Before proposing a mechanism to control the diameter of Al nanorods, we must first assess the current state of understanding and determine why the controllable growth of Al

nanorods has not been reported so far. Based on modeling studies – including atomistic simulations and theoretical formulations – the growth of metallic nanorods relies on the kinetic stability of multiple-layer Maraviroc cost surface steps [11, 12]. This stability further correlates with the magnitude of diffusion barriers that adatoms experience when moving over multiple-layer surface step [13, 14]. According to quantum mechanics calculations, this diffusion barrier is only 0.13 eV for Al [15], compared to 0.40 eV for copper [16], and as a result, the growth of pure Al nanorods has been predicted to be impossible [11]. In contrast to our model prediction, two experimental studies R788 order by Au et al. and Khan et al. [6, 10] have realized Al nanorods. In reconciling the modeling prediction and the experiments, we note three pieces of knowledge: (1) oxygen (O) atoms may be present at large quantities

in the medium to high vacuum levels of the experimental studies [6, 10]; (2) O has been used as a surfactant in thin film growth [17, 18]; and (3) Al oxide has a much higher melting temperature than Al, and therefore, the adatom diffusion barrier over the surface steps of Al oxide is much larger than the 0.13 eV of Al. In this letter, we first propose the mechanism that enables the growth of Al nanorods using physical vapor deposition based on the three pieces of knowledge noted above. Taking the mechanism tuclazepam to action in combination with existing theory, we go on to grow Al nanorods with controllable diameters through modulation of vacuum levels and substrate temperatures. As schematically shown in Figure  1, our proposal combines the use of glancing angle deposition (GLAD) [19] and the use of O as a surfactant, the amount of which is controlled by the vacuum level. Figure 1 Oxygen surfactant mechanism

schematic. Schematic of controllably growing Al nanorods (in gray) using physical vapor deposition, with O atoms (red spheres) as surfactant. In the following, we describe how this mechanism functions. Due to the glancing angle incidence, deposited Al atoms land primarily on the top of nanorods or nanorod nuclei (troughs of a rough surface). At low to medium vacuum level, for example 1 × 10 -2 Pa, a large number of O atoms will quickly bind to and decorate the step edges, which are preferential binding sites of surfactant atoms [20]. The stronger local Al-O interactions (relative to Al-Al interactions) will result in a large diffusion barrier for Al adatoms over the surface steps that are decorated by O. Varying the amount of O atoms, through the control of vacuum level, will change either the local chemical composition or the spatial dimension of the Al oxide near the surface steps.