is applied for the first time this steady state is usually initially set by repeatedly running the measurement sequence without data acquisition before actual acquisition starts in a first case the aim is for example that the transverse steady state magnetization reaches a maximum in region v 1 and then disappears in region v 2 wherein in this example it must be assumed that the given experimental parameters are identical throughout the region of the object to achieve this the following stipulations must be made for the pulses p n as shown in fig5 in region v 1 the pulses must have a flip angle u03b1 opt and a pulse phase u03c6 n 0 u00b0 for odd n and u03c6 n 180 u00b0 for even n in region v 2 u03b1 opt must also be implemented as a flip angle but u03c6 n 0 u00b0 must be achieved for all n these stipulations can be met for example with b 1 tailoring by selecting amplitude and phase factors for the individual transmission elements ta 1 tan for a sufficiently large number of existing degrees of freedom such that in a first configuration in both regions an identical amplitude and phase of the b 1 field of the transmission antenna device is achieved in a second configuration the factors are chosen such that an amplitude identical in both regions is still achieved but with a phase offset by 180 u00b0 in v 1 in consecutive repetitions the same rf waveform is now injected alternately with these two transmission configurations alternatively to b 1 tailoring the above stipulations can also be met by means of zrshfp to achieve this suitable additional magnetic fields must first be selected and then according to reference 5 for example the amplitude and.