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Photochemistry and Photophysics of Coordination Compounds

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<strong>Photochemistry</strong> <strong>and</strong> <strong>Photophysics</strong> <strong>of</strong> <strong>Coordination</strong> <strong>Compounds</strong>: Copper 85<br />

Fig. 15 Schematic orbital splitting diagrams for [Cu(NN)2] + . Left, D2d symmetry; right,<br />

D2 symmetry. Grey arrows represent the transitions leading to b<strong>and</strong>s I (— —), b<strong>and</strong> II<br />

(···), <strong>and</strong> b<strong>and</strong> III (– – –)<br />

A simple picture able to rationalize the MLCT absorption patterns <strong>of</strong><br />

these complexes in solution is difficult, nevertheless some general trends have<br />

been found by analyzing the MLCT absorption maxima <strong>and</strong> molar extinction<br />

coefficients <strong>of</strong> series <strong>of</strong> [Cu(NN)2] + compounds <strong>and</strong> have been reported<br />

elsewhere [15].<br />

The spectrum <strong>of</strong> [Cu(4)2] + in Fig. 13 exhibits a well-established fingerprint<br />

for complexes with 2,9-aryl substitution <strong>of</strong> the phenanthroline ring, i.e.<br />

a pronounced low-energy shoulder extending down to 650 nm (b<strong>and</strong> I, see<br />

above), which is practically absent in the case <strong>of</strong> [Cu(1)2] + .Thispatternisrelated<br />

to the above mentioned intramolecular π-stacking interactions, which<br />

make the transition corresponding to b<strong>and</strong> I more permitted. The absorption<br />

spectrum <strong>of</strong> [Cu(5)2] + is somewhat different if compared to both [Cu(4)2] +<br />

<strong>and</strong> [Cu(1)2] + . The low energy b<strong>and</strong> is wider <strong>and</strong> more intense <strong>and</strong> the peak<br />

around 440, which is typically the most intense in [Cu(NN)2] + complexes, appears<br />

as just a weak shoulder [74]. This trend is due to the presence <strong>of</strong> the<br />

cumbersome tert-butyl groups on the phenyl residues, that limit π-π stacking<br />

interactions <strong>and</strong> make the structure <strong>of</strong> the complex particularly rigid.<br />

The MLCT absorption pr<strong>of</strong>ile <strong>of</strong> [Cu(5)2] + is found to be similar to that <strong>of</strong><br />

aCu(I)-catenate complex made <strong>of</strong> two interlocked 27-membered rings containing<br />

a phenanthroline moiety <strong>and</strong> exhibiting a very rigid coordination<br />

environment [75]. The structural peculiarity <strong>of</strong> [Cu(5)2] + , as revealed by the<br />

absorption spectrum, is in accord with its extraordinary kinetic inertness towards<br />

demetallation [74].<br />

Interestingly, it has been found that the complex [Cu(6)2] + (Fig. 14) exhibits<br />

a very weak b<strong>and</strong> above 500 nm despite the presence <strong>of</strong> phenyl rings in<br />

the 2 <strong>and</strong> 9 positions [71]. Indeed this confirms the above described model:<br />

the methyl groups in the 3 <strong>and</strong> 8 position contrast the flattening distortion,

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