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SPRITE single-point ramped imaging

SPRITE Single-point ramped imaging with Tx enhancement... [Pg.604]

SPREAD saturation pulses with reduced amplitude distribution SPRITE single-point ramped imaging with Ti enhancement SQUID superconducting quantum-interference device... [Pg.562]

Balcom, B.J., MacGregor, R.P., Beyea, S.D., Green, D.P., Armstrong, R.L., and Bremmer, T.W. 1996. Single point ramped imaging with T1 enhancement (SPRITE). J. Magn. Reson. A123, 131-134. [Pg.90]

Fig. 3.4.2 Schematic description of the three-dimensional SPRITE imaging technique. Gz, Gx and Gy are the phase encode magnetic field gradients and are amplitude cycled. A single data point is acquired at a fixed encoding time tp after the rf excitation pulse from the free induction decay (FID). TR is the time between rf pulses. Notice that Gx is ramped (+GZ max to -GXt max) and one /c-space point is acquired for each value of the magnetic field gradient. Gy and Gz are on during the Gx magnetic field gradient ramp and turned off at the end. Fig. 3.4.2 Schematic description of the three-dimensional SPRITE imaging technique. Gz, Gx and Gy are the phase encode magnetic field gradients and are amplitude cycled. A single data point is acquired at a fixed encoding time tp after the rf excitation pulse from the free induction decay (FID). TR is the time between rf pulses. Notice that Gx is ramped (+GZ max to -GXt max) and one /c-space point is acquired for each value of the magnetic field gradient. Gy and Gz are on during the Gx magnetic field gradient ramp and turned off at the end.

See other pages where SPRITE single-point ramped imaging is mentioned: [Pg.1]    [Pg.267]    [Pg.104]    [Pg.1]    [Pg.104]    [Pg.1]    [Pg.267]    [Pg.104]    [Pg.1]    [Pg.104]    [Pg.286]    [Pg.57]    [Pg.284]    [Pg.289]    [Pg.290]    [Pg.110]    [Pg.107]    [Pg.457]    [Pg.340]    [Pg.341]    [Pg.162]    [Pg.42]    [Pg.71]    [Pg.291]   


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