Department of Chemistry and the Smalley-Curl Institute, Rice University, Houston, Texas 77005, United States.
Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, United States.
ACS Nano. 2023 Sep 12;17(17):17568-17575. doi: 10.1021/acsnano.3c06906. Epub 2023 Aug 30.
Time-resolved fluorescence spectroscopy has been used to study the displacement of adsorbed sodium dodecyl sulfate (SDS) from the surface of single-wall carbon nanotubes (SWCNTs) by short strands of single-stranded DNA. Intensity changes in near-infrared emission peaks of various SWCNT structures were analyzed following the addition of six different (GT) oligomers ( from 3 to 20) to SDS-coated nanotube samples. There is a strong kinetic dependence on the oligomer length, with (GT) giving an initial rate more than 300 times greater than that of (GT). For shorter oligos in the (GT) series, we observe an inverse dependence of the displacement rate on the SWCNT diameter, with SDS displaced from (6,5) more than twice as fast as from (8,7). However, this diameter dependence is reversed for oligos with more than six (GT) units. There is also a systematic dependence of the displacement rate on the nanotube chiral angle that is strongest for (GT), leading to a factor of ∼3 initial rate difference between (9,1) and (6,5) despite their identical diameters. To account for these findings, we propose a simple two-step kinetic model in which disruption of the original SDS coating is followed by conformational relaxation of ssDNA on the nanotube surface. The relaxation is relatively fast for ssDNA oligos shorter than 12 bp, making the first step rate-determining. Conversely, relaxation of the longer oligomers is slow enough that the second step becomes rate-determining.
时间分辨荧光光谱法已被用于研究短链单链 DNA 从单壁碳纳米管 (SWCNT) 表面取代吸附的十二烷基硫酸钠 (SDS)。在向 SDS 涂覆的纳米管样品中添加六种不同的 (GT) 寡聚物(3 到 20 个碱基)后,分析了各种 SWCNT 结构的近红外发射峰的强度变化。寡聚物长度对动力学有很强的依赖性,(GT) 的初始速率比 (GT) 高 300 多倍。对于 (GT) 系列中较短的寡聚物,我们观察到置换速率与 SWCNT 直径的反比关系,(6,5) 从 SDS 中的置换速度比 (8,7) 快两倍以上。然而,对于具有超过六个 (GT) 单元的寡聚物,这种直径依赖性则相反。置换速率还与纳米管手性角存在系统依赖性,对于 (GT) 而言,这种依赖性最强,导致 (9,1) 和 (6,5) 之间的初始速率差异约为 3 倍,尽管它们的直径相同。为了解释这些发现,我们提出了一个简单的两步动力学模型,其中原始 SDS 涂层的破坏接着是 ssDNA 在纳米管表面的构象松弛。对于短于 12 个碱基的 ssDNA 寡聚物,松弛相对较快,因此第一步是速率决定步骤。相反,较长寡聚物的松弛速度足够慢,使得第二步成为速率决定步骤。