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. Author manuscript; available in PMC: 2017 Nov 30.
Published in final edited form as: Magn Reson Med. 2013 Nov 11;72(3):806–815. doi: 10.1002/mrm.24989

FIG. 1.

FIG. 1

Signal evolution (amplitude and phase) of two different magnetizations after an inversion recovery pulse. The two magnetizations pointing to the z direction at equilibrium (a), will both be inverted after an inversion pulse (b). Due to the different T1 relaxation rates, after a certain delay (TI), opposite polarities will result (c). If an image acquisition is performed at this time, using, for example, a 90° excitation, both of the magnetizations will be flipped to the x–y plane. But due to the opposite Mz polarities before excitation, they will present a π phase difference in the transverse plane (d).