Islam Sk Imadul, Pyne Partha, Das Dipak Kumar, Mukherjee Shounak, Chakrabarty Suman, Mitra Rajib Kumar
Department of Chemical Biological and Macromolecular Sciences, S.N. Bose National Centre for Basic Sciences, Block JD, Sector III, Salt Lake, Kolkata 700106, India.
Langmuir. 2022 Mar 15;38(10):3105-3112. doi: 10.1021/acs.langmuir.1c02999. Epub 2022 Mar 4.
Both electrostatic and hydrophobic interactions play pivotal roles in ligand-surfactant binding interaction, especially for ionic surfactants. While much studies have been reported in the micellar region, less attention has been paid on such interactions at a low (premicellar) surfactant concentration. We here study the interaction between the cationic dye rhodamine 6G (R6G) with surfactants of different charge types: anionic SDS, cationic CTAB, and nonionic Tx 100 using absorption and emission spectroscopy. We identify that R6G forms dimeric aggregates at a premicellar concentration of SDS. Formation of aggregates is also confirmed from classical simulation measurements. CTAB and Tx 100 do not form any such aggregate, presumably owing to unfavorable electrostatic interactions. For a molecular-level understanding, we perform two-photon absorption (TPA) spectroscopy for the same systems. TPA allows us to calculate the two-photon absorption cross section and subsequently the change in the dipole moment (Δμ) between ground and excited states of the dye. We calculate the Δμ and observe that it passes through a maximum at a surfactant concentration half of the critical micelle concentration of SDS. This observation imparts support to earlier quantum mechanical calculation, which infers deviation from the parallel orientation of the dye during surfactant-induced aggregation. We extended our measurements and varied the carbon chain length of the anionic surfactant, and we found that all of them exhibit a maximum in Δμ, while their relative magnitude is dependent on the surfactant carbon chain length.
静电相互作用和疏水相互作用在配体 - 表面活性剂结合相互作用中都起着关键作用,尤其是对于离子型表面活性剂。虽然在胶束区域已经报道了很多研究,但在低(胶束前)表面活性剂浓度下对这种相互作用的关注较少。我们在此使用吸收光谱和发射光谱研究阳离子染料罗丹明6G(R6G)与不同电荷类型的表面活性剂之间的相互作用:阴离子型十二烷基硫酸钠(SDS)、阳离子型十六烷基三甲基溴化铵(CTAB)和非离子型吐温100(Tx 100)。我们发现R6G在SDS的胶束前浓度下形成二聚体聚集体。经典模拟测量也证实了聚集体的形成。CTAB和Tx 100不会形成任何此类聚集体,可能是由于不利的静电相互作用。为了从分子水平上理解,我们对相同的体系进行了双光子吸收(TPA)光谱研究。TPA使我们能够计算双光子吸收截面,并随后计算染料基态和激发态之间的偶极矩变化(Δμ)。我们计算了Δμ,观察到它在SDS临界胶束浓度一半的表面活性剂浓度处达到最大值。这一观察结果支持了早期的量子力学计算,该计算推断在表面活性剂诱导的聚集过程中染料的取向偏离平行。我们扩展了测量范围并改变了阴离子表面活性剂的碳链长度,发现它们都在Δμ处出现最大值,而它们的相对大小取决于表面活性剂的碳链长度。