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| Content Provider | World Health Organization (WHO)-Global Index Medicus |
|---|---|
| Author | Law, Yuen-chi Kui, Steven C. F. Zhu, Nianyong Phillips, David Lee Che, Chi-ming Tong, Glenna So Ming Leung, King Hong |
| Description | Author Affiliation: Tong GS ( Department of Chemistry, Institute of Molecular Functional Materials and HKU-CAS Joint Laboratory on New Materials, The University of Hong Kong, Pokfulam, Hong Kong SAR, China.) |
| Abstract | The complexes $[Pt(tBu_{3}tpy)\{CC(C_{6}H_{4}CC)_{n−1}R\}]^{+}$ (n=1: R=alkyl and aryl (Ar); n=1–3: R=phenyl (Ph) or $Ph-N(CH_{3})_{2}-4;$ n=1 and 2, $R=Ph-NH_{2}-4;$ $tBu_{3}tpy=4,4`,4``-tri-tert-butyl-2,2`:6`,2``-terpyridine)$ and $[Pt(Cl_{3}tpy)(CCR)]^{+}$ (R=tert-butyl (tBu), Ph, 9,9’-dibutylfluorene, 9,9’-dibutyl-7-dimethyl-amine-fluorene; $Cl_{3}tpy=4,4`,4``-trichloro-2,2`:6`,2``-terpyridine)$ were prepared. The effects of substituent(s) on the terpyridine (tpy) and acetylide ligands and chain length of arylacetylide ligands on the absorption and emission spectra were examined. Resonance Raman (RR) spectra of $[Pt(tBu_{3}tpy)(CCR)]^{+}$ (R=n-butyl, Ph, and $C_{6}H_{4}-OCH_{3}-4)$ obtained in acetonitrile at 298 K reveal that the structural distortion of the CC bond in the electronic excited state obtained by 502.9 nm excitation is substantially larger than that obtained by 416 nm excitation. Density functional theory (DFT) and time-dependent DFT (TDDFT) calculations on $[Pt(H_{3}tpy)(CCR)]^{+}$ (R= n-propyl (nPr), 2-pyridyl (Py)), $[Pt(H_{3}tpy)\{CC(C_{6}H_{4}CC)_{n−1}Ph\}]^{+}$ (n=1–3), and $[Pt(H_{3}tpy)\{CC(C_{6}H_{4}CC)_{n−1}C_{6}H_{4}-N(CH_{3})_{2}-4\}]^{+}/+H^{+}$ (n=1–3; $H_{3}tpy=nonsubstituted$ terpyridine) at two different conformations were performed, namely, with the phenyl rings of the arylacetylide ligands coplanar (“cop”) with and perpendicular (“per”) to the $H_{3}tpy$ ligand. Combining the experimental data and calculated results, the two lowest energy absorption peak maxima, $λ_{1}$ and $λ_{2},$ of $[Pt(Y_{3}tpy)(CCR)]^{+}$ (Y=tBu or Cl, R=aryl) are attributed to $^{1}[π(CCR)→π*(Y_{3}tpy)]$ in the “cop” conformation and mixed $^{1}[d_{π}(Pt)→π*(Y_{3}tpy)]/^{1}[π(CCR)→π*(Y_{3}tpy)]$ transitions in the “per” conformation. The lowest energy absorption peak $λ_{1}$ for $[Pt(tBu_{3}tpy)\{CC(C_{6}H_{4}CC)_{n−1}C_{6}H_{4}-H-4\}]^{+}$ (n=1–3) shows a redshift with increasing chain length. However, for $[Pt(tBu_{3}tpy)\{CC(C6H4CC)_{n−1}C_{6}H_{4}-N(CH_{3})_{2}-4\}]^{+}$ (n=1–3), $λ_{1}$ shows a blueshift with increasing chain length n, but shows a redshift after the addition of acid. The emissions of $[Pt(Y_{3}tpy)(CCR)]^{+}$ (Y=tBu or Cl) at 524–642 nm measured in dichloromethane at 298 K are assigned to the $^{3}[π(CCAr)→π*(Y_{3}tpy)]$ excited states and mixed $^{3}[d_{π}(Pt)→π*(Y_{3}tpy)]/^{3}[π(CC)→π*(Y_{3}tpy)]$ excited states for R=aryl and alkyl groups, respectively. $[Pt(tBu_{3}tpy)\{CC(C_{6}H_{4}CC)_{n−1}C_{6}H_{4}-N(CH_{3})_{2}-4\}]^{+}$ (n=1 and 2) are nonemissive, and this is attributed to the small energy gap between the singlet ground state $(S_{0})$ and the lowest triplet excited state $(T_{1}).$ |
| ISSN | 09476539 |
| e-ISSN | 15213765 |
| Journal | Chemistry - A European Journal |
| Issue Number | 22 |
| Volume Number | 16 |
| Language | English |
| Publisher | Wiley-VCH;ChemPubSoc Europe |
| Publisher Date | 2010-06-11 |
| Publisher Place | Germany |
| Access Restriction | Open |
| Subject Keyword | Chemistry |
| Content Type | Text |
| Resource Type | Article |
| Subject | Organic Chemistry Catalysis |
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