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Dark- and Photoexcited-State Electronic Structures of [Ru(SO<sub>2</sub>)(NH<sub>3</sub>)<sub>4</sub>X]Y Complexes and Their Relation to SO<sub>2</sub> Photoconversion Efficiency

Listed in figshare and Loughborough Research Repository — shown once because both records carry DOI 10.1021/acs.jpclett.6c02623.s001

Single crystals of the [Ru(SO<sub>2</sub>)(NH<sub>3</sub>)<sub>4</sub>X]Y family of complexes are promising photoswitches or photoactuators; they respond structurally to visible light, undergoing SO<sub>2</sub> linkage photoisomerization with high spatiotemporal precision.

Description

However, the SO<sub>2</sub> photoconversion efficiency (PCE) varies markedly with the <i>trans</i>-ligand X and no unifying molecular design principle is yet available.

This study addresses this knowledge gap by performing electronic-structure calculations on 11 respective crystal structures of these complexes using reference crystal structures characterized by single-crystal X-ray diffraction under light irradiation. We focus on 4 structural archetypes of [Ru(SO<sub>2</sub>)(NH<sub>3</sub>)<sub>4</sub>X][tosylate]<sub>2</sub>, where X = H<sub>2</sub>O (<b>1</b>), 3-F-pyridine (<b>2</b>), 3-Cl-pyridine (<b>3</b>), and 3-Br-pyridine (<b>4</b>), to elucidate how the <i>trans</i>-ligands control the Ru-centered electronic rearrangement upon photoexcitation.

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The dark-state projected densities of states of these crystal structures are qualitatively similar across the series, exhibiting [Ru]-S π-bonding and [Ru]-X π/σ interactions. By contrast, electronic-structure calculations using time-dependent density functional theory reveal distinct photoexcited-state behavior: in <b>1</b>, photoexcitation populates an antibonding <i>d</i><sub><i>yz</i></sub>-<i>p</i><sub><i>y</i></sub> orbital, weakening the [Ru]-S bond and lowering the SO<sub>2</sub> photoisomerization barrier; in <b>2</b>−<b>4</b>, photoexcitation simultaneously populates this antibonding orbital and depopulates its bonding counterpart, weakening the [Ru]-S bond substantially more to afford a correspondingly higher PCE than in <b>1</b>.

Response charge-density analyses visualize the corresponding photoinduced charge redistribution in real space, consistent with the finer ordering of the PCE: <b>3</b> < <b>2</b> < <b>4</b>. We additionally propose the Ru <i>d</i>-band center as a descriptor for PCE: within a common class of <i>trans</i>-ligand, the PCE tends to decrease as the <i>d</i>-band center shifts toward the Fermi level, as shown here for ten pyridyl-ligated structures, although other factors also contribute to the photoisomerization process.

Together, these results provide a mechanistic account of photoexcited-state changes in the electronic structure of [Ru(SO<sub>2</sub>)(NH<sub>3</sub>)<sub>4</sub>X]Y complexes and suggest a practical screening metric for the rational molecular design of this family of high-PCE photoresponsive single crystals for quantum photosensing applications.

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Density functional theory 75%
Provenance · 2 source records, 34 field assertions
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figshareoai:figshare.com:article/3399092612 d agoJSON v1
Loughborough Research Repositoryoai:figshare.com:article/3399092611 d agoJSON v1
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