GaAs-based microcavities. [2] However, the applications of III-V and II-VI inorganic semiconductors in polaritonics are relatively limited due to the challenging growth techniques required to create wide bandgap semiconductors together with the necessity of using cryogenic temperatures to create Wannier-Mott excitons. [3,4] Organic semiconductors however comprise the broadest class of strongly coupled materials developed to date and include molecular dyes, crystalline organic molecules, oligofluorenes, and conjugated polymers. [5][6][7][8][9][10][11] Owing to the high quantum yield, large dipole moment of optical transitions and high-binding energy of excitons, organic semiconductors have permitted the physics and applications of polaritonics to be explored at room temperature. [12,13] Polariton lasing is one of the most distinctive nonlinear phenomena related to the collective behavior of exciton polaritons. In contrast to conventional photon lasers, a polariton laser does not necessitate the electronic inversion of population, but is instead driven by a stimulated relaxation to a coherent state during the process of condensation to the ground polariton state. This process has allowed polariton lasers to exhibit significantly lower thresholds compared to photon lasers that have been fabricated using the same device configuration. [14,15] Recently, we demonstrated polariton lasing in the yellow part of the spectrum in an organic microcavity containing the molecular dye bromine-substituted boron-dipyrromethene (BODIPY-Br). [5] In the present paper, we explore the incorporation of another molecular dye of the BODIPY family, namely BODIPY-G1 fluorescent dye, into a microcavity and show that by incorporating a wedged cavity-layer configuration, we can achieve strong coupling over a broad range of exciton-photon detuning conditions. Such structures allow us to controllably access different cavity lengths and thus select the energy of the ground polariton state. We then use this approach to provide evidence of polariton lasing over a broad range of wavelengths (>30 nm) utilizing a single material system.