Aebischer Annina, Gumy Frédéric, Bünzli Jean-Claude G
Laboratory of Lanthanide Supramolecular Chemistry, Ecole Polytechnique Fédérale de Lausanne (EPFL), BCH 1402, 1015 Lausanne, Switzerland.
Phys Chem Chem Phys. 2009 Mar 7;11(9):1346-53. doi: 10.1039/b816131c. Epub 2009 Jan 19.
The efficiency with which the surroundings of trivalent lanthanide ions sensitize their luminescence (eta(sens)) is a key parameter in the design of highly emitting molecular edifices and materials. Evaluation of eta(sens) requires the measurement of the overall and intrinsic quantum yields obtained upon ligand and metal excitation, respectively. We describe a modified integration sphere enabling absolute determination of these quantities on small amounts of solid samples or solutions (60 muL). The sphere is tested for linear response of emitted versus absorbed light intensities with increasing concentration of Cs(3)[Ln(dpa)(3)] solutions (Ln = Eu, Tb). The overall (Q = 29 +/- 2%) and intrinsic (Q = 41 +/- 2%) quantum yields obtained for Eu allow the direct calculation of eta(sens) (71 +/- 6%) while the radiative lifetime (tau(rad) = 4.1 +/- 0.3 ms) is calculated from Q and the observed lifetime. The intrinsic quantum yield matches the value extracted from emission parameters using the simplified equation proposed by Werts et al. but, on the other hand, the theoretical estimate using spontaneous transition probabilities calculated from Judd-Ofelt (JO) parameters is off by -25% (3.15 ms). In the case of Cs(3)[Tb(dpa)(3)], the molar absorption coefficient of the (5)D(4)<--(7)F(6) transition is too small to measure Q for the solution but this quantity could be determined for the microcrystalline sample (72 +/- 5%, tau(rad) = 1.9 +/- 0.1 ms). In this case, the JO theoretical estimate leads to a much too short tau(rad) value. The large difference in eta(sens) for microcrystalline samples of Eu (85%) and Tb (42%) tris(dipicolinates) is attributed to back energy transfer in the latter compound consecutive to a sizeable overlap between the (5)D(4)-->(7)F(6) emission and the absorption spectrum of the dipicolinate triplet, this overlap being smaller in the case of the solution. The overall quantum yield of Na(3)[Yb(dpa)(3)] in aqueous solution is very low (0.015 +/- 0.002%) due to both poor sensitization efficiency (8%) and small intrinsic quantum yield (Q = 0.178 +/- 0.003%; tau(rad) = 1.31 +/- 0.02 ms). For evaluating intrinsic quantum yields of Yb in aqueous solutions of coordination compounds from lifetimes, a value of 1.2-1.3 ms is recommended.
三价镧系离子周围环境敏化其发光的效率(η(sens))是设计高发光分子结构和材料的关键参数。评估η(sens)需要分别测量配体激发和金属激发时获得的总量子产率和本征量子产率。我们描述了一种改进的积分球,能够对少量固体样品或溶液(60 μL)绝对测定这些量。该积分球针对Cs(3)[Ln(dpa)(3)]溶液(Ln = Eu、Tb)浓度增加时发射光与吸收光强度的线性响应进行了测试。Eu的总量子产率(Q = 29 ± 2%)和本征量子产率(Q = 41 ± 2%)使得可以直接计算η(sens)(71 ± 6%),而辐射寿命(τ(rad) = 4.1 ± 0.3 ms)则根据Q和观测寿命计算得出。本征量子产率与使用Werts等人提出的简化方程从发射参数提取的值相符,但另一方面,使用从Judd-Ofelt(JO)参数计算的自发跃迁概率的理论估计偏差为 -25%(3.15 ms)。在Cs(3)[Tb(dpa)(3)]的情况下,(5)D(4)<--(7)F(6)跃迁的摩尔吸收系数太小,无法测量该溶液的Q,但可以确定微晶样品的该量(72 ± 5%,τ(rad) = 1.9 ± 0.1 ms)。在这种情况下,JO理论估计得出的τ(rad)值太短。Eu和Tb的三(二吡啶甲酸)微晶样品的η(sens)差异很大(分别为85%和42%),这归因于后者化合物中存在反向能量转移,这是由于(5)D(4)-->(7)F(6)发射与二吡啶甲酸三重态的吸收光谱之间有相当大的重叠,而在溶液中这种重叠较小。Na(3)[Yb(dpa)(3)]在水溶液中的总量子产率非常低(0.015 ± 0.002%),这是由于敏化效率差(8%)和本征量子产率小(Q = 0.178 ± 0.003%;τ(rad) = 1.31 ± 0.02 ms)。为了根据寿命评估配位化合物水溶液中Yb的本征量子产率,建议使用1.2 - 1.3 ms的值。