Dedicated to the memory of Darshan RanganathanExcitation energy transfer within and between molecular systems plays an important role in natural processes, such as photosynthesis. In this context, there has been widespread interest in mimicking the mechanism of solar-energy harvesting of natural photosynthesis with the aid of synthetic molecular systems. Apart from this, photoinduced energy transfer has become significant in the area of photovoltaics, organic light-emitting diodes, fluorescent labeling, and in a variety of photonic devices. In most of these cases, energy transfer is considerably influenced by the supramolecular ordering and spatial relationship of the donor and acceptor chromophores. Molecular architectures such as hydrogen-bonded systems, [1] dendrimers, [2] chromophore-linked polymers, [3] Langmuir±Blodgett films, [4] and self-assembled monolayers [5] are of extremely important in this context. Among a plethora of donor±acceptor systems investigated, energy and electron transfer from oligo(phenylenevinylene)s (OPVs) and poly(phenylenevinylene)s (PPVs) to acceptors, such as C 60 , [6] phenanthroline, [7] and doped organic dyes [8] have generated enormous interest because of their potential use in photovoltaic and light-emitting devices. From this view point, the recent reports by Meijer and coworkers on energy and electron transfer from OPV-functionalized dendrimers and supramolecular assemblies to various acceptors are of particular interest. [9] This situation has prompted us to investigate on the potential of OPV based organogels for the purpose of energy transfer and light harvesting. [10] Small-molecule-based organogels have attracted much attention in recent years because of their interesting physical properties and architectural elegance. [11] However, organogels based on p-conjugated systems are relatively very few. [12] Recently, we have reported hydrogen-bond-and p-stackinduced supramolecular assembly of the OPV derivatives 1 a,b, which leads to the formation of entangled nanostructures, which induce gelation of hydrocarbon solvents. [13] The absorption and emission properties of 1 a,b showed dramatic changes during gelation, which is an indication of strong intermolecular p-electronic coupling of the ordered selfassembled OPV gel. Excitation of 1 a,b in cyclohexane at 380 and 470 nm revealed the emission corresponding to the monomeric species (l em ¼ 455 and 483 nm, F f ¼ 0.40 AE 0.01 related to quinine sulfate, t ¼ 1.46 ns; Figure 1, spectrum b) and self-assembled species (l em ¼ 525 and 565 nm, F f ¼ 0.40 AE 0.01 related to Rhodamine 6G, t ¼ 1.62 ns; Figure 1, spectrum c), which showed strong dependency on solvent polarity and temperature.Herein we describe an interesting case of a thermoreversible fluorescence-resonance energy transfer (FRET) and light harvesting, exclusively from OPV based supramolecular gel nanostructures of 1 a,b to an organic dye. To study the feasibility of such an energy transfer, we chose Rhodamine B as the acceptor, the absorption (l max ¼ 555 nm...