We study the luminescence dynamics of telecom wavelength InAs quantum dots grown on InP(111)A by droplet epitaxy. The use of the ternary alloy InAlGaAs as a barrier material leads to photon emission in the 1.55 µm telecom C-band. The luminescence decay is well described in terms of the theoretical interband transition strength without the impact of nonradiative recombination. The intensity autocorrelation function shows clear anti-bunching photon statistics. The results suggest that our quantum dots are useful for constructing a practical source of single photons and quantum entangled photon pairs. This is the version of the article before peer review, as submitted to Applied Physics Express. The final published version will be available as an Open Access article from the journal's site.A source of single photons and quantum entangled photon pairs is a key device in vast quantum technologies. Semiconductor quantum dots are expected to serve as photon sources that can be operated very efficiently and deterministically. Numerous efforts have already been made to develop a practical quantum dot photon source. However, photon emission in the standard telecom band, particularly around a wavelength of 1.55 µm, which is the maximum transmission window of silica optical fibers, is a material challenge. Careful growth optimization is required to achieve a 1.55 µm emission 1-10 . Nevertheless, the well-known quantum dot growth based on the Stranski-Krastanow mode leads to an asymmetric dot shape, which is not favorable for entangled pair generation.The problem is ideally solved by using droplet epitaxy, which offers considerable freedom regarding the choice of materials and substrates 11 . The application of a C 3v symmetric (111)A surface to the growth substrate results in the creation of almost perfectly symmetric quantum dots, which can work in both the visible wavelength region 12,13 and the infrared telecom wavelength region 14,15 . Recently, the emission wavelength has been extended beyond 1.5 µm for InAs dots embedded in InAlGaAs on InP(111)A 16 . However, the previous samples were not sufficiently optimized: the dot density was too high for a single quantum dot to be isolated using standard micro optics. Moreover, the dot size distribution is relatively large so that careful dot selection is required to find a dot that emits at 1.55 µm.Here, we extend the droplet epitaxy scheme to achieve a purely 1.55 µm photon emission. We introduce the high temperature crystallization protocol, which has recently been applied to the GaAs material system 17,18 , to the InAs/InP material system in order to improve the a) Electronic mail: ha.neul@nims.go.jp b) Electronic mail: kuroda.takashi@nims.go.jp FIG. 1. (Color online) (b) The luminescence spectra of a large ensemble of InAs quantum dots in In0.52Al0.12Ga0.36As /InP(111)A at 12 K at different excitation powers. (b) The luminescence spectra of a single isolated InAs dot with a cw excitation of 40 nW. We focus on this dot in our time-resolved study. The inset shows an atomic fo...