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    Tb<sup>3+</sup>ā†’Eu<sup>3+</sup> Energy Transfer in Mixed-Lanthanide-Organic Frameworks

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    In this work, we report a theoretical and experimental investigation of the energy transfer mechanism in two isotypical 2D coordination polymers, <sub>āˆž</sub>[(Tb<sub>1ā€“<i>x</i></sub>Eu<sub><i>x</i></sub>)Ā­(DPA)Ā­(HDPA)], where H<sub>2</sub>DPA is pyridine 2,6-dicarboxylic acid and <i>x</i> = 0.05 or 0.50. Emission spectra of <sub>āˆž</sub>[(Tb<sub>0.95</sub>Eu<sub>0.05</sub>)Ā­(DPA)Ā­(HDPA)] and <sub>āˆž</sub>[(Tb<sub>0.5</sub>Eu<sub>0.5</sub>)Ā­(DPA)Ā­(HDPA)], <b>(1)</b> and <b>(2)</b>, show that the high quenching effect on Tb<sup>3+</sup> emission caused by Eu<sup>3+</sup> ion indicates an efficient Tb<sup>3+</sup>ā†’Eu<sup>3+</sup> energy transfer (ET). The <i>k</i><sub>ET</sub> of Tb<sup>3+</sup><i>ā†’</i> Eu<sup>3+</sup> ET and rise rates (<i>k</i><sub>r</sub>) of Eu<sup>3+</sup> as a function of temperature for <b>(1)</b> are on the same order of magnitude, indicating that the sensitization of the Eu<sup>3+Ā 5</sup><i>D</i><sub>0</sub> level is highly fed by ET from the <sup>5</sup><i>D</i><sub>4</sub> level of Tb<sup>3+</sup> ion. The Ī·<sub>ET</sub> and <i>R</i><sub>0</sub> values vary in the 67ā€“79% and 7.15 to 7.93 ƅ ranges. Hence, Tb<sup>3+</sup> is enabled to transfer efficiently to Eu<sup>3+</sup> that can occupy the possible sites at 6.32 and 6.75 ƅ. For <b>(2)</b>, the ET processes occur on average with Ī·<sub>ET</sub> and <i>R</i><sub>0</sub> of 97% and 31 ƅ, respectively. Consequently, Tb<sup>3+</sup> ion is enabled to transfer energy to Eu<sup>3+</sup> localized at different layers. The theoretical model developed by Malta was implemented aiming to insert more insights about the dominant mechanisms involved in the ET between lanthanides ions. Calculated single Tb<sup>3+</sup>ā†’ Eu<sup>3+</sup> ETs are three orders of magnitude inferior to those experimentally; however, it can be explained by the theoretical model that does not consider the role of phonon assistance in the Ln<sup>3+</sup><i>ā†’</i> Ln<sup>3+</sup> ET processes. In addition, the Tb<sup>3+</sup>ā†’ Eu<sup>3+</sup> ET processes are predominantly governed by dipoleā€“dipole (dā€“d) and dipoleā€“quadrupole (d<i>ā€“</i>q) mechanisms
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