A theoretical and numerical consideration of the longitudinal and transverse relaxations in the rotating frame

• Published in: Magnetic resonance imaging Vol. 31; no. 9; pp. 1544 - 1558
• Main Author: Murase, Kenya
• Format: Journal Article
• Language: English
• Published: Netherlands Elsevier Inc 01.11.2013
• Subjects: Algorithms; Bloch equations; Chemical exchange saturation transfer; Diffusion; Evolution; Image Processing, Computer-Assisted; Longitudinal relaxation; Magnetic Resonance Imaging; Magnetics; Models, Theoretical; Protons; Radio Waves; Radiology; Reproducibility of Results; Rotating frame; Spin lock; Stochastic Processes; Transverse relaxation; Water - chemistry; Chemical exchange saturation transfer; Bloch equations; Transverse relaxation; Spin lock; Longitudinal relaxation; Rotating frame
• ISSN: 0730-725X; 1873-5894
• DOI: 10.1016/j.mri.2013.07.004

Abstract We previously derived a simple equation for solving time-dependent Bloch equations by a matrix operation. The purpose of this study was to present a theoretical and numerical consideration of the longitudinal ( R1ρ = 1/ T1ρ ) and transverse relaxation rates in the rotating frame ( R2ρ = 1/ T2ρ ), based on this method. First, we derived an equation describing the time evolution of the magnetization vector ( M (t)) by expanding the matrix exponential into the eigenvalues and the corresponding eigenvectors using diagonalization. Second, we obtained the longitudinal magnetization vector in the rotating frame ( M1ρ (t)) by taking the inner product of M (t) and the eigenvector with the smallest eigenvalue in modulus, and then we obtained the transverse magnetization vector in the rotating frame ( M2ρ (t)) by subtracting M1ρ (t) from M (t). For comparison, we also computed the spin-locked magnetization vector. We derived the exact solutions for R1ρ and R2ρ from the eigenvalues, and compared them with those obtained numerically from M1ρ (t) and M2ρ (t), respectively. There was excellent agreement between them. From the exact solutions for R1ρ and R2ρ , R2ρ was found to be given by R 2 ρ = (2 R2 + R1 )/2 − R 1 ρ /2, where R1 and R2 denote the conventional longitudinal and transverse relaxation rates, respectively. We also derived M1ρ (t) and M2ρ (t) for bulk water protons, in which the effect of chemical exchange was taken into account using a 2-pool chemical exchange model, and we compared the R1ρ and R2ρ values obtained from the eigenvalues and those obtained numerically from M1ρ (t) and M2ρ (t). There was also excellent agreement between them. In conclusion, this study will be useful for better understanding of the longitudinal and transverse relaxations in the rotating frame and for analyzing the contrast mechanisms in T1ρ - and T2ρ -weighted MRI.