Dissipation splits the 1D Mott transition into two distinct critical points via an intermediate compressible gapless dissipative phase with zero superfluid stiffness.
Polymerized Membranes, a Review
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
Membranes are of great technological and biological as well as theoretical interest. Two main classes of membranes can be distinguished: Fluid membranes and polymerized, tethered membranes. Here, we review progress in the theoretical understanding of polymerized membranes, i.e. membranes with a fixed internal connectivity. We start by collecting basic physical properties, clarifying the role of bending rigidity and disorder, theoretically and experimentally as well as numerically. We then give a thorough introduction into the theory of self-avoiding membranes, or more generally non-local field theories with delta-like interactions. Based on a proof of perturbative renormalizability for non-local field-theories, renormalization group calculations can be performed up to 2-loop order, which in 3 dimensions predict a crumpled phase with fractal dimension of about 2.4. The tricritical behavior of membranes is discussed and shown to be quite different from that of polymers. Dynamical properties are studied in the same frame-work. Along the same lines, disorder can be included leading to interesting applications. We also construct a generalization of the O(N)-model, which in the limit N->0 reduces to self-avoiding membranes in analogy with the O(N)-model, which in the limit N->0 reduces to self-avoiding polymers. We also describe the instanton-contribution governing the large-order behavior of perturbation theory. Some technical details are relegated to the appendices.
fields
cond-mat.str-el 1years
2026 1verdicts
UNVERDICTED 1representative citing papers
citing papers explorer
-
Dissipation splits the Mott transition in one dimension
Dissipation splits the 1D Mott transition into two distinct critical points via an intermediate compressible gapless dissipative phase with zero superfluid stiffness.