1997
DOI: 10.1021/jp962394f
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Weak Temperature Dependence in the Magnetic Circular Dichroism of Matrix-Isolated Copper Phthalocyanine

Abstract: Weak temperature dependence is reported for the Q-band magnetic circular dichroism of Cu phthalocyanine in an Ar matrix between 15 and 1.5 K. Moment analysis reveals a zero-field splitting of 1.5 ± 0.5 cm-1 in the singdoublet Q state. This is interpreted to be a consequence of interference between spin−orbit coupling and exchange interactions with the tripdoublet state.

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Cited by 11 publications
(23 citation statements)
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“…However, this physically implausible state is higher in energy than the depicted configuration, both because the d x 2 −y 2 orbital is less stable than the ligand HOMO and because it is harder to pair electrons within the more compact metal-centred orbital. This analysis is supported by previous experimental [77,78,79,80,81] and computational [82,77,78,83,18,79,84] studies that agree on the ground state configuration shown in Figure 2.…”
Section: Nipc Cupc Znpcsupporting
confidence: 86%
“…However, this physically implausible state is higher in energy than the depicted configuration, both because the d x 2 −y 2 orbital is less stable than the ligand HOMO and because it is harder to pair electrons within the more compact metal-centred orbital. This analysis is supported by previous experimental [77,78,79,80,81] and computational [82,77,78,83,18,79,84] studies that agree on the ground state configuration shown in Figure 2.…”
Section: Nipc Cupc Znpcsupporting
confidence: 86%
“…54 In contrast to all of the previous examples considered here, even at very low temperatures the MCD of the Q-band is only very weakly temperature dependent. 54 In contrast to all of the previous examples considered here, even at very low temperatures the MCD of the Q-band is only very weakly temperature dependent.…”
Section: Cu Phthalocyaninecontrasting
confidence: 62%
“…54 In contrast to all of the previous examples considered here, even at very low temperatures the MCD of the Q-band is only very weakly temperature dependent. 54 The experimental and simulated spectra of CuPhth are presented in Fig. 54 From an analysis of the temperature dependence of the MCD intensity for this state is found to be 1.5 cm −1 .…”
Section: Cu Phthalocyaninecontrasting
confidence: 62%
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“…Q 00 at 736 nm corresponds to the a 1 u ( π ) → e g ( π * ) transition at the HOMO-LUMO gap and is polarized in the plane of the molecule. Q 10 at 696 nm is the contribution of vibrational overtones and Q 20 located at 658 nm can be assigned as a transition from lower lying σ states in the valence band manifold ( e u ( σ ) → e g ( π * )), polarized perpendicular to the molecular plane and vibronically coupled to Q 00 43 . Absorption spectrum of the Cu-OBPc thin films is significantly broadened compared to that of the solution due to the Davydov splitting and excitonic coupling in the crystalline phase that leads to more complex band structure 39 44 .…”
Section: Resultsmentioning
confidence: 99%