Extended AbstractOver the last decade, extensive advances have been made in the understanding of protein crystallization; for summaries see ROSENBERGER, ROSENBERGER et al.. Proteins crystallize by layer spreading mechanisms. This is macroscopically indicated by well developed facets that are often observed. On a molecular level, layer growth has been revealed by electron microscopy (DURBIN, FEHER) and atomic force microscopy studies (DURBIN et al.; KONNERT et al.; MCPHERSON et al.; LAND et al.; MALKIN et al.) that reproduced the whole body of morphology scenarios known for crystallization from inorganic solutions. These include layer spreading from dislocations and 2D nuclei, interaction of growth steps from sources of different activity, and impediment of step propagation by impurities and foreign particles.Since the earliest kinetics investigations it has become apparent that protein crystal growth is more controlled by interfacial kinetics than by bulk transport; for references see ROSENBERGER et al.. Furthermore, two to three orders of magnitude higher supersaturations are required than in inorganic solution growth, to obtain comparable growth rates. Due to these slow kinetics and the large size of the solute macro-ions (crystal building blocks) involved, the interplay between the bulk transport-dependent supply of solute and impurities and the interfacial kinetics can be investigated by conventional optical means. Thus, proteins present ideal model systems for advanced crystal growth studies Particularly detailed insight on the growth kinetics has been obtained from in-situ highresolution interferometric microscopy (VEKILOV et al., 1995a), which permits the simultaneous acquisition of practically continuous time traces of the normal growth rate R and vicinal slope p at various locations across whole crystal faces. Since p is proportional to the local growth step density, these observations permit correlations between the bulk transport, that can be modified, and the microscopic morphological response in the form of the spatio-temporal changes in step motion.The results, when time-averaged over periods of the order of ten minutes reveal the pertinence of all intrinsic and impurity-induced kinetics mechanisms observed in inorganic systems VEKILOV et al., 1995b;LIN et al.;. However, utilization of the high temporal resolution afforded by this advanced interferometric technique, resulted in a new understanding of step propagation. It was found that even under highly stable external solution conditions, both R and p undergo strong fluctuations with a characteristic time of a few minutes . The unsteadiness in p reveals that the fluctuations are due to the bunching and debunching of