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细胞随机内化纳米颗粒的模型。

Model for random internalization of nanoparticles by cells.

机构信息

Department of Mathematics, <a href="https://ror.org/027m9bs27">University of Manchester</a>, Manchester M13 9PL, United Kingdom.

Laboratory of Stochastic Transport of Nanoparticles in Living Systems, Laboratory of Multi-Scale Mathematical Modeling, Department of Theoretical and Mathematical Physics, <a href="https://ror.org/00hs7dr46">Ural Federal University</a>, Lenin Avenue, 51, Ekaterinburg 620000, Russia.

出版信息

Phys Rev E. 2024 Oct;110(4-1):044101. doi: 10.1103/PhysRevE.110.044101.

DOI:10.1103/PhysRevE.110.044101
PMID:39562967
Abstract

We propose a stochastic model for the internalization of nanoparticles by cells formulating cellular uptake as a compound Poisson process with a random probability of success. This is an alternative approach to the one presented by Rees et al. [Nat. Commun. 10, 2341 (2019)2041-172310.1038/s41467-018-07882-8] who explained overdispersion in nanoparticle uptake and associated negative binomial distribution by considering a Poisson distribution for particle arrival and a gamma-distributed cell area. In our stochastic model, the formation of new pits is represented by the Poisson process, whereas the capturing process and the population heterogeneity are described by a random Bernoulli process with a beta-distributed probability of success. The random probability of success generates ensemble-averaged conditional transition probabilities that increase with the number of newly formed pits (self-reinforcement). As a result, an ensemble-averaged nanoparticle uptake can be represented as a Polya process. We derive an explicit formula for the distribution of the random number of pits containing nanoparticles. In the limit of the fast nucleation and low probability of nanoparticle capture, we find the negative binomial distribution.

摘要

我们提出了一个细胞内纳米颗粒内化的随机模型,将细胞摄取表述为具有随机成功概率的复合泊松过程。这是 Rees 等人提出的方法的一种替代方法[Nat. Commun. 10, 2341 (2019)2041-172310.1038/s41467-018-07882-8],他们通过考虑粒子到达的泊松分布和细胞面积的伽马分布来解释纳米颗粒摄取的过分散性和相关的负二项分布。在我们的随机模型中,新坑的形成由泊松过程表示,而捕获过程和种群异质性由具有贝塔分布成功概率的随机伯努利过程描述。随机成功概率产生了随新形成坑(自我强化)数量增加的平均条件转移概率。结果,平均纳颗粒摄取可以表示为 Polya 过程。我们推导出了包含纳米颗粒的随机坑数量分布的显式公式。在快速成核和纳米颗粒捕获概率低的极限下,我们发现了负二项分布。

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