TY - JOUR
T1 - Ligand-field excited states of hexacyanochromate and hexacyanocobaltate as sensitisers for near-infrared luminescence from Nd(III) and Yb(III) in cyanide-bridged d-f assemblies
AU - Lazarides, Theodore
AU - Davies, Graham M.
AU - Adams, Harry
AU - Sabatini, Cristiana
AU - Barigelletti, Francesco
AU - Barbieri, Andrea
AU - Pope, Simon J A
AU - Faulkner, Stephen
AU - Ward, Michael D.
PY - 2007
Y1 - 2007
N2 - Crystallisation of [Co(CN)6]3- or [Cr(CN) 6]3- with Ln(iii) salts (Ln = Nd, Gd, Yb) from aqueous dmf afforded the cyanide-bridged d/f systems [Ln(dmf)4(H 2O)3(μ-CN)Co(CN)5] (Co-Ln, discrete dinuclear species) and {[Cr(CN)4(μ-CN)2Ln(H 2O)2(dmf)4]}∞ (Cr-Ln, infinite cyanide-bridged chains with alternating Cr and Ln centres). With Ln = Gd the characteristic long-lived phosphorescence from d-d excited states of the [M(CN)6]3- units was apparent in the red region of the spectrum, with lifetimes of the order of 1 μs, since the heavy atom effect of the Gd(iii) promotes inter-system crossing at the [M(CN)6] 3- units to generate the phosphorescent spin-forbidden excited states. With Ln = Yb or Nd however, the d-block luminescence was completely quenched due to fast (>108 s-1) energy-transfer to the Ln(iii) centre, resulting in the characteristic sensitised emission from Yb(iii) and Nd(iii) in the near-IR region. For both Co-Nd and Co-Yb, calculations based on spectroscopic overlap between emission of the donor (Co) and absorption of the acceptor (Ln) suggest that the Dexter energy-transfer mechanism is responsible for the complete quenching that we observe. © The Royal Society of Chemistry and Owner Societies.
AB - Crystallisation of [Co(CN)6]3- or [Cr(CN) 6]3- with Ln(iii) salts (Ln = Nd, Gd, Yb) from aqueous dmf afforded the cyanide-bridged d/f systems [Ln(dmf)4(H 2O)3(μ-CN)Co(CN)5] (Co-Ln, discrete dinuclear species) and {[Cr(CN)4(μ-CN)2Ln(H 2O)2(dmf)4]}∞ (Cr-Ln, infinite cyanide-bridged chains with alternating Cr and Ln centres). With Ln = Gd the characteristic long-lived phosphorescence from d-d excited states of the [M(CN)6]3- units was apparent in the red region of the spectrum, with lifetimes of the order of 1 μs, since the heavy atom effect of the Gd(iii) promotes inter-system crossing at the [M(CN)6] 3- units to generate the phosphorescent spin-forbidden excited states. With Ln = Yb or Nd however, the d-block luminescence was completely quenched due to fast (>108 s-1) energy-transfer to the Ln(iii) centre, resulting in the characteristic sensitised emission from Yb(iii) and Nd(iii) in the near-IR region. For both Co-Nd and Co-Yb, calculations based on spectroscopic overlap between emission of the donor (Co) and absorption of the acceptor (Ln) suggest that the Dexter energy-transfer mechanism is responsible for the complete quenching that we observe. © The Royal Society of Chemistry and Owner Societies.
M3 - Article
SN - 1474-9092
VL - 6
SP - 1152
EP - 1157
JO - Photochemical and Photobiological Sciences
JF - Photochemical and Photobiological Sciences
IS - 11
ER -