Kirill Katsov
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fusionSoft condensed matter systems are ubiquitous in nature. Their softness is reflected in a rich spectrum of phenomena, such as self-assembly of amphiphiles in solution, micro-phase separation of block copolymers, liquid crystallinity, visco-elasticity of polymeric solutions and melts, etc. With these unique properties these systems have already found diverse industrial applications ranging from pharmaceuticals to advanced materials and show much promise in the future. Moreover, many phenomena exhibited by the classical soft matter systems apparently hold answers to questions concerned with the structure and dynamics of biological systems. I believe in the idea that even though most biological functions definitely rely on a very specific biochemistry, there is a multitude of universal physical phenomena that provide the basis to this diverse functionality and can be described by generic models. 

In spite of the importance of this field, we are still lacking even basic understanding of many aspects of the underlying mechanisms. The difficulty can be directly linked to the fact that the soft degrees of freedom associated with these phenomena have characteristic length and time scales ranging from the molecular to mesoscopic to macroscopic. Another complicating feature is that these systems can be relatively easily brought out of the equilibrium and/or get trapped in numerous long living metastable states.

confinmentIn my research I apply a range of different approaches (field theory, scaling,  phenomenological and coarse-grained modeling) to address the problems related to equilibrium strongly fluctuating systems (e.g., polymer solutions), out-of-equilibrium systems (bilayer membrane fusion), systems trapped in long living metastable states (defects in self-assembled structures, micelles), the effect of confinement on self-assembly (nano-patterning, novel structures), and mechanical properties of micro-phase separated polymeric systems (linear and non-linear response to strain, viscoelasticity and its coupling to the structure).