The effect of high performance gradients on fast gradient echo imaging

The effect of gradient system performance on segmented k‐space gradient echo imaging is presented. Three cases were investigated. First, an ideal system that has infinite slew rates and unlimited maximum gradient strengths was considered. Second, a “high speed” imaging system (2.3 (G/cm), 23 (G/cm)/ms) was considered. These two cases were compared with a “conventional” imaging system (1(G/cm), 1.67 (G/cm)/ms). It was found that substantial increases in SNR can be achieved (≈︁ 45%) by using high speed versus a conventional gradient system, for a TR of 6 ms. For trapezoidal gradient waveforms, there exists an optimum maximum gradient strength for a given slew rate, and any increase in gradient strength above this optimum will not be utilized by an optimized sequence. These studies have shown that increasing TR without decreasing the bandwidth is not a good way to increase SNR for constant scan time.

[1]  D. Parker,et al.  Signal-to-noise efficiency in magnetic resonance imaging. , 1990, Medical physics.

[2]  R M Henkelman,et al.  Elimination of transverse coherences in FLASH MRI , 1988, Magnetic resonance in medicine.

[3]  V. Wedeen Magnetic resonance imaging of myocardial kinematics. technique to detect, localize, and quantify the strain rates of the active human myocardium , 1992, Magnetic resonance in medicine.

[4]  M. Gyngell,et al.  The steady-state signals in short-repetition-time sequences , 1989 .

[5]  G H Glover,et al.  Projection Reconstruction Techniques for Reduction of Motion Effects in MRI , 1992, Magnetic resonance in medicine.

[6]  W. Edelstein,et al.  The intrinsic signal‐to‐noise ratio in NMR imaging , 1986, Magnetic resonance in medicine.

[7]  M. Moseley,et al.  Echo-planar MR imaging of normal and ischemic myocardium with gadodiamide injection. , 1993, Radiology.

[8]  R. R. Ernst,et al.  Application of Fourier Transform Spectroscopy to Magnetic Resonance , 1966 .

[9]  W. Hinshaw,et al.  Image formation by nuclear magnetic resonance: The sensitive‐point method , 1976 .

[10]  R. Henkelman Measurement of signal intensities in the presence of noise in MR images. , 1985, Medical physics.

[11]  M. L. Wood,et al.  Spoiling of transverse magnetization in steady‐state sequences , 1991, Magnetic resonance in medicine.

[12]  R. Edelman,et al.  Cineangiography of the heart in a single breath hold with a segmented turboFLASH sequence. , 1991, Radiology.

[13]  Bob S. Hu,et al.  Fast Spiral Coronary Artery Imaging , 1992, Magnetic resonance in medicine.

[14]  S. Riederer,et al.  Analysis of T2 limitations and off‐resonance effects on spatial resolution and artifacts in echo‐planar imaging , 1990, Magnetic resonance in medicine.

[15]  S. Riederer,et al.  A spoiling sequence for suppression of residual transverse magnetization , 1990, Magnetic resonance in medicine.

[16]  E. McVeigh,et al.  Cardiac Tagging with Breath‐Hold Cine MRI , 1992, Magnetic resonance in medicine.