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Physics and scaling prospects of pH-based genome sequencers

机译:基于pH的基因组测序仪的物理和规模化前景

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Fig. 2 shows the temporal distribution of proton inside the well and the polymer layer (the diffusion coefficient of protons in electrolyte and polymer is Dfree= 9.31×10−5 and Dpoly= 4×10−8 cm2/s, respectively). The calculated voltage shift (ΔV) in MOSFET successfully explains the experiment data with two different sizes of wells and beads, as shown in Fig. 3. As we scale the microwells by a factor of k, the sensitivity remains constant: this is because the number of protons released from bead is proportional to the bead area (∼ k−2) and the sensor surface area is also scaled by a factor of k−2. Since the surface group charge on the oxide surface changes linearly with proton density while the amount excess protons is much smaller than that in the well, the voltage signal remains constant.
机译:图2显示了孔和聚合物层内部的质子的时间分布(质子在电解质和聚合物中的扩散系数为Dfree = 9.31×10 -5 和Dpoly = 4×10 -8 cm 2 / s)。 MOSFET中计算出的电压漂移(ΔV)成功地解释了两种不同大小的孔和珠子的实验数据,如图3所示。当我们将微孔按k缩放时,灵敏度保持恒定:这是因为从磁珠释放的质子数与磁珠面积成正比(〜k -2 ),传感器表面积也按k -2 的比例缩放。由于氧化物表面上的表面基团电荷随质子密度线性变化,而多余的质子量远小于阱中的质子量,因此电压信号保持恒定。

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