantitative images, providing detailed information about tissue characteristics. The term fingerprint, as used herein, refers to the time evolution curve of the MRF signal. The dictionary is created as follows: (1) A range of variation for each parameter is defined, for example: T.sub.1: [100:20:200 ms], [2100:100:3000 ms], [3200:500:5000 ms]; T.sub.2: [10:5:150 ms], [160:10:200 ms], [220:20:300 ms], [400:100:2000 ms]; (2) Using the Bloch equations, all possible time evolution curves are computed based on the dynamic ranges of the tissue parameters. The time evolution curves forms the dictionary.
[0054] D. The k-space data is reconstructed into a plurality of images using the FLOR reconstruction algorithm. The reconstructed MRF signal is then compared with the entries in the dictionary by calculating the inner product. The inner product that yields the highest value indicates the entry in the dictionary that most closely matches the reconstructed MRF signal. The corresponding tissue parameters (T.sub.1, T.sub.2) for the entry are then assigned to the pixel, resulting in a quantitative parameter map for the entire image.
[0055] The experiment is split into two parts: simulation experiment and actual scanning experiment.
(1) Simulation Experiments
[0056] As shown in the top part of
[0057] To compare the disclosed method, three other techniques were also tested, including conventional FISP sequences, CRLB-optimized FISP sequences, and a combination of FISP sequences and PSIF sequences. A mask was applied to isolate the region of interest in the brain. The deviation between the ground truth values and the results from the simulation was calculated as follows: bias=I.sub.2/I.sub.2, where I and represent the quantitative true values and the simulated quantitative results, respectively.
[0058] The experimental results and error maps are shown in
[0059] In
(2) Actual Scanning Experiments
[0060] In vivo experiments were conducted using a Siemens Prisma 3.0T MRI scanner with a 20-channel head coil, with w. Written consent was obtained from healthy volunteers before the experiments.
TABLE-US-00001 TABLE 1 Normalized standard deviation of the results FISP CRLB-FISP FISP&PSIF Proposed T.sub.1 Nstd 1.32 1.28 1.35 1.36 T.sub.2 Nstd 2.80 2.43 2.79 1.96
[0061] The tissue parameters and the RF pulse parameters are defined as follows:
[0062] T.sub.1 (Longitudinal Relaxation Time): A parameter representing the time required for the longitudinal magnetization vector to recover to 67% of its total signal intensity after being disturbed by an RF pulse.
[0063] T.sub.2 (Transverse Relaxation Time): A parameter representing the time required for the transverse magnetization vector to decay from 100% to 37% of its initial signal intensity due to interactions between nuclear spins, after the application of an RF pulse.
[0064] FA (Flip Angle): A parameter representing the angle by which the magnetization vector is deflected from its alignment with the main magnetic field by the excitation RF pulse. Specifically, when FA=90, the magnetization vector is perpendicular to the main magnetic field direction.
[0065] TE (Echo Time): A parameter representing the time interval between the center of the RF excitation signal and the center of the received echo signal in the MRF sequence.
[0066] TR (Repetition Time): A parameter representing the time interval between two consecutive RF excitations in the MRF sequence, which controls the longitudinal relaxation process between excitations.
[0067] SE (Selection): A parameter that selects between the two signal contrast modules used in the MRF sequence. When SE=1, the FISP contrast module is selected, and when SE=0, the PSIF contrast module is selected.
[0068] AM (Flip Angle Multiplier): A parameter representing the multiplier factor by which the flip angle used in the PSIF contrast module is adjusted relative to the flip angle used in the FISP contrast module.
[0069] It will be obvious to those skilled in the art that changes and modifications may be made, and therefore, the aim in the appended claims is to cover all such changes and modifications.