1992
DOI: 10.1021/j100201a028
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Localized orbital study on the electronic structure of phthalocyanine dimers

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Cited by 110 publications
(111 citation statements)
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“…12,13 The close proximity of the two rings (2.8 Å for lutetium) gives rise to delocalized charge distributions and results in strong CT coupling due to significant wavefunction overlap. 14 The resulting high degree of charge carrier mobility readily explains their semiconductivity 15,16 and electrochromic behavior. 17,18 In its electronic ground state, lutetium bisphthalocyanine ([LuPc 2 ]) is a stable radical ([LuPc 2 ]…”
Section: Introductionmentioning
confidence: 99%
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“…12,13 The close proximity of the two rings (2.8 Å for lutetium) gives rise to delocalized charge distributions and results in strong CT coupling due to significant wavefunction overlap. 14 The resulting high degree of charge carrier mobility readily explains their semiconductivity 15,16 and electrochromic behavior. 17,18 In its electronic ground state, lutetium bisphthalocyanine ([LuPc 2 ]) is a stable radical ([LuPc 2 ]…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, the anion ([LuPc 2 ] − ) exhibits CT states in the same energy range as the LE states. 14 The additional CT coupling drastically changes the electronic structure and gives rise to two bands in the linear absorption spectrum (Fig. 1).…”
Section: Introductionmentioning
confidence: 99%
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“…The amplitude of cp2 rises on a 30 fs timescale, while the amplitude of cp1 shows a delayed rise. Neither the double peak structure of the low energy band nor the distinct cross-peak dynamics are predicted by the exciton model previously used to describe [LuPc 2 ]  [3]. To find the origin of these additional transitions, we investigated the influence of the counter-ion on the electronic structure by TD-DFT calculations [4].…”
Section: Resultsmentioning
confidence: 99%
“…In the neutral form, the single transition in the linear absorption spectrum can be understood as a transition to the upper state in an H-type dimer formed by resonance coupling between the LEs on each of the rings. For the anion, configuration interaction between inter-ring CTand LE-states yields a double peak structure in the linear absorption spectrum [3]. For a symmetric complex, each transition is two-(anion) or four-fold (radical) degenerate.…”
Section: Introductionmentioning
confidence: 99%