We demonstrate room temperature visible wavelength photoluminescence from In0.5Ga0.5As quantum dots embedded in a GaP membrane. Time-resolved above band photoluminescence measurements of quantum dot emission show a biexpontential decay with lifetimes of ≈200 ps. We fabricate photonic crystal cavities which provide enhanced outcoupling of quantum dot emission, allowing the observation of narrow lines indicative of single quantum dot emission. This materials system is compatible with monolithic integration on Si, and is promising for high efficiency detection of single quantum dot emission as well as optoelectronic devices emitting at visible wavelengths.Semiconductor quantum dot (QD) emitters grown in gallium phosphide are important for both classical optoelectronic and quantum applications. The close match between the lattice constants of GaP and Si (0.37% at 300K [1]) is promising for monolithic integration with silicon [1][2][3], and the large electronic band gap of GaP allows light emission at visible wavelengths. Single quantum dots (QDs) at visible wavelengths are beneficial for quantum applications since Si avalanche photodiodes (APDs) have maximum quantum efficiency in the red part of spectrum; additionally, emission in this part of the spectrum can be frequency downconverted to telecommunications wavelengths using readily available lasers [4,5].Quantum dots emitting in the red have been extensively studied over the past decade in materials systems including InP/InGaP[6-9], InP/GaP [10,11], InP/AlGaInP [12,13], GaInP/GaP [14], InAs/GaP [15], and AlGaInP/GaP [16]. Of these systems, clear single quantum dots with narrow emission lines exhibiting antibunching have been observed only in the InP/InGaP and InP/AlGaInP systems. GaP-based materials, by contrast, allow either monolithic integration with Si or growth on a non-absorbing GaP substrate (due to the large indirect electronic band gap); additionally, the stronger second order optical nonlinearity of GaP compared to InGaP is preferable for on-chip frequency downconversion to telecom wavelengths. Recently [17], low temperature emission (80K) was measured from In 0.5 Ga 0.5 As self-assembled QDs in GaP emitting in the red part of the spectrum. This system provides large wavelength tunability as the In fraction can be varied from 0.07-0.50 without introducing dislocations; additionally it should provide deeper confinement for carriers than InP/GaP. Subsequently, room temperature emission was measured from In 0.3 Ga 0.7 As/GaP QDs[18]; measured temperature dependence of emission and supporting tight binding calculations indicated good confinement of carriers and type-I emission. Here, we further characterize this materials system, integrate it with photonic nanostructures that enhance the emission of the QDs, and observe evidence indicative of emission from individual QDs. The QDs are grown by solid source molecular beam epitaxy in the center of a 200 nm thick GaP membrane grown on top of a 500 nm layer of Al 0.8 Ga 0.2 P on a (001) GaP substrate. Fig. 1a sho...