2017
DOI: 10.1039/c6sc01220e
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Ultrafast transient IR spectroscopy and DFT calculations of ruthenium(ii) polypyridyl complexes

Abstract: TRIR spectroscopy identifies the low-energy ligand-field state in the relaxation cascade for ruthenium(ii) polypyridyl complexes.

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Cited by 68 publications
(100 citation statements)
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“…However, in Ru II polypyridine complexes there is usually additional nonradiative relaxation from the 3 MLCT via the 3 T 1g excited state (Figure 3b) [37,38]. Depending on ligand design [39], this metal-centered state can be energetically very close and nonradiative relaxation becomes very rapid, and this is the reason why [Ru(tpy) 2 ] 2+ (tpy = 2,2 :6 ,2"-terpyridine) is essentially non-emissive in solution at room temperature [40]. Conversely, when the 3 T 1g state is located energetically sufficiently above the 3 MLCT manifold, high luminescence quantum yields and long excited state lifetimes are achievable [41].…”
Section: Resultsmentioning
confidence: 99%
“…However, in Ru II polypyridine complexes there is usually additional nonradiative relaxation from the 3 MLCT via the 3 T 1g excited state (Figure 3b) [37,38]. Depending on ligand design [39], this metal-centered state can be energetically very close and nonradiative relaxation becomes very rapid, and this is the reason why [Ru(tpy) 2 ] 2+ (tpy = 2,2 :6 ,2"-terpyridine) is essentially non-emissive in solution at room temperature [40]. Conversely, when the 3 T 1g state is located energetically sufficiently above the 3 MLCT manifold, high luminescence quantum yields and long excited state lifetimes are achievable [41].…”
Section: Resultsmentioning
confidence: 99%
“…This horizontal displacement opensu pap athway for the 3 MLCT excited-state population to cross over ac ertain barrieri nto the 3 T 1g state, and from there onwards to the 1 A 1g ground state. [4] In [Ru(tpy) 2 ] 2 + (tpy = 2,2':6',2''-terpyridine), the 3 T 1g state is markedly lower than that in [Ru(bpy) 3 ] 2 + ,a nd this is the main reason why [Ru(tpy) 2 ] 2 + is essentially nonemissive at room temperature in fluid solution, whereas [Ru(bpy) 3 ] 2 + has ad ecent luminescence quantumy ield under such conditions. [5] The lower energy of the 3 T 1g state in [Ru(tpy) 2 ] 2 + is ad irect consequence of the weaker ligand field caused by tpy,r elative to bpy,due to smaller N-Ru-N angles.…”
Section: Commonalities and Differencesi Nt He Photophysics Of Ru II Amentioning
confidence: 99%
“…For instance, in the extensively studied prototype Fe II molecule Fe II (bpy) 3 (bpy=2,2′‐bipyridine), the charge‐separated MLCT state deactivates on an ultrafast timescale into high‐spin MC states . Similar ultrafast transitions into 3 MC states have been observed and described for ruthenium sensitizer complexes . By destabilizing the MC scavenger states we, and other groups, have recently developed iron complexes with significantly slower deactivation of the MLCT states …”
Section: Introductionmentioning
confidence: 58%
“…[9,10] Similar ultrafast transitions into 3 MC states have been observed and described for ruthenium sensitizer complexes. [11][12][13] By destabilizing the MC scavenger states we,a nd other groups,h ave recently developed iron complexes with significantly slower deactivation of the MLCT states. [14][15][16][17][18][19][20][21] This makes the iron carbene complexes interesting as ap romising new class of photosensitizers, [22] with recently demonstrated capability to inject electrons efficiently into aT iO 2 substrate,a nd carry out bimolecular oxidation and reduction processes.…”
Section: Introductionmentioning
confidence: 99%