Electronic energy transfer plays a crucial role in many natural processes, ranging from self-protection [1] to repair mechanisms [2] and energy transduction. [3] One of the primary reasons for employing such indirect excitation is that ideal reagents for inducing chemical change, such as electron transfer or conformational exchange, rarely possess optimal light-absorbing properties.[4] This simple strategy of equipping an elaborate photochemical device with an ancillary photon collector, programmed to absorb over a broad spectral range and to emit at a discrete wavelength, is also relevant to artificial photosynthetic systems. Indeed, such strategies may have relevance to the design of dye-sensitized solar cells [5] and certain organic light-emitting diodes.[6] Similar processes also appear relevant to conducting polymers [7] and solar concentrators.[8] A further, and possibly important, role for lightharvesting units is to promote the harmless dissipation of ultraviolet (UV) photons, arising from increased UVB radiation at the Earths surface because of stratospheric ozone depletion that would otherwise initiate photo-degradation. The latter realization has led to the recent investigation of cases where an upper-lying excited state (e.g., S 2 ) of a strongly fluorescent dye functions as the energy acceptor for high-energy photons while the lowest-energy excited state acts as sensitiser for the photonic device.[9] Complementary reports have shown that the S 2 states of certain dyes, notably carotenes [10] and metallo-porphyrins, [11] can be used as energy donors.In terms of protective mechanisms and device efficacy, it is essential that the S 2 state formed through energy transfer undergoes rapid electronic relaxation (i.e., internal conversion) to the corresponding S 1 state, without opening new routes for deleterious or antagonistic chemical steps. Although the S 2 states of most organic molecules tend to be very short-lived, there are notable exceptions [12] and few rules other than the generic Englman-Jortner energy-gap law [13] by which to predict their lifetimes. Even less is understood about how the internal conversion dynamics depend on the molecular structure and the local environment. We now report on internal conversion in two boron dipyrromethene dyes for which the meso-phenyl ring is either constrained (Bodipy) or free to rotate (Robod), the latter class of dye being popular rheology probes. [14] Our particular interest lies with understanding the effect of nuclear motion on the ultrafast dynamics of upper-lying excited states. Earlier work has concluded that deactivation of the higher-lying (i.e., S 3 and/or S 2 ) excited states and the simultaneous population of the S 1 states of such dyes occur on timescales of a few hundreds of femtoseconds while vibrational cooling of the S 1 state occurs over approximately 20 ps. [15] The two dyes, Robod and Bodipy (Scheme 1), differ by virtue of the substitution pattern at the pyrrole units. This structural change has an important effect on the photophysical p...