Cagnetta Francesco, Škultéty Viktor, Evans Martin R, Marenduzzo Davide
SUPA, School of Physics and Astronomy, The University of Edinburgh, Edinburgh, EH9 3FD Scotland, United Kingdom.
Phys Rev E. 2022 Jan;105(1-1):014610. doi: 10.1103/PhysRevE.105.014610.
Motivated by experimental observations of patterning at the leading edge of motile eukaryotic cells, we introduce a general model for the dynamics of nearly-flat fluid membranes driven from within by an ensemble of activators. We include, in particular, a kinematic coupling between activator density and membrane slope which generically arises whenever the membrane has a nonvanishing normal speed. We unveil the phase diagram of the model by means of a perturbative field-theoretical renormalization group analysis. Due to the aforementioned kinematic coupling the natural early-time dynamical scaling is acoustic, that is the dynamical critical exponent is 1. However, as soon as the the normal velocity of the membrane is tuned to zero, the system crosses over to diffusive dynamic scaling in mean field. Distinct critical points can be reached depending on how the limit of vanishing velocity is realized: in each of them corrections to scaling due to nonlinear coupling terms must be taken into account. The detailed analysis of these critical points reveals novel scaling regimes which can be accessed with perturbative methods, together with signs of strong coupling behavior, which establishes a promising ground for further nonperturbative calculations. Our results unify several previous studies on the dynamics of active membrane, while also identifying nontrivial scaling regimes which cannot be captured by passive theories of fluctuating interfaces and are relevant for the physics of living membranes.
受运动真核细胞前沿图案形成实验观察结果的启发,我们引入了一个通用模型,用于描述由一组激活剂从内部驱动的近平面流体膜的动力学。特别地,我们纳入了激活剂密度与膜斜率之间的运动学耦合,只要膜具有非零法向速度,这种耦合通常就会出现。我们通过微扰场论重整化群分析揭示了该模型的相图。由于上述运动学耦合,自然的早期动力学标度是声学的,即动力学临界指数为1。然而,一旦膜的法向速度调至零,系统在平均场中就会转变为扩散动力学标度。根据实现速度消失极限的方式,可以达到不同的临界点:在每个临界点,都必须考虑非线性耦合项对标度的修正。对这些临界点的详细分析揭示了可以用微扰方法进入的新标度区域,以及强耦合行为的迹象,这为进一步的非微扰计算奠定了有前景的基础。我们的结果统一了先前关于活性膜动力学的多项研究,同时也确定了波动界面的被动理论无法捕捉的非平凡标度区域,这些区域与活膜的物理学相关。