Non-equilibrium induction of tin in germanium: towards direct bandgap Ge1−xSnx nanowires

The development of non-equilibrium group IV nanoscale alloys is critical to achieving new functionalities, such as the formation of a direct bandgap in a conventional indirect bandgap elemental semiconductor. Here, we describe the fabrication of uniform diameter, direct bandgap Ge1−xSnx alloy nanowires, with a Sn incorporation up to 9.2 at.%, far in excess of the equilibrium solubility of Sn in bulk Ge, through a conventional catalytic bottom-up growth paradigm using noble metal and metal alloy catalysts. Metal alloy catalysts permitted a greater inclusion of Sn in Ge nanowires compared with conventional Au catalysts, when used during vapour–liquid–solid growth. The addition of an annealing step close to the Ge-Sn eutectic temperature (230 °C) during cool-down, further facilitated the excessive dissolution of Sn in the nanowires. Sn was distributed throughout the Ge nanowire lattice with no metallic Sn segregation or precipitation at the surface or within the bulk of the nanowires. The non-equilibrium incorporation of Sn into the Ge nanowires can be understood in terms of a kinetic trapping model for impurity incorporation at the triple-phase boundary during growth.

[1]  Hongjun Gao,et al.  Self-assembled two-dimensional superlattice of Au-Ag alloy nanocrystals , 2002 .

[2]  Hugh Geaney,et al.  Synthesis of Tin Catalyzed Silicon and Germanium Nanowires in a Solvent–Vapor System and Optimization of the Seed/Nanowire Interface for Dual Lithium Cycling , 2013 .

[3]  G. Patriarche,et al.  Incorporation and redistribution of impurities into silicon nanowires during metal-particle-assisted growth , 2014, Nature Communications.

[4]  C. Leinenbach,et al.  Wetting Behavior of Ternary Au-Ge-X (X = Sb, Sn) Alloys on Cu and Ni , 2013, Journal of Electronic Materials.

[5]  J. Ciulik,et al.  The AuSn phase diagram , 1993 .

[6]  P. Voorhees,et al.  Catalyst incorporation at defects during nanowire growth. , 2012, Nano letters.

[7]  James S. Harris,et al.  Increased photoluminescence of strain-reduced, high-Sn composition Ge1−xSnx alloys grown by molecular beam epitaxy , 2011 .

[8]  Zoran Ikonic,et al.  The direct and indirect bandgaps of unstrained SixGe1−x−ySny and their photonic device applications , 2012 .

[9]  R. Soref Mid-infrared photonics in silicon and germanium , 2010 .

[10]  Harry A. Atwater,et al.  INTERBAND TRANSITIONS IN SNXGE1-X ALLOYS , 1997 .

[11]  Charles M. Lieber,et al.  Imaging and analysis of nanowires , 2004, Microscopy research and technique.

[12]  Ashish Arora,et al.  Indirect-to-direct band gap crossover in few-layer MoTe₂. , 2015, Nano letters.

[13]  J. M. Gray,et al.  On-chip optical interconnects made with gallium nitride nanowires. , 2013, Nano letters.

[14]  Martin Kittler,et al.  Germanium tin: silicon photonics toward the mid-infrared , 2013 .

[15]  Steven G. Louie,et al.  Computational design of direct-bandgap semiconductors that lattice-match silicon , 2001, Nature.

[16]  John Kouvetakis,et al.  TIN-BASED GROUP IV SEMICONDUCTORS: New Platforms for Opto- and Microelectronics on Silicon , 2006 .

[17]  John Kouvetakis,et al.  Scaling law for the compositional dependence of Raman frequencies in SnGe and GeSi alloys , 2004 .

[18]  Harry A. Atwater,et al.  Nonlithographic epitaxial SnxGe1−x dense nanowire arrays grown on Ge(001) , 2003 .

[19]  Corey L. Bungay,et al.  Tunable band structure in diamond–cubic tin–germanium alloys grown on silicon substrates , 2003 .

[20]  S. Barth,et al.  Microwave-assisted solution-liquid-solid growth of Ge1-xSnx nanowires with high tin content. , 2015, Chemical communications.

[21]  K. Dick,et al.  Controlled polytypic and twin-plane superlattices in iii-v nanowires. , 2009, Nature nanotechnology.

[22]  Peng Wang,et al.  High-resolution detection of Au catalyst atoms in Si nanowires. , 2008, Nature nanotechnology.

[23]  Qun Wei,et al.  Strain-engineered direct-indirect band gap transition and its mechanism in two-dimensional phosphorene , 2014 .

[24]  P. Voorhees,et al.  Phase equilibrium and nucleation in VLS-grown nanowires. , 2008, Nano letters.

[25]  In-situ observations of nanoscale effects in germanium nanowire growth with ternary eutectic alloys. , 2015, Small.

[26]  Zoran Ikonic,et al.  Band structure calculations of Si–Ge–Sn alloys: achieving direct band gap materials , 2007 .

[27]  Bozhi Tian,et al.  Rational growth of branched nanowire heterostructures with synthetically encoded properties and function , 2011, Proceedings of the National Academy of Sciences.

[28]  J. C. Baker,et al.  Solute trapping by rapid solidification , 1969 .

[29]  Manipulating the growth kinetics of vapor-liquid-solid propagated Ge nanowires. , 2013, Nano letters.

[30]  Gregor Mussler,et al.  Optical Transitions in Direct-Bandgap Ge1–xSnx Alloys , 2015 .

[31]  Johnson,et al.  Electronic structure of ordered silicon alloys: Direct-gap systems. , 1996, Physical review. B, Condensed matter.

[32]  Yi-Chiau Huang,et al.  Highly selective dry etching of germanium over germanium-tin (Ge(1-x)Sn(x)): a novel route for Ge(1-x)Sn(x) nanostructure fabrication. , 2013, Nano letters.

[33]  S. Senz,et al.  Colossal injection of catalyst atoms into silicon nanowires , 2013, Nature.

[34]  James S. Harris,et al.  Raman study of strained Ge1−xSnx alloys , 2011 .

[35]  David Smith,et al.  SnGe superstructure materials for Si-based infrared optoelectronics , 2003 .

[36]  Krishna C. Saraswat,et al.  Achieving direct band gap in germanium through integration of Sn alloying and external strain , 2013 .

[37]  John Kouvetakis,et al.  Synthesis of ternary SiGeSn semiconductors on Si(100) via SnxGe1−x buffer layers , 2003 .

[38]  Xingao Gong,et al.  Origin of the Unusually Large Band-Gap Bowing and the Breakdown of the Band-Edge Distribution Rule in the SnxGe1-x Alloys , 2008 .

[39]  Jenkins Dw,et al.  Electronic properties of metastable GexSn , 1987 .

[40]  J. Faist,et al.  Lasing in direct-bandgap GeSn alloy grown on Si , 2015, Nature Photonics.

[41]  Stefan Zollner,et al.  Ge–Sn semiconductors for band-gap and lattice engineering , 2002 .

[42]  E. O’Reilly,et al.  Nature of the band gap of silicon and germanium nanowires , 2006 .

[43]  Marvin L. Cohen,et al.  Possibility of increased mobility in Ge-Sn alloy system , 2007 .

[44]  P. Galenko Solute trapping and diffusionless solidification in a binary system. , 2007, Physical review. E, Statistical, nonlinear, and soft matter physics.

[45]  M. Morris,et al.  Inherent control of growth, morphology, and defect formation in germanium nanowires. , 2012, Nano letters.

[46]  Chenming Hu,et al.  Green transistor as a solution to the IC power crisis , 2008, 2008 9th International Conference on Solid-State and Integrated-Circuit Technology.

[47]  S. Gradečak,et al.  Controlled modulation of diameter and composition along individual III-V nitride nanowires. , 2013, Nano letters.

[48]  E. Sutter,et al.  Size-dependent phase diagram of nanoscale alloy drops used in vapor--liquid--solid growth of semiconductor nanowires. , 2010, ACS nano.

[49]  Atomistics of vapour–liquid–solid nanowire growth , 2013, Nature communications.

[50]  C. L. Senaratne,et al.  Advances in Light Emission from Group-IV Alloys via Lattice Engineering and n-Type Doping Based on Custom-Designed Chemistries , 2014 .

[51]  Wei Du,et al.  Direct-bandgap GeSn grown on silicon with 2230 nm photoluminescence , 2014 .