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State Estimation of the Time-Varying and Spatially Localized Concentration of Signal Molecules from the Stochastic Adsorption Dynamics on the Carbon Nanotube-Based Sensors and Its Application to Tumor Cell Detection

机译:基于碳纳米管传感器的随机吸附动力学的信号分子时变和空间局部浓度状态估计及其在肿瘤细胞检测中的应用

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摘要

This paper addresses a problem of estimating time-varying, local concentrations of signal molecules with a carbon-nanotube (CNT)-based sensor array system, which sends signals triggered by monomolecular adsorption/desorption events of proximate molecules on the surfaces of the sensors. Such sensors work on nano-scale phenomena and show inherently stochastic non-Gaussian behavior, which is best represented by the chemical master equation (CME) describing the time evolution of the probabilities for all the possible number of adsorbed molecules. In the CME, the adsorption rate on each sensor is linearly proportional to the local concentration in the bulk phase. State estimators are proposed for these types of sensors that fully address their stochastic nature. For CNT-based sensors motivated by tumor cell detection, the particle filter, which is nonparametric and can handle non-Gaussian distributions, is compared to a Kalman filter that approximates the underlying distributions by Gaussians. In addition, the second-order generalized pseudo Bayesian estimation (GPB2) algorithm and the Markov chain Monte Carlo (MCMC) algorithm are incorporated into KF and PF respectively, for detecting latent drift in the concentration affected by different states of a cell.
机译:本文解决了使用基于碳纳米管(CNT)的传感器阵列系统估算信号分子随时间变化的局部浓度的问题,该系统发送传感器表面上邻近分子的单分子吸附/解吸事件触发的信号。这种传感器可处理纳米尺度的现象,并表现出固有的随机非高斯行为,最好用化学主方程(CME)表示,该方程描述了所有可能数量的被吸附分子的概率随时间的演化。在CME中,每个传感器上的吸附速率与本体相中的局部浓度成线性比例。针对这些类型的传感器提出了状态估计器,以充分解决其随机性。对于由肿瘤细胞检测驱动的基于CNT的传感器,将非参数化且可以处理非高斯分布的粒子过滤器与近似于高斯分布的基本分布的卡尔曼过滤器进行比较。此外,将二阶广义伪贝叶斯估计(GPB2)算法和马尔可夫链蒙特卡洛(MCMC)算法分别合并到KF和PF中,以检测受单元状态不同影响的浓度中的潜在漂移。

著录项

  • 期刊名称 other
  • 作者单位
  • 年(卷),期 -1(10),11
  • 年度 -1
  • 页码 e0141930
  • 总页数 21
  • 原文格式 PDF
  • 正文语种
  • 中图分类
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  • 入库时间 2022-08-21 11:14:04

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