Limits to Metallic Conduction in Atomic-Scale Quasi-One-Dimensional Silicon Wires

被引:23
作者
Weber, Bent [1 ]
Ryu, Hoon [2 ]
Tan, Y. -H. Matthias [3 ]
Klimeck, Gerhard [3 ]
Simmons, Michelle Y. [1 ]
机构
[1] Univ New S Wales, Sch Phys, Ctr Excellence Quantum Computat & Commun Techol, Sydney, NSW 2052, Australia
[2] KISTI, Natl Inst Supercomp & Networking, Taejon 305806, South Korea
[3] Purdue Univ, Birck Nanotechnol Ctr, Network Computat Nanotechnol, W Lafayette, IN 47907 USA
基金
澳大利亚研究理事会;
关键词
COULOMB-BLOCKADE; ELECTRON-SPIN; QUANTUM; FLUCTUATIONS; CONFINEMENT; TRANSITION;
D O I
10.1103/PhysRevLett.113.246802
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The recent observation of ultralow resistivity in highly doped, atomic-scale silicon wires has sparked interest in what limits conduction in these quasi-1D systems. Here we present electron transport measurements of gated Si:P wires of widths 4.6 and 1.5 nm. At 4.6 nm we find an electron mobility, mu(el) similar or equal to 60 cm(2)/V s, in excellent agreement with that of macroscopic Hall bars. Metallic conduction persists to millikelvin temperatures where we observe Gaussian conductance fluctuations of order delta G similar to e(2)/h. In thinner wires (1.5 nm), metallic conduction breaks down at G less than or similar to e(2)/h, where localization of carriers leads to Coulomb blockade. Metallic behavior is explained by the large carrier densities in Si:P delta-doped systems, allowing the occupation of all six valleys of the silicon conduction band, enhancing the number of 1D channels and hence the localization length.
引用
收藏
页数:5
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