Sigg Daniel, Carnevale Vincenzo
dPET, Spokane, Washington; Institute for Computational Molecular Science, Temple University, Philadelphia, Pennsylvania.
Institute for Computational Molecular Science, Temple University, Philadelphia, Pennsylvania.
Biophys J. 2025 May 6;124(9):1356-1375. doi: 10.1016/j.bpj.2025.02.006. Epub 2025 Feb 12.
The opening kinetics of ion channels are typically modeled using Markov schemes, which assume a finite number of states linked by time-independent rate constants. Although aggregate closed or open states may, under the right conditions, experience short-term (exponential) memory of previous gating events, there is experimental evidence for stretched-exponential or power-law memory decay that does not conform to Markov theory. Here, using Monte Carlo simulations of a lattice system, we investigate long-term memory in channels coupled to a heterogeneous membrane near the critical temperature. We observed that increasing the strength of the channel-lipid coupling parameter from zero to nearly 1 kT per lipid binding site leads to a progression in the autocorrelation of successive open dwell times. This evolution changes from 1) multiexponential decay to 2) power-law decay, and finally to 3) stretched exponential decay, mirroring changes in channel distribution from: 1) complete independence, 2) partitioning in the interphase between lipid domains, and 3) partitioning inside the domain favorable to the activation state of the channel. The intermediate power-law regime demonstrates characteristics of long-term memory, such as trend-reinforcing values of the Hurst exponent. Still, this regime passes a previously proposed Markovianity test utilizing conditional dwell time histograms. We conclude that low-energy state-dependent interactions between ion channels and a dynamic membrane soften the Markov assumption by maintaining a fluctuating microenvironment and storing configurational memory, thus supporting the existence of long memory tails without necessarily diminishing the usefulness of Markov modeling.
离子通道的开放动力学通常使用马尔可夫模型进行建模,该模型假设存在有限数量的状态,这些状态由与时间无关的速率常数相连。尽管在适当条件下,总的关闭或开放状态可能会对先前的门控事件有短期(指数)记忆,但有实验证据表明存在不符合马尔可夫理论的拉伸指数或幂律记忆衰减。在这里,我们使用晶格系统的蒙特卡罗模拟,研究了在临界温度附近与异质膜耦合的通道中的长期记忆。我们观察到,将通道 - 脂质耦合参数的强度从零增加到每个脂质结合位点接近1 kT,会导致连续开放驻留时间的自相关出现变化。这种演变从1)多指数衰减变为2)幂律衰减,最终变为3)拉伸指数衰减,反映了通道分布的变化,从:1)完全独立,2)在脂质域间相中的分配,到3)在有利于通道激活状态的域内的分配。中间的幂律 regime 表现出长期记忆的特征,例如赫斯特指数的趋势增强值。然而,这个 regime 通过了先前提出的利用条件驻留时间直方图的马尔可夫性测试。我们得出结论,离子通道与动态膜之间的低能态依赖相互作用通过维持波动的微环境和存储构型记忆,软化了马尔可夫假设,从而支持了长记忆尾的存在,而不一定会降低马尔可夫建模的有用性。