Arabidopsis ͉ LHCII ͉ NPQ ͉ two-photon excitation P lants are exposed to sunlight intensities varying over several orders of magnitude during a typical day (1). Under low light conditions, almost all absorbed sunlight photons are used for the primary photosynthetic reaction steps. However, under high light conditions the photosynthetic apparatus must be protected from excess excitation energy, because it may lead to deleterious side-effects. Balancing between efficient utilization of solar energy under restrictive light conditions and dissipation of excess energy when the absorbed light exceeds the photosynthetic capacity is therefore essential for the survival and fitness of plants (2). It is known that light-induced increase of the pH gradient across the thylakoid membrane (3, 4) and the presence of the protein PsbS (5) are necessary for the down-regulation of the photosynthetic activity under excess light and that Zea is simultaneously formed from violaxanthin (Vio) through the enzymatic xanthophyll cycle (6). However, although many different studies have been undertaken to elucidate the details of this important regulation, a complete picture of its mechanisms is still missing. Several different regulation models have been proposed and indeed it cannot be excluded that different mechanisms contribute more or less to plants adaptation to varying light conditions. However, at present even the regulation site and photophysical mechanisms are unresolved, because the models are at least partly contradicting each other (5, 7-15).The most important measurable signature of plants regulation activity is its varying residual Chl fluorescence intensity (16), which is proportional to the regulated amount of excitation energy in the photosynthetic apparatus. The actual extent of adaptation-dependent quenching of Chl singlet excited state energy, known as nonphotochemical quenching (NPQ), is typically quantified by the parameterwhich reflects the reduction in the residual Chl fluorescence of plants, FЈ m , brought about by the unknown excitation energy dissipation mechanisms, in comparison to the residual Chl fluorescence observable from the completely dark adapted plant, F m , in which no photoprotective energy dissipation is operating. FЈ m and F m are usually measured using short, intense light flashes that saturate the photosynthetic reaction center chemistry. This guarantees that the observed differences in FЈ m and F m reflect only the extent of energy dissipation through photoprotective channels, without affecting the adaptation status of the plant (16). It is long known that carotenoids play an important role in the regulation mechanisms and several different types of electronic interactions between carotenoids and Chls have been proposed to play a key role as dissipation valves for excess excitation energy (9, 10, 12). However, so far it was difficult to quantify the extent of these interactions and to investigate directly their involvement in the flow of excitation energy and its regulation, especially in living...

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The low-temperature fabrication of flexible ZnO photo-anodes for dye-sensitized solar cells (DSSCs) by templated electrochemical deposition of films was performed in an enlarged and technical simplified deposition setup to demonstrate the feasibility of the scale-up of the deposition process. After extraction of eosin Y (EY) from the initially deposited ZnO/EY hybrid films, mesoporous ZnO films with an area of about 40 cm2 were reproducibly obtained on fluorine doped tin oxide (FTO)-glass as well as flexible indium tin oxide (ITO)–polyethylenterephthalate (PET) substrates. With a film thickness of up to 9 µm and a high specific surface area of up to about 77 m2·cm−3 the ZnO films on the flexible substrates show suitable properties for DSSCs. Operative flexible DSSC modules proved the suitability of the ZnO films for use as DSSC photo-anodes. Under a low light intensity of about 0.007 sun these modules achieved decent performance parameters with conversion efficiencies of up to 2.58%. With rising light intensity the performance parameters deteriorated, leading to conversion efficiencies below 1% at light intensities above 0.5 sun. The poor performance of the modules under high light intensities can be attributed to their high series resistances.