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Rare-Earth and Antimony-Oxo Clusters Simultaneously Connecting Antimonotungstates Comprising Divacant and Tetravacant Keggin Fragments

48

Citations

65

References

2019

Year

Abstract

Four novel rare-earth (RE) and Sb-oxo clusters simultaneously bridging antimonotungstates (ATs) [H<sub>2</sub>N(CH<sub>3</sub>)<sub>2</sub>]<sub>8</sub>Na<sub>6</sub>H<sub>8</sub>{[RE<sub>4</sub>(H<sub>2</sub>O)<sub>6</sub>Sb<sub>6</sub>O<sub>4</sub>](SbW<sub>10</sub>O<sub>37</sub>)<sub>2</sub>(SbW<sub>8</sub>O<sub>31</sub>)<sub>2</sub>}·24H<sub>2</sub>O [RE = Dy<sup>3+</sup> (<b>1</b>), Er<sup>3+</sup> (<b>2</b>), Y<sup>3+</sup> (<b>3</b>), Ho<sup>3+</sup> (<b>4</b>)] were triumphantly isolated by using Na<sub>9</sub>[B-α-SbW<sub>9</sub>O<sub>33</sub>]·19.5H<sub>2</sub>O, dimethylamine hydrochloride, SbCl<sub>3</sub>, and RE(NO<sub>3</sub>)<sub>3</sub>·6H<sub>2</sub>O in acidic aqueous solution. Their tetrameric polyoxoanions are all established by two [SbW<sub>10</sub>O<sub>37</sub>]<sup>11-</sup> and two [B-α-SbW<sub>8</sub>O<sub>31</sub>]<sup>11-</sup> segments encapsulating a RE-Sb heterometal [RE<sub>4</sub>(H<sub>2</sub>O)<sub>6</sub>Sb<sub>6</sub>O<sub>4</sub>]<sup>22+</sup> cluster. Under the O→W LMCT excitation at 268 nm of AT segments, RE ions in <b>1</b> and <b>2</b> can absorb the <sup>3</sup>T<sub>1u</sub>→<sup>1</sup>A<sub>1g</sub> emission energy of AT segments, giving rise to the sensitization of AT segments to the emission of RE ions. Through the sensitization of AT segments, the emission intensities of RE ions in <b>1</b> and <b>2</b> are increased and lifetimes are prolonged. Photoluminescence and energy transfer measurements indicate that Dy<sup>3+</sup> ions in <b>1</b> can obtain more energy from AT segments than to Er<sup>3+</sup> ions in <b>2</b>. Furthermore, the sensitization effects of AT segments to different <i>f</i>-<i>f</i> transitions of RE ions have been compared in <b>1</b> and <b>2</b>. Under the sensitization of AT segments, the <sup>4</sup>F<sub>9/2</sub>→<sup>6</sup>H<sub>15/2</sub> transition obtains the most energy compared with the <sup>4</sup>F<sub>9/2</sub>→<sup>6</sup>H<sub>13/2</sub> and <sup>4</sup>F<sub>9/2</sub>→<sup>6</sup>H<sub>11/2</sub> transitions in <b>1</b>, and the <sup>2</sup>H<sub>11/2</sub>→<sup>4</sup>I<sub>15/2</sub> transition obtains more energy than the <sup>4</sup>S<sub>3/2</sub>→<sup>4</sup>I<sub>15/2</sub> transition in <b>2</b>. It seems that the better energy level match of <sup>3</sup>T<sub>1u</sub>→<sup>1</sup>A<sub>1g</sub> transition of AT segments with <i>f</i>-<i>f</i> emission transitions of RE ions will lead to a stronger sensitization effect.

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