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罗丹明 6G 激发能在纤维素微球上的捕获。

Trapping of Rhodamine 6G excitation energy on cellulose microparticles.

机构信息

INQUIMAE/DQIAyQF, Facultad de Ciencias Exactas y Naturales, UBA, Ciudad Universitaria, Pab. II, C1428EHA Buenos Aires, Argentina.

出版信息

Phys Chem Chem Phys. 2010 Mar 7;12(9):2246-53. doi: 10.1039/b919583a. Epub 2010 Jan 18.

Abstract

Rhodamine 6G (R6G) was adsorbed on cellulose microparticles and fluorescence quantum yields and decays were measured as a function of dye loading. Though no spectroscopic evidence of dye aggregation was found, a noticeable decrease of quantum yield--after correction for reabsorption and reemission of fluorescence--and shortening of decays were observed at the highest loadings. These effects were attributed to the dissipation of the excitation energy by traps constituted by R6G pairs, leading to static and dynamic quenching produced by direct absorption of traps and non-radiative energy transfer from monomers, respectively. Regarding the nature of traps, two extreme approaches were considered: (a) equilibrium between monomers slightly interacting in the ground state and (b) randomly distributed monomers located below a critical distance (statistical traps). Both approaches accounted quantitatively for the observed facts. The effect of energy migration was evaluated through computational simulations. As the concentration of traps could only be indirectly inferred, in some experiments an external energy transfer quencher, Methylene Blue, was coadsorbed and the results were compared with those obtained with pure R6G.

摘要

若丹明 6G(R6G)被吸附在纤维素微球上,作为染料负载的函数,测量其荧光量子产率和衰减。尽管没有发现染料聚集的光谱证据,但在最高负载下,观察到量子产率显著降低(经过荧光再吸收和再发射的校正),衰减时间缩短。这些效应归因于由 R6G 对构成的陷阱消耗激发能量,从而导致由陷阱直接吸收和单体非辐射能量转移分别产生静态和动态猝灭。关于陷阱的性质,考虑了两种极端的方法:(a)在基态略微相互作用的单体之间的平衡和(b)位于临界距离以下的随机分布的单体(统计陷阱)。这两种方法都定量地解释了观察到的事实。通过计算模拟评估了能量迁移的影响。由于只能间接推断陷阱的浓度,在某些实验中,共吸附了外源能量转移猝灭剂亚甲蓝,并将结果与纯 R6G 的结果进行了比较。

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