Explicit phenomenological solutions for magnetization exposed to an arbitrary NMR diffusion steady state pulse sequence

2021 ◽  
Vol 155 (14) ◽  
pp. 144204
Author(s):  
Anthony M. Lee ◽  
Timothy Stait-Gardner ◽  
William S. Price
2020 ◽  
Vol 6 (44) ◽  
pp. eabd1635
Author(s):  
R. Edelman ◽  
N. Leloudas ◽  
J. Pang ◽  
J. Bailes ◽  
R. Merrell ◽  
...  

A technique that provides more accurate cancer detection would be of great value. Toward this end, we developed T1 relaxation-enhanced steady-state (T1RESS), a novel magnetic resonance imaging (MRI) pulse sequence that enables the flexible modulation of T1 weighting and provides the unique feature that intravascular signals can be toggled on and off in contrast-enhanced scans. T1RESS makes it possible to effectively use an MRI technique with improved signal-to-noise ratio efficiency for cancer imaging. In a proof-of-concept study, “dark blood” unbalanced T1RESS provided a twofold improvement in tumor-to-brain contrast compared with standard techniques, whereas balanced T1RESS greatly enhanced vascular detail. In conclusion, T1RESS represents a new MRI technique with substantial potential value for cancer imaging, along with a broad range of other clinical applications.


2015 ◽  
Vol 5 (1) ◽  
Author(s):  
Xin Lu ◽  
Shi-You Chen ◽  
Jing-Long Ma ◽  
Lei Hou ◽  
Guo-Qian Liao ◽  
...  

1983 ◽  
Vol 51 (1) ◽  
pp. 153-156 ◽  
Author(s):  
Jürgen Lauterwein ◽  
Ioannis P Gerothanassis
Keyword(s):  

1988 ◽  
Vol 142 ◽  
Author(s):  
K. Linga Murty ◽  
O. Kanert

AbstractNuclear magnetic resonance pulse techniques are used in-situ during creep of single crystals of NaCl to evaluate the contribution of mobile dislocations to spin relaxation. 23Na spin-lattice relaxation rates were measured in the rotating frame (T1ρ) during compression creep of single crystals of NaCl along [110] direction at 473K at an applied stress of 20 MPa. The relaxation rates are evaluated from the spin-echo height following π/2, locking and 67° pulse sequence. The height of the free induction decay decreased as soon as the load is applied followed by a gradual increase until the steady-state is reached, at which point a saturation value is observed corresponding to the constant steady-state creep-rate. The mean jump distance of the mobile dislocations, evaluated from the ratio of the signal heights without deformation and during creep, decreased with time/strain reaching a constant value during steady-state creep regime. The results are compared with the dislocation-dislocation spacing, subgrain size as well as the jump distance predicted from creep models. The effects of dilvalent Ca and solid solution with LiCl are examined.


2002 ◽  
Vol 57 (6-7) ◽  
pp. 297-303 ◽  
Author(s):  
G. V. Mozjoukhine

The frequency offset effects of the signal interference during steady-state pulse sequences for remote nuclear quadrupole resonance (NQR) of 14N nuclei were investigated for the purposes of optimization in remote NQR. The experimental investigations with the separation of interfering NQR signals in sequences for observing signals {α0° |β90° −τ−α180° |β90° −τ} and {α0° |β90° −τ−α0° |β270° −τ} were carried out. The applications of the spherical tensor method for pure NQR of spin I = 1 for the investigation of these sequences and one pulse sequence, two pulse sequences are presented, too.


2008 ◽  
Vol 462 (4-6) ◽  
pp. 331-336 ◽  
Author(s):  
Tim Stait-Gardner ◽  
P.G. Anil Kumar ◽  
William S. Price
Keyword(s):  

1992 ◽  
Vol 47 (1-2) ◽  
pp. 415-420 ◽  
Author(s):  
S. S. Kim ◽  
J. R. P. Jayakody ◽  
R. A. Marino

AbstractThe behavior of induction signals during steady-state pulse irradiations in 14N NQR was investigated experimentally. It has long been known that the signal response to a long sequence of η pulses will dramatically increase for pulse spacings less than T2. This increase is exponential, and can result in signals comparable to optimally prepared Free Induction Decays. Because these "SORC" signals recur as long as the pulsing continues, very efficient signal-averaging can result. The dependence of these quasi steady-state signals on pulse parameters and on frequency offset are presented, together with a discussion of the applicability of the method.


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