The method according to one of the preceding claims, wherein said sequence of radio frequency pulses further comprises a first 90° radio frequency pulse (RF1) having a phase φ11 and acting on the protons, wherein the first group (NA) of 180° radio frequency pulses is consecutively applied nA times during said first time interval (τA) after said first 90° radio frequency pulse (RF1), and wherein said sequence of radio frequency pulses further comprises a second 90° radio frequency pulse (RF2) having a phase φ12 and acting on the protons, which second 90° radio frequency pulse (RF2) succeeds the first 90° radio frequency pulse (RF1) and is applied to the protons at an end of the first time interval (τA), wherein the second group (NB) of 180° radio frequency pulses is consecutively applied ng times during said second time interval (τB) after said second 90° radio frequency pulse (RF2), and wherein said sequence of radio frequency pulses further comprises a third 90° radio frequency pulse (RF3) having a phase φ13 and acting on the protons, which third 90° radio frequency pulse (RF3) succeeds the second 90° radio frequency pulse (RF2) and is applied to the protons at an end of the second time interval (τB), wherein the third group (NC) of 180° radio frequency pulses is consecutively applied nC times during said third time interval (τC) after said third 90° radio frequency pulse (RF3).