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Triplet-triplet energy transfer controlled by the donor-acceptor distance in rigidly held palladium-containing cofacial bisporphyrins

机译:三重态-三重态能量传递受刚性持有的含钯界面双卟啉中供体-受体距离的控制

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摘要

Eleven new complexes, including mono-, heterobi-, and homobimetallic cofacial bisporphyrins, (Pd)H2DPS, (M)H2DPX, (M)H2DPB, (PdZn)DPS, (PdZn)DPX, (Pt)(2)DPX, (M)(2)DPB (M=Pd, Pt), and (Pt)P (DPS4- = 4,6-bis[5-(2,8,13,17-tetraethyl-3,7,12,18-tetramethylporphyrinyl)]di- benzothiophene tetraanion, DPX4-= 4,5-bis[5-(2,8,13,17-tetraethyl-3,7,12,18-tetramethylporphlrinvl)]-9,9-dimethyl-xanthene tetraanion, DPB4- = 1,8-bis[5(2,8,13,17-tetraethyl-3,7,12,18-tetrame- thylporphyrinyl)]biphenylene tetraanion, P2-=5-phenyl-2,8,13,17-tetraethvl-3,7,12,18-tetramethylporphyin dianion) have been synthesized and characterized. The photophysical properties of the donor (M)P (M=Pd or Pt, P= porphyrin chromophore) and the acceptor (free base H2P or (Zn)P) depend on the C-meso - C-meso distance and the presence of a heavy atom such as Pd-II or Pt-II. The data were compared with those for the known compounds (Pd)(2)DPS, (Pd)(2)DPX, H4DPS, H4DPX, H4DPB, (Pd)P, (Zn)P, and H2P The rate constants for triplet-triplet energy transfer (k(ET)) were measured for the heterobimetallic (PdZn) and monometallic [(M)H-2] derivatives (M=Pd, Pt). The fluorescence lifetimes (Delta tau(F)) of the acceptors decrease as a result of the heavy-atom effect, and vary as follows: (Pd)H2DPS < (Pd)H2DPX-(Pd)H2DPB. The k(ET) values calculated according to the equation k(ET) = (1/tau(emi) - 1/tau(emi)(0)), where tau(emi)(0) is the emission lifetime of the homobimetallic bisporphyrins (no ET occurs), are equal to 0, 247 +/- 57 and 133 +/- 52 s(-1) for DPS, DPX, and DPB, respectively, in the (Pd)H-2 series. These measurements allowed the range of distance over which the Dexter mechanism for T-1-T-1 energy transfer ceases to operate to be determined. This distance is somewhere between 4.3 and 6.3 A, in agreement with our recent findings on singlet-singlet energy transfer. During the course of this study, the X-ray crystal structure for (Pd)H,DPX was obtained; triclinic (P1), a = 11.1016(1), b = 14.9868(2), c = 20.6786(3) A, alpha = 102.091(1), beta =100.587(1), gamma 101.817(1)degrees, V = 3199.19(7) A(3), Z = 2.
机译:十一种新的配合物,包括单金属,杂双金属和同金属双界面双卟啉,(Pd)H2DPS,(M)H2DPX,(M)H2DPB,(PdZn)DPS,(PdZn)DPX,(Pt)(2)DPX,( M)(2)DPB(M = Pd,Pt)和(Pt)P(DPS4- = 4,6-双[5-(2,8,13,17-四乙基-3,7,12,18-四甲基卟啉基)]-二苯并噻吩四阴离子,DPX4- = 4,5-双[5-(2,8,13,17-四乙基-3,7,12,18-四甲基卟啉 lrinvl)]-9,9-二甲基- an吨四阴离子,DPB4- = 1,8-双[5(2,8,13,17-四乙基-3,7,12,18-四甲基卟啉基)]联苯四阴离子,P2- = 5-苯基-2,8 (13,17-tetraethvl-3,7,12,18-tetramethylporphyin dianion)已经合成并表征。供体(M)P(M = Pd或Pt,P =卟啉发色团)和受体(游离碱H2P或(Zn)P)的光物理性质取决于C-meso-C-meso距离和重原子,例如Pd-II或Pt-II。将该数据与已知化合物(Pd)(2)DPS,(Pd)(2)DPX,H4DPS,H4DPX,H4DPB,(Pd)P,(Zn)P和H2P的数据进行比较。测量了异双金属(PdZn)和单金属[(M)H-2]衍生物(M = Pd,Pt)的三重态能量转移(k(ET))。由于重原子效应,受体的荧光寿命(Delta tau(F))减少,并且变化如下:(Pd)H2DPS <(Pd)H2DPX-(Pd)H2DPB。根据方程式k(ET)=(1 / tau(emi)-1 / tau(emi)(0))计算的k(ET)值,其中tau(emi)(0)是同双金属的发射寿命(Pd)H-2系列中的DPS,DPX和DPB的双卟啉(无ET发生)分别等于0、247 +/- 57和133 +/- 52 s(-1)。这些测量结果确定了用于T-1-T-1能量转移的Dexter机构停止工作的距离范围。这个距离在4.3和6.3 A之间,这与我们最近关于单重态-单重态能量转移的发现一致。在研究过程中,获得了(Pd)H,DPX的X射线晶体结构。三斜晶(P1),a = 11.1016(1),b = 14.9868(2),c = 20.6786(3)A,alpha = 102.091(1),beta = 100.587(1),伽马101.817(1)度,V = 3199.19(7)A(3),Z = 2

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