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AMPA 受体在兴奋性突触后密度中的自拥挤现象可以影响异常的受体亚扩散。

Self-crowding of AMPA receptors in the excitatory postsynaptic density can effectuate anomalous receptor sub-diffusion.

机构信息

School of Computational and Integrative Sciences, Jawaharlal Nehru University, New Delhi, India.

出版信息

PLoS Comput Biol. 2018 Feb 14;14(2):e1005984. doi: 10.1371/journal.pcbi.1005984. eCollection 2018 Feb.

DOI:10.1371/journal.pcbi.1005984
PMID:29444074
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5812565/
Abstract

AMPA receptors (AMPARs) and their associations with auxiliary transmembrane proteins are bulky structures with large steric-exclusion volumes. Hence, self-crowding of AMPARs, depending on the local density, may affect their lateral diffusion in the postsynaptic membrane as well as in the highly crowded postsynaptic density (PSD) at excitatory synapses. Earlier theoretical studies considered only the roles of transmembrane obstacles and the AMPAR-binding submembranous scaffold proteins in shaping receptor diffusion within PSD. Using lattice model of diffusion, the present study investigates the additional impacts of self-crowding on the anomalousity and effective diffusion coefficient (Deff) of AMPAR diffusion. A recursive algorithm for avoiding false self-blocking during diffusion simulation is also proposed. The findings suggest that high density of AMPARs in the obstacle-free membrane itself engenders strongly anomalous diffusion and severe decline in Deff. Adding transmembrane obstacles to the membrane accentuates the anomalousity arising from self-crowding due to the reduced free diffusion space. Contrarily, enhanced AMPAR-scaffold binding, either through increase in binding strength or scaffold density or both, ameliorates the anomalousity resulting from self-crowding. However, binding has differential impacts on Deff depending on the receptor density. Increase in binding causes consistent decrease in Deff for low and moderate receptor density. For high density, binding increases Deff as long as it reduces anomalousity associated with intense self-crowding. Given a sufficiently strong binding condition when diffusion acquires normal behavior, further increase in binding causes decrease in Deff. Supporting earlier experimental observations are mentioned and implications of present findings to the experimental observations on AMPAR diffusion are also drawn.

摘要

AMPA 受体 (AMPARs) 及其与辅助跨膜蛋白的结合物是具有较大空间位阻体积的庞杂结构。因此,AMPAR 的自拥挤程度(取决于局部密度)可能会影响它们在突触后膜中的侧向扩散,以及在兴奋性突触后致密区(PSD)中的高度拥挤状态下的扩散。早期的理论研究仅考虑了跨膜障碍和 AMPAR 结合的亚膜基质蛋白在塑造 PSD 内受体扩散中的作用。本研究使用扩散晶格模型,研究了自拥挤对 AMPAR 扩散的异常性和有效扩散系数 (Deff) 的额外影响。还提出了一种用于避免扩散模拟中虚假自阻塞的递归算法。研究结果表明,无障碍物膜中 AMPAR 密度高本身会导致强烈的异常扩散和 Deff 的严重下降。在膜中添加跨膜障碍会加剧由于自由扩散空间减少而产生的自拥挤引起的异常性。相反,增强 AMPAR 支架的结合(无论是通过增加结合强度、支架密度还是两者同时增加)都可以改善自拥挤引起的异常性。然而,结合对 Deff 的影响因受体密度而异。增加结合会导致低和中等受体密度下的 Deff 持续下降。对于高密度,只要结合能减轻与强烈自拥挤相关的异常性,结合就会增加 Deff。当扩散表现出正常行为时,给出足够强的结合条件,进一步增加结合会导致 Deff 下降。文中提到了与早期实验观察结果的一致性,并对 AMPAR 扩散的实验观察结果进行了分析。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/137161715940/pcbi.1005984.g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/424437061686/pcbi.1005984.g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/277d1de1b169/pcbi.1005984.g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/b4744e538a1e/pcbi.1005984.g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/39cbedb1027d/pcbi.1005984.g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/9d438791290a/pcbi.1005984.g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/896422a84cf2/pcbi.1005984.g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/6476b04df3b5/pcbi.1005984.g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/61b298407214/pcbi.1005984.g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/0adf646260ec/pcbi.1005984.g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/137161715940/pcbi.1005984.g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/424437061686/pcbi.1005984.g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/277d1de1b169/pcbi.1005984.g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/b4744e538a1e/pcbi.1005984.g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/39cbedb1027d/pcbi.1005984.g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/9d438791290a/pcbi.1005984.g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/896422a84cf2/pcbi.1005984.g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/6476b04df3b5/pcbi.1005984.g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/61b298407214/pcbi.1005984.g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/0adf646260ec/pcbi.1005984.g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/946b/5812565/137161715940/pcbi.1005984.g010.jpg

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