Method for operating a magnetic resonance imaging apparatus

Claim 1

A method for operating a magnetic resonance imaging apparatus, comprising the steps of: (a) exciting nuclear spins in an examination subject by emitting an excitation pulse having a flip angle α≦90° and having a phase associated therewith; (b) emitting first gradient pulses including a first gradient pulse in a first direction and a first gradient pulse in a second direction perpendicular to said first direction; (c) reading out nuclear magnetic signals arising in said subject by emitting a second gradient pulse in said first direction and having an opposite operational sign with respect to said first gradient pulse in said first direction; (d) rephasing said nuclear spins by emitting further gradient pulses including a further gradient pulse in said first direction and a further gradient pulse in said second direction; (e) repeating steps (a), (b), (c), and (d) with a repetition time T R with a different first gradient pulse in said second direction in each repetition and with an alternating operational sign of said flip angle thereby causing an inversion of the phase relation of the respective excitation pulses in successive repetitions of step (a), and thereby establishing a steady-state condition wherein the magnetization of the nuclear spins moves approximately between +α/2 and -α/2; and (f) emitting a radiofrequency pulse, before step (a) of each repetition, having a flip angle α/2 and a phase relation which is inverted relative to said excitation pulse in step (a), at a time of T R /2 before said excitation pulse in step (a).

Claim 2

A method for operating a magnetic resonance imaging apparatus, comprising the steps of: (a) exciting nuclear spins in an examination subject by emitting an excitation pulse having a flip angle α≦90° and having a phase associated therewith; (b) emitting first gradient pulses including a first gradient pulse in a first direction and a first gradient pulse in a second direction perpendicular to said first direction; (c) reading out nuclear magnetic signals arising in said subject by emitting a second gradient pulse in said first direction and having an opposite operational sign with respect to said first gradient pulse in said first direction; (d) rephasing said nuclear spins by emitting further gradient pulses including a further gradient pulse in said first direction and a further gradient pulse in said second direction; (e) repeating steps (a), (b), (c), and (d) with a repetition time T R with a different first gradient pulse in said second direction in each repetition and with an alternating operational sign of said flip angle thereby causing an inversion of the phase relation of the respective excitation pulses in successive repetitions of step (a), and thereby establishing a steady-state condition wherein the magnetization of the nuclear spins moves approximately between +α/2 and -α/2; and (f) emitting a radiofrequency pulse, before step (a) of each repetition, having a flip angle α/2 and a phase relation which is inverted relative to said excitation pulse in step (a), at a time of T R /2 before said excitation pulse in step (a).