The effect of surfaces on the optical properties of GaAs nanowires is evidenced by comparing nanowires with or without an AlGaAs capping shell as a function of the diameter. We find that the optical properties of unpassivated nanowires are governed by Fermi-level pinning, whereas, the optical properties of passivated nanowires are mainly governed by surface recombinations. Finally, we measure a surface recombination velocity of 3 ϫ 10 3 cm s −1 one order of magnitude lower than values previously reported for ͕110͖ GaAs surfaces. These results will serve as guidance for the application of nanowires in solar cell and light emitting devices. © 2010 American Institute of Physics. ͓doi:10.1063/1.3519980͔Semiconducting nanowires ͑NWs͒ are a topic of intense research as they offer the opportunity to explore properties of one-dimensional electronic systems. The understanding and the mastering of the electronic properties of such onedimensional systems are essential to achieve high efficiency devices. In particular, with the increase of the surface/volume ratio, the electronic properties of NW based devices become strongly dependent on the surface electronic states that can alter their electronic properties. Two main surface effects are reported in literature: surface states can act as recombination centers for free carriers 1,2 or as surface charged traps. 3,4 The first effect has recently been quantified by an original optical method for silicon NWs. 5,6 The surface charge traps induce a pinning of the Fermi-level at the surface. A depletion shell appears and the electronic channel available for carriers is narrowed. Experimental proof of this effect in semiconducting NWs was observed by photoconductivity or capacitancevoltage measurements. [7][8][9][10] In this letter, we present our results on the influence of surfaces on GaAs NWs measured by low temperature microphotoluminescence ͑-PL͒ spectroscopy. A systematic comparison is done between unpassivated NWs and those that were capped with a shell of Al 0.4 Ga 0.6 As. Moreover, we take advantage of the tapered shape of the NWs to understand the role of diameter and surface/volume ratios in the luminescence efficiency. We demonstrate that capping directly modifies the recombination velocity and that passivated NW electronic properties are governed by surface recombinations, whereas, unpassivated NWs are strongly depleted by the Fermi-level pinning at the surface induced by charged surface trap states. This work will serve as a guidance for the passivation of the NW surfaces, which is of crucial importance for applications in laser and solar cell technology.
11GaAs NWs were synthesized by molecular beam epitaxy. The growth conditions are described elsewhere.
12-14The NWs have a prismatic shape and exhibit a pure zincblende GaAs crystal structure oriented along the ͑111͒ direction. Surfaces are ͕110͖ oriented. 15,16 The NWs are extremely long ͑16 m͒ and present a tapered shape ͑diameters go from 140 nm at the base to 70 nm at the tip͒. We investigated two samples which di...