We have determined the lattice location of implanted arsenic in GaN by means of conversion electron emission channeling from radioactive 73 As. We give direct evidence that As is an amphoteric impurity, thus settling the long-standing question as to whether it prefers cation or anion sites in GaN. The amphoteric character of As and the fact that As Ga "antisites" are not minority defects provide additional aspects to be taken into account for an explanantion of the so-called "miscibility gap" in ternary GaAs 1−x N x compounds, which cannot be grown with a single phase for values of x in the range 0. The growth and properties of ternary semiconductors of the nitride family have been under intense investigation ever since nitrides emerged as blue-light emitting devices in the 1990s. The particular interest in the ternary nitrides results from the fact that they allow adjusting the semiconductor band gap to values not available in pure compounds. One of the ternary systems under study is GaAs 1−x N x , which shows some intriguing properties such as large band gap bowing parameter [1][2][3]. Unfortunately the growth of GaAs 1−x N x compounds encounters significant difficulties, one of the reasons being that GaAs crystallizes in the cubic zinc blende structure while the most stable polytype of GaN is hexagonal wurtzite. However, while, on the As-rich side of the phase diagram, it is possible to incorporate up to ~10-15% of N into cubic GaAs [3,4], on the N-rich side not more than ~1% of As in GaN have been achieved [5][6][7][8]. In the intermediate region, usually the coexistence of hexagonal N-rich GaAsN and cubic As-rich GaNAs phases is observed.GaN which is lightly As-doped is also highly interesting due to the fact that it shows intense blue luminescence centered around 2.6 eV, as observed already many years ago in Asimplanted GaN by Pankove and Hutchby [9] and Metcalfe et al [10], and subsequently also found in GaN doped with As during growth [5,[11][12][13][14][15][16]. The chemical nature of the 2.6 eV blue luminescence and the fact that it results from optical centers involving one As atom only was unambiguously proven by means of the radiotracer photoluminescence (PL) work of Stötzler et al [17], who studied the luminescence along the radioactive decay chains 71 As→ 71 Ge→ 71 Ga and 72 Se→ 72 As→ 72 Ge. Following the ion implantation of 71 As and 72 Se they observed the intensity of the 2.6 eV luminescence to scale with the amount of radioactive 71 As and 72 As resulting from radioactive decay.The amphoteric nature of As in GaN was first proposed by Guido et al [18], who suggested that As could fill up both Ga and N vacancies and thus reduce yellow band emission and carrier scattering in GaN. Subsequently, the 2.6 eV blue luminescence [12,[14][15][16]19] and a deep level ~0.8 eV below the conduction band have been attributed to As Ga [20,21]. While there are indications that the As Ga :As N ratio changes with the overall Ga:N:As stoichiometry [13,15], so far no direct evidence for so-called As Ga "anti-sit...