Zn 3 As 2 is a promising earth-abundant semiconductor material. Its bandgap, around 1 eV, can be tuned across the infrared by alloying and makes this material suited for applications in optoelectronics. Here, we report the crystalline structure and electrical properties of strain-free Zn 3 As 2 nanosails, grown by metal-organic vapor phase epitaxy. We demonstrate that the crystalline structure is consistent with the P4 2 /nmc (D 15 4h ) α"-Zn 3 As 2 metastable phase. Temperature-dependent Hall effect measurements indicate that the material is degenerately p-doped with a hole mobility close to 10 3 cm 2 V À1 s À1 . Our results display the potential of Zn 3 As 2 nanostructures for next generation energy harvesting and optoelectronic devices.The increasing production of high-performance electronic devices and the push towards generating energy in a sustainable manner leads to sustainability challenges for optoelectronic and photovoltaic (PV) technologies. Particularly affected are devices using atomic elements of scarce abundance in the earth's crust, which prevents their widespread deployment. In this context, highly functional materials made of earth-abundant elements are being sought for both PV and optoelectronic applications. The second most abundant element in the earth's crust, silicon, is a semiconductor very successfully deployed in the PV market. It suffers nonetheless from its indirect bandgap and the consequently high purity required for the production of efficient solar cells. Both characteristics increase the energy needs for silicon PV device production. The so-called "second generation" solar cells, built with much thinner, direct bandgap active layers, could in principle solve these two issues. Still, these thin film solar cells exhibit either a long energy payback time (amorphous silicon) or they use scarce and expensive elements (ex: copper, indium, gallium, selenium, cadmium, tellurium).Direct bandgap semiconductors employing earth-abundant elements could combine the advantages of all these material families. They would enable efficient light collection in a thin film of easily available materials. Copper zinc tin sulfide (CZTS) and zinc phosphide (Zn 3 P 2 ) have received increasing attention as materials satisfying these criteria for efficient and sustainable light conversion discussed so far. Belonging to the same family, zinc arsenide (Zn 3 As 2 ) is a p-type semiconductor structurally similar to Zn 3 P 2 . It exhibits a band gap around 1.0 eV [1] and potentially high hole mobilities. [2] The stoichiometry of this material can be transformed continuously into Cd 3 As 2 [3] or Zn 3 P 2[4] by appropriate atomic substitutions, shifting its bandgap energy toward 1.5 eV and 0 eV, respectively. (Zn 1Àx Cd x ) 3 As 2 transforms from a semiconductor to a threedimensional Dirac semimetal as x reaches 0.62. [5] The ability to tune its direct bandgap energy makes this material system very attractive for long-wavelength optoelectronics and as a constituent in multi-junction solar cells. M II 3 X V 2 comp...