All authors discussed the results. FY completed the manuscript. All authors

read and approved the final manuscript.”
“Background We are currently PI3K inhibitor living through a transition in electronic circuitry from the classical to the quantum domain. With Moore’s Law on the way out, thanks to the recent unveiling of ohmic 2 nm epitaxial nanowires [1] and epitaxially gated single-atom quantum transistors [2], the challenge for scientists becomes finding new ways to increase the density and speed of devices as we can no longer rely on being able to shrink their components. Far-sighted speculation has already been abundant for many years regarding efficient use of the third dimension in device architecture [3–6], breaking the two-dimensional paradigm of current electronics manufacturing techniques. Recent germanium-based

works [7, STI571 8] illustrated fundamental physics required for full 3D device implementation and heralded the creation of multiple stacked δ-layers of dopants within a semiconductor. Each of these layers could potentially display atomically abrupt doped regions for selleck products in-plane device function and control. Multiple layers of this nature have indeed been created in Ge [9]. The P in Ge atomic layer deposition technique parallels phosphorus in silicon 1/4 monolayer (ML) doping (Si: δP), created using scanning tunnelling microscope lithography, with a few minor technological improvements (annealling temperatures, amongst others) [8]. In Anidulafungin (LY303366) contrast, one major advantage of improvements to silicon technology is that uptake may be far easier, given the ubiquity of silicon architecture in the present everyday life. We may therefore expect to see, in the near future, Si: δP systems of similar construction. The time is thus ripe to attend to possible three-dimensional architectures built from phosphorus in silicon. Although Si:P

single-donor physics is well understood, and several studies have been completed on single-structure epitaxial Si: δP circuit components (such as infinite single monolayers [10–17], single thicker layers [18, 19], epitaxial dots [20], and nanowires [1, 21]), a true extension studying interactions between device building blocks in the third dimension is currently missing. The description of experimental devices is a thorny problem involving the trade-off between describing quantum systems with enough rigour and yet taking sufficient account of the disorder inherent to manufacturing processes. A first approach might therefore be to study the simplest case of interacting device components, namely two P-doped single monolayers (bilayers) [22, 23]. Given the computational limitations of ab initio modelling it is currently not possible to treat the disordered multi-layer system in full. Two approaches suggest themselves. In [23] the approach was to simplify the description of the delta-layer in order to study disorder through a mixed atom pseudopotentials approach.