Abstract: Recently, we have shown that net magnetization transfer among scalar coupled homonuclear spins can be obtained by the application of a spin-lock field (I), or more effectively, by the application of a phase-alternated spin-lock field (2, 3). Analogous methods to accomplish net homonuclear magnetization transfer, based on different rfirradiation schemes have previously been reported by Braunschweiler and Ernst (4). As they and others (5-9) have pointed out, the key to net magnetization transfer between two coupled spins, A and X, is to remove the Zeeman contributions, HzA and Hzx, from the Hamiltonian, or to make them identical, i.e., HzA = Hz,. This can be accomplished by suitable rf irradiation schemes or by zero-field NMR (JO). In this communication we describe a new mixing scheme that is based on the MLEV-16 composite pulse decoupling cycle (II). We have modified this cycle to make it less sensitive to pulse imperfections and it will be shown that this type of MLEV mixing provides net magnetization transfer over a substantial bandwidth with only limited rf power. More importantly, the apparent decay constant of spin-locked magnetization can be prolonged by up to a factor of two (compared to TIP) by using this new type of mixing scheme. If the Zeeman part of the Hamiltonian is eliminated, the spin system will evolve solely under the influence of scalar coupling. Magnetization can then propagate through the molecule in a way that is very similar to spin diffusion among protons in a rigid solid, where dipolar couplings are usually much larger than differences in chemical shift. For molecules consisting of only two coupled homonuclear spins, A and X, Braunschweiler and Ernst have shown that in the isotropic coupling limit there is an oscillatory exchange of the A and X magnetization, with period 1 /JAx. Explicit results for the AX2 case have very recently been presented by Chandrakumar and Subramanian (12). For larger spin systems a computer simulation program appears to be the easiest way to predict the rate at which magnetization will propagate through the molecule. AS demonstrated earlier (2), the net magnetization transfer obtained in this type of experiment permits the recording of phase-sensitive spectra, and gives in many cases enhanced resolution and sensitivity compared to the widely used COSY experiment (13-16). For short mixing times (<0.1/J), only direct connectivities will be observed. For longer mixing times, magnetization that has been transferred from spin A to spin M during the first part of the mixing period can be relayed to spin X during the second