This investigation was motivated by a desire to get a deeper insight into the mechanism of carotenoiod-to-bacteriochlorophyll (Car-to-BChl) energy transfer proceeding via the carotenoid S1 state. (Here, we call the 2Ag - and 1Bu + states “the S1 and S2 states” according to the notation presently accepted.) To systematically examine the effect of the conjugation length of carotenoid on the rate and efficiency of the Car(S1)-to-BChl(Qy) energy transfer, we performed the following experiments. (1) Subpicosecond time-resolved absorption spectroscopy was employed to measure the S1-state lifetimes of lycopene (number of conjugated CC bonds, n = 11), spheroidene (n = 10), and neurosporene (n = 9), both free in n-hexane and bound to the LH2 complexes from Rhodospirillum molischianum (Rs. molischianum), Rhodobactor sphaeroides (Rb. sphaeroides) 2.4.1, and Rb. sphaeroides G1C, respectively. The lifetime of each free (bound) carotenoid was determined to be 4.7(3.4) ps for lycopene, 9.3(1.7) ps for spheroidene, and 21.2(1.3) ps for neurosporene. It was found that the rate and the efficiency of the Car(S1)-to-BChl(Qy) energy transfer increase systematically when the number of conjugated CC bonds decreases. (2) High-sensitivity steady-state fluorescence spectroscopy was used to measure the spectra of dual emission from the S2 and S1 states for the above carotenoids dissolved in n-hexane. The fluorescence data, combined with the above kinetic data, allowed us to evaluate the magnitudes of the transition-dipole moments associated with the Car(S1) emission. It was found that the S1 emissions of the above carotenoids carry noticeably large oscillator strengths (transition-dipole moments). In the case of the LH2 complex from Rs. molischianum, whose structural information is now available, the time constant of the Car(S1)-to-BChl(Qy) energy transfer (18.6 ps), which was predicted on the basis of a Car(S2)-to-BChl(Qy) full Coulombic coupling scaled by the ratio of the S1 vs S2 transition dipole moments, was in good agreement with the one spectroscopically determined (12.3 ps). The oscillator strength associated with the Car(S1) emission was discussed in terms of the state mixing between the carotenoid S2 and S1 states.

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This minireview article highlights the energetics and the dynamics of the 1(1)B(u)(-) and 3(1)A(g)(-) states of carotenoids discovered very recently. Those "hidden" covalent states have been revealed by measurements of resonance-Raman excitation profiles of crystalline carotenoids. The dependence of the energies of the low-lying singlet states, including the 1(1)B(u)(+), 3(1)A(g)(-), 1(1)B(u)(-), and 2(1)A(g)(-) states, on the number of conjugated double bonds (n) is in agreement with the extrapolation of those state energies calculated by Tavan and Schulten for shorter polyenes (P. Tavan and K. Schulten, Journal of Chemical Physics, 1986, vol. 85, pp. 6602-6609). It has also been shown that the internal-conversion processes among those singlet states take place in accord with the state ordering, i.e., 1(1)B(u)(+) --> 1(1)B(u)(-) --> 2(1)A(g)(-) --> 1(1)A(g)(-) (the ground state) for carotenoids having n = 9 and 10, whereas 1(1)B(u)(+) --> 3(1)A(g)(-) --> 1(1)B(u) (-) --> 2(1)A(g)(-) --> 1(1)A(g)(-) for carotenoids having n = 11-13. Radiative transitions of 1(1)B(u)(+) --> 2(1)A(g)(-) and 1(1)B(u)(-) --> 2(1)A(g)(-) as well as a branching into the triplet manifold of 1(1)B(u)(-) --> 1(3)A(g) --> 1(3)B(u) have also been found. Those low-lying singlet states of all-trans carotenoids can facilitate multiple channels of singlet-energy transfer to bacteriochlorophyll in the LH2 antenna complexes of purple photosynthetic bacteria. Thus, the newly found 1(1)B(u)(-) and 3(1)A(g)(-) states of carotenoids need to be incorporated into the picture of carotenoid-to-bacteriochlorophyll singlet-energy transfer.

Fluorescence spectra of all-trans-anhydrorhodovibrin and spirilloxanthin having the number of conjugated double bonds n ) 12 and 13 were recorded in n-hexane solution. The optically forbidden 2A gf 1A gfluorescence was observed for carotenoids having such a long conjugated chain, and the optically forbidden 1B uf 1A gfluorescence was identified for the first time. The proposed energies of the 2A g -, 1B u -, and 1B u + fluorescence origins are 12 500, 14 900, and 19 200 cm -1 for anhydrorhodovibrin and 11 900, 13 600, and 18 900 cm -1 for spirilloxanthin (at 295 K). The estimated transition dipole moments for fluorescence from the 2A g -, 1B u -, and 1B u + states to the ground 1A gstate are 1.24, 4.76, and 17.4 D for the former and 1.37, 3.72, and 16.8 D for the latter.