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本文引用的文献

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How to make a DNA chip.如何制作DNA芯片。
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Polymer brushes.聚合物刷。
Science. 1991 Feb 22;251(4996):905-14. doi: 10.1126/science.251.4996.905.
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Kinetic measurements of DNA hybridization on an oligonucleotide-immobilized 27-MHz quartz crystal microbalance.在固定有寡核苷酸的27兆赫兹石英晶体微天平上进行DNA杂交的动力学测量。
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Effect of end-group sticking energy on the properties of polymer brushes: comparing experiment and theory.端基粘附能对聚合物刷性质的影响:实验与理论的比较
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Hybridization isotherms of DNA microarrays and the quantification of mutation studies.DNA微阵列的杂交等温线与突变研究的定量分析
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The thermodynamics of DNA structural motifs.DNA结构基序的热力学
Annu Rev Biophys Biomol Struct. 2004;33:415-40. doi: 10.1146/annurev.biophys.32.110601.141800.
8
Sensitivity, specificity, and the hybridization isotherms of DNA chips.DNA芯片的灵敏度、特异性及杂交等温线。
Biophys J. 2004 Feb;86(2):718-30. doi: 10.1016/S0006-3495(04)74150-8.
9
Solving the riddle of the bright mismatches: labeling and effective binding in oligonucleotide arrays.解开明亮错配之谜:寡核苷酸阵列中的标记与有效结合
Phys Rev E Stat Nonlin Soft Matter Phys. 2003 Jul;68(1 Pt 1):011906. doi: 10.1103/PhysRevE.68.011906. Epub 2003 Jul 16.
10
Modeling of DNA microarray data by using physical properties of hybridization.利用杂交物理特性对DNA微阵列数据进行建模。
Proc Natl Acad Sci U S A. 2003 Jun 24;100(13):7575-80. doi: 10.1073/pnas.0832500100. Epub 2003 Jun 13.

DNA芯片上的刷效应:热力学、动力学及设计准则

Brush effects on DNA chips: thermodynamics, kinetics, and design guidelines.

作者信息

Halperin A, Buhot A, Zhulina E B

机构信息

UMR 5819 SPrAM (UJF, CNRS, CEA), DRFMC, CEA Grenoble, France.

出版信息

Biophys J. 2005 Aug;89(2):796-811. doi: 10.1529/biophysj.105.063479. Epub 2005 May 20.

DOI:10.1529/biophysj.105.063479
PMID:15908581
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1366630/
Abstract

In biology experiments, oligonucleotide microarrays are contacted with a solution of long nucleic acid targets. The hybridized probes thus carry long tails. When the surface density of the oligonucleotide probes is high enough, the progress of hybridization gives rise to a polyelectrolyte brush due to mutual crowding of the nucleic acid tails. The free-energy penalty associated with the brush modifies both the hybridization isotherms and the rate equations: the attainable hybridization is lowered significantly as is the hybridization rate. When the equilibrium hybridization fraction, x(eq), is low, the hybridization follows a Langmuir type isotherm, x(eq)/(1 - x(eq)) = c(t)K where c(t) is the target concentration and K is the equilibrium constant. K is smaller than its bulk value by a factor (n/N)(2/5) due to wall effects where n and N denote the number of bases in the probe and the target. At higher x(eq), when the brush is formed, the leading correction is x(eq)/(1 - x(eq)) = c(t)K exp - const'x(eq)(2/3) - x(B)(2/3) where x(B) corresponds to the onset of the brush regime. The denaturation rate constant in the two regimes is identical. However, the hybridization rate constant in the brush regime is lower, the leading correction being exp -const' x(2/3) - x(B)(2/3).

摘要

在生物学实验中,寡核苷酸微阵列与长核酸靶标的溶液接触。由此杂交的探针带有长尾巴。当寡核苷酸探针的表面密度足够高时,由于核酸尾巴的相互拥挤,杂交过程会产生聚电解质刷。与该刷相关的自由能惩罚会改变杂交等温线和速率方程:可达到的杂交显著降低,杂交速率也是如此。当平衡杂交分数x(eq)较低时,杂交遵循朗缪尔型等温线,x(eq)/(1 - x(eq)) = c(t)K,其中c(t)是靶标浓度,K是平衡常数。由于壁效应,K比其本体值小一个因子(n/N)(2/5),其中n和N分别表示探针和靶标中的碱基数。在较高的x(eq)时,当形成刷时,主要的校正为x(eq)/(1 - x(eq)) = c(t)K exp - const'x(eq)(2/3) - x(B)(2/3),其中x(B)对应于刷状区域的起始。两种情况下的变性速率常数相同。然而,刷状区域中的杂交速率常数较低,主要校正为exp -const' x(2/3) - x(B)(2/3)。