Jürgen Baier, Max Maier, Roland Engl, Michael Landthaler, and Wolfgang Bäumler
(J. Baier, M. Maier, R. Engl, M. Landthaler, and W. Bäumler)

Journal of Physical Chemistry B, 2005, Volume 109, Issue 7, Page 3041-3046
(J. Phys. Chem. B 2005, 109 (7), 3041-3046)

doi: 10.1021/jp0455531

Abstract:
Singlet oxygen was generated by energy transfer from the photoexcited sensitizer, Photofrin or 9-acetoxy-2,7,12,17-tetrakis-(beta-methoxyethyl)-porphycene (ATMPn), to molecular oxygen. Singlet oxygen was detected time-resolved by its luminescence at 1270 nm in an environment of increasing complexity, water (H2O), pure phosphatidylcholine, phosphatidylcholine in water (lipid suspensions), and aqueous suspensions of living cells. In the case of the lipid suspensions, the sensitizers accumulated in the lipids, whereas the localizations in the cells are the membranes containing phosphatidylcholine. By use of Photofrin, the measured luminescence decay times of singlet oxygen were 3.5 ± 0.5 µs in water, 14 ± 2 µs in lipid, 9 ± 2 µs in aqueous suspensions of lipid droplets, and 10 ± 3 µs in aqueous suspensions of human colonic cancer cells (HT29). The decay time in cell suspensions was much longer than in water and was comparable to the value in suspensions of phosphatidylcholine. That luminescence signal might be attributed to singlet oxygen decaying in the lipid areas of cellular membranes. The measured luminescence decay times of singlet oxygen excited by ATMPn in pure lipid and lipid suspensions were the same within the experimental error as for Photofrin. In contrast to experiments with Photofrin, the decay time in aqueous suspension of HT29 cells was 6 ± 2 µs when using ATMPn.

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