Efficient electron and hole doping in compositionally abrupt Si/Ge nanowires
Related Experiment Video
Updated: May 13, 2026

Monolayer Contact Doping of Silicon Surfaces and Nanowires Using Organophosphorus Compounds
Published on: December 2, 2013
Pengfei Li1, Rulong Zhou, Bicai Pan
1Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China.
Abstract:
Efficient doping in semiconductor nanowires can be a challenging task in materials science. In this study, we explore effects of various dopant elements (P, N, Al, B, and O) on the electronic properties of three types of compositionally abrupt SiGe nanowires (NWs), namely, the core-shell Ge(core)/Si(shell) and Si(core)/Ge(shell) NWs, and the fused triangular-prism SiGe NW. Based on the density-functional theory calculations, we find that the substitution of Ge by the pentavalent P at the interfacial region between the core and shell of Ge/Si NWs leads to an easy injection of high-density free-electron-like carriers, whereas the substitution of Si by trivalent Al or B at the interfacial region leads to an easy injection of high-density free-hole-like carriers. However, the introduction of the pentavalent N has little effect on the conductivity of the three types of SiGe NWs. For the divalent O dopant, only the substitution of Si by O in the fused triangular-prism SiGe NW can result in high-density free-hole-like carriers at low temperature. This comprehensive study demonstrates, for the first time, that the doping efficiency not only depends on the type of dopant element (which is well-known) but also on the interfacial geometry of the Si/Ge domains within the compositionally abrupt NWs. The study can offer guidance to the synthesis of novel compositionally abrupt SiGe NWs through a tailored interfacial geometry and controlled interfacial doping.
More Related Videos
Related Concept Videos
Semiconductors
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Types of Semiconductors
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Fermi Level Dynamics
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
P-N junction
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...

