“…The efficient intersystem crossing produces a high population of the excited triplet state. Because the triplet−triplet transient absorption cross sections are higher than the ground-state absorption cross sections, , C 60 in room-temperature solution exhibits excellent nonlinear absorptive optical limiting properties. − In fact, C 60 is actively investigated as one of the best broad-band optical limiters for potential laser power limiting and optical switching applications. , Similar excited-state properties have been observed for C 60 derivatives. − ,,,− For example, it has been shown that the excited-state properties of different methano-C 60 and pyrrolidino-C 60 derivatives are rather similar. ,,,, The derivatives are more fluorescent than the parent C 60 , with fluorescence yields of the derivatives being larger by approximately a factor of 3 and fluorescence lifetimes being longer by approximately 25% (1.4−1.6 ns for the derivatives vs 1.2 ns for C 60 ). , The intersystem crossing continues to be the dominating excited-singlet-state decay pathway in the C 60 derivatives, again with unity intersystem yields according to results from singlet molecular oxygen generation measurements. ,, The triplet−triplet transient absorption spectra of the C 60 derivatives have spectral profiles similar to that of the parent C 60 , but the spectra of the derivatives are slightly blue-shifted and have lower absorption cross sections. ,, However, the nonlinear absorptive properties of the C 60 derivatives as measured by optical limiting responses toward a nanosecond pulsed laser at 532 nm are only marginally different from those of the parent C 60 in room-temperature solutions. ,− …”