The CAMELSPIN experiment, introduced by Bothner-By et al. (1, 2), makes it possible to study nuclear Overhauser effect (NOE) enhancements in molecules where the motional correlation time is such that there are no enhancements in conventional NOE spectra. In conventional NOE studies positive enhancements are expected for small rapidly tumbling molecules, while negative enhancements are expected for large slowly tumbling molecules. A significant number of medium-sized molecules have correlation times that result in NOE enhancements near to the zero-crossing point between these two extremes and hence show either no or only very small enhancements. The CAMELSPIN experiment detects cross relaxation between spinlocked transverse magnetization, in contrast to conventional NOE experiments which utilize longitudinal magnetization. The precise dynamics of cross relaxation between transverse magnetizations are such that positive NOE enhancements are seen for all correlation times (I, 3), thus making it possible to study molecules for which conventional NOE experiments yield no enhancements. The conditions of spin locking used in the CAMELSPIN experiment can also bring about coherence transfer between scalar-coupled spins (4-7). This type of transfer can be utilized for correlation spectroscopy of various kinds (such as the TOCSY experiment (6)), and has recently been dubbed HOHAHA by Bax et al. ( 7). Such transfer between scalar-coupled spins is very undesirable in CAMELSPIN spectra since the resulting cross peaks may obscure the desired NOE cross peaks or, more seriously, may give rise to “false” NOE cross peaks (8, 9). These false cross peaks arise from an NOE transfer followed by a HOHAHA transfer (or vice versa) and they are indistinguishable in a single spectrum from genuine NOE cross peaks. The presence of these false NOE cross peaks can thus cause substantial errors or ambiguities of interpretation. The purpose of this communication is to describe a modified method of recording CAMELSPIN spectra in which the HOHAHA mechanism is effectively suppressed, thus allowing such spectra to be interpreted without ambiguity. Differentiation of NOE and HOHAHA transfer is impossible using the usual methods of phase cycling or randomization of the mixing time. However, the two processes vary greatly in their sensitivity to the offset and field strength of the spin-locking field and have different time dependences. The method described here utilizes these