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Rapid repetition of the “burst” sequence: The role of diffusion and consequences for imaging

When the Burst pulse sequence (Hennig ef al. MAGMA 1, 39–48 (1993)) is applied with elementary pulses of finite flip angle, a non‐uniform longitudinal magnetization is created, in the form of a series of fine bands of saturated spins. Both during and after the pulse train, the molecules contained within these bands diffuse. In this paper a full description is given of the evolution of the non‐uniform longitudinal magnetization subsequent to the pulse train and the theory is verified experimentally. The value of the diffusion coefficient influences strongly the signal obtained when the Burst sequence is repeated rapidly. The consequences of this for imaging are discussed and, in particular, for the so‐called “frequency‐shifted” Burst technique.