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 S-1 state. (Here, we call the 2A(g)(-) and 1B(u)(+) states "the S-1 and S-2 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(S-1)-to-BChl(Q(y)) energy transfer, we performed the following experiments. (1) Subpicosecond time-resolved absorption spectroscopy was employed to measure the S-1-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(Q(y),) 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 S-2 and S-1 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(S-1) emission. It was found that the S-1 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(Q(y)) energy transfer (18.6 ps), which was predicted on the basis of a Car(S-1)-to-BChl(Q(y)) full Coulombic coupling scaled by the ratio of the S1 vs St 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 S-2 and S-1 states.