Crystal growth mechanisms are crucial to understanding the complexity of crystal morphologies in nature and advanced technological materials, such as the faceting and dendrites found in snowflakes and the microstructure and associated strength properties of structural and icy planetary materials. In this article, we present observations of pressure-induced ice VI crystal growth, which have been predicted theoretically, but had never been observed experimentally to our knowledge. Under modulated pressure conditions in a dynamic-diamond anvil cell, rough single ice VI crystal initially grows into well defined octahedral crystal facets. However, as the compression rate increases, the crystal surface dramatically changes from rough to facet, and from convex to concave because of a surface instability, and thereby the growth rate suddenly increases by an order of magnitude. Depending on the compression rate, this discontinuous jump in crystal growth rate or ''shock crystal growth'' eventually produces 2D carpet-type fractal morphology, and moreover dendrites form under sinusoidal compression, whose crystal morphologies are remarkably similar to those predicted in theoretical simulations under a temperature gradient field. The observed strong dependence of the growth mechanism on compression rate, therefore, suggests a different approach to developing a comprehensive understanding of crystal growth dynamics.dynamic-diamond anvil cell C rystal morphology and microstructure of ice strongly alter rheological properties of solids and, thus, affect the dynamics and evolution of many water-rich solid bodies in the solar system such as Earth crest, Pluto, Titan, and comets. Crystal growth also exhibits many interesting phenomena such as roughening-faceting transitions (1-3), surface instabilities (4), and fractal and dendritic growth (4, 5). There have been extensive studies (1-6) of the faceting and dendritic shapes of crystals, which represent, respectively, the simplest and the most complex morphologies, and play significant roles in pattern formation, metallurgy, and biology. The two morphologies have been explained by interface-and diffusion-controlled growth, i.e., atomic or molecular attachment kinetics across the interface between liquids and crystals for the former and diffusion of heat or mass for the latter. Growth mechanisms, however, are not very well understood yet, even in the case of simple facet growth, for example, the faceting and surface instability in two dimensions depending on cooling rate or concentration rate (1, 2), and abnormal growth and protrusion at crystal corners and edges (1-3, 7-9).Facet growth has been explained by a geometric model (7) that describes the interface motion of crystals by the shape and position of the crystal surface because of the slow kinetics of atomic or molecular attachment. Interestingly, the geometric model predicts discontinuous behavior of crystal growth on faceting, called shock that forms when two or more facets or edges meet at the same position at the same time. ...