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1.1 Porphyrins - Friedrich-Alexander-Universität Erlangen-Nürnberg

1.1 Porphyrins - Friedrich-Alexander-Universität Erlangen-Nürnberg

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OD<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

230 K<br />

500 600 λ [nm] 700<br />

fluorescence<br />

3·10 4<br />

2·10 4<br />

1·10 4<br />

0<br />

295 K<br />

295 K<br />

Discussion and Results 3<br />

The origin of those three components was clarified taking into account the following facts:<br />

• 53 appears “chemically pure”, meaning at least >98 % purity bsd. on analytic means<br />

• component C is only detectable as it has a quite different fluorescence life-time and<br />

as the fluorescence of the major components is a priori low<br />

• regular metallo-porphyrins like Zn(II)-53 (which will be discussed later) only show one<br />

major fluorophore<br />

• variations in concentration (e.g. high dilution) do not change the ratio P(A) : P(B)<br />

Thus, C could be assigned an impurity – maybe free base TTBPP 19 or any other synthetic<br />

residue. Concerning A and B, it seemed to be clear, that they could not be monomer and<br />

dimer or any other aggregate and that it has to be a specific feature of free base compound<br />

53. One possible explanation could be the presence of distinct tautomeric structures with<br />

differing photophysical properties, like the already presented VT-NMR studies hinted to.<br />

3.2.3.4.2 Fluorescence Spectroscopy at Varied Temperatures 108<br />

To verify the abovementioned assumption, temperature dependent absorption and<br />

fluorescence spectra were recorded in solution. Changing the temperature should thereby<br />

have a significant effect onto the equilibrium position between both tautomeric structures<br />

resulting in varying shapes in both spectra. Some results are depicted in Figure 22.<br />

290 K<br />

230 K<br />

290 K<br />

225 K<br />

660 720 λ [nm]<br />

Figure 22. Temperature dependent absorption spectra (left) and fluorescence spectra (right,<br />

excitation at 532 nm) of 53.<br />

From those findings, several conclusions can be deduced. The ratio 𝑟 �� of tautomers<br />

P(A):P(B) is temperature dependent whereas at lower temperatures, one tautomer (e.g.<br />

tautomer A) becomes more predominant. A quantitative evaluation can then be achieved by<br />

780<br />

55

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