We investigated the origin of broad luminescence observed from an array of site-controlled InGaN nanodots grown by selective area epitaxy (SAE). Epitaxially grown site-controlled nanodots with lateral dimensions <50 nm and an array density of 10 10 cm À2 have been studied. During the nanoscale SAE, incorporation of adatoms from the SiO 2 mask has greater relative importance, resulting in a non-uniform growth profile. This non-uniform growth profile leads to significant broadening of the InGaN nano-heterostructure luminescence. Later in the SAE process, an orientation-dependent growth rate coalesces various crystal planes and transforms these nanostructures into a more uniform array.1 Introduction III-nitride nanostructures possess unique properties, such as a wide tuning range for the emission wavelength [1, 2] large exciton binding energy (!26 meV in bulk) [3,4], and robust spin coherence [5], making them particularly attractive for applications in nanophotonics [6,7], spintronics [5,8], and quantum information processing [7,9]. In many of these applications, it is critical to be able to control the dimension and location of the nanostructures. For example, exciton-cavity coupling requires the precise placement of a single quantum dot heterostructure at the anti-node of an optical cavity [10]. To date, most of the III-nitride nanostructures have been fabricated by the self-assembled Stranski-Krastanow (SK) growth [11], which does not enforce control over the structures' position or dimension, demotivating their practical use on the device level. In recent years, selective area epitaxy (SAE) using metal-organic chemical vapor deposition (MOCVD) has been proven to be feasible for the fabrication of a variety of site-controlled III-nitride nanostructures, such as nanowires [12] and nanodots [2,[13][14][15][16][17][18]. During SAE, the morphology of the three-dimensional epistructure grown within the mask opening evolves according to the growth dynamics [12,19], source supply mechanisms [20,21], and growth rate anisotropy [22,23]. Because optical properties of III-nitride heterostructures strongly