TY - JOUR
T1 - Solution-Phase Growth of Cu Nanowires with Aspect Ratios Greater Than 1000
T2 - Multiscale Theory
AU - Kim, Junseok
AU - Cui, Jianming
AU - Fichthorn, Kristen A.
N1 - Funding Information:
This work is funded by the Department of Energy, Office of Basic Energy Sciences, Materials Science Division (Grant No. DE FG02-07ER46414) (J.K.). J.K. acknowledges training provided by the Computational Materials Education and Training (CoMET) NSF Research Traineeship (No. DGE-1449785). This work is also funded by the National Science Foundation (Grant No. OAC-1835607) (J.C.). This work used the Extreme Science and Engineering Discovery Environment (XSEDE), which is supported by National Science Foundation Grant No. ACI-1548562.
Publisher Copyright:
©
PY - 2021/11/23
Y1 - 2021/11/23
N2 - Penta-twinned metal nanowires are finding widespread application in existing and emerging technologies. However, little is known about their growth mechanisms. We probe the origins of chloride- and alkylamine-mediated, solution-phase growth of penta-twinned Cu nanowires from first-principles using multiscale theory. Using quantum density functional theory (DFT) calculations, we characterize the binding and surface diffusion of Cu atoms on chlorine-covered Cu(100) and Cu(111) surfaces. We find stronger binding and slower diffusion of Cu atoms on chlorinated Cu(111) than on chlorinated Cu(100), which is a reversal of the trend for bare Cu surfaces. We also probe interfacet diffusion and find that this proceeds faster from Cu(100) to Cu(111) than the reverse. Using the DFT rates for hopping between individual sites at Ångstrom scales, we calculate coarse-grained, interfacet rates for nanowires of various lengths-up to hundreds of micrometers-and diameters in the 10 nm range. We predict nanowires with aspect ratios of ∼100, based on surface diffusion alone. We also account for the influence of a self-assembled alkylamine layer that covers most of the {100} facets, but is absent or thin and disordered on the {111} facets and in an "end zone"near the {100}/{111} boundary. With an end zone, we predict a wide range of nanowire aspect ratios in the experimental ranges. Our work reveals the mechanisms by which a halide-chloride-promotes the growth of high-aspect-ratio nanowires.
AB - Penta-twinned metal nanowires are finding widespread application in existing and emerging technologies. However, little is known about their growth mechanisms. We probe the origins of chloride- and alkylamine-mediated, solution-phase growth of penta-twinned Cu nanowires from first-principles using multiscale theory. Using quantum density functional theory (DFT) calculations, we characterize the binding and surface diffusion of Cu atoms on chlorine-covered Cu(100) and Cu(111) surfaces. We find stronger binding and slower diffusion of Cu atoms on chlorinated Cu(111) than on chlorinated Cu(100), which is a reversal of the trend for bare Cu surfaces. We also probe interfacet diffusion and find that this proceeds faster from Cu(100) to Cu(111) than the reverse. Using the DFT rates for hopping between individual sites at Ångstrom scales, we calculate coarse-grained, interfacet rates for nanowires of various lengths-up to hundreds of micrometers-and diameters in the 10 nm range. We predict nanowires with aspect ratios of ∼100, based on surface diffusion alone. We also account for the influence of a self-assembled alkylamine layer that covers most of the {100} facets, but is absent or thin and disordered on the {111} facets and in an "end zone"near the {100}/{111} boundary. With an end zone, we predict a wide range of nanowire aspect ratios in the experimental ranges. Our work reveals the mechanisms by which a halide-chloride-promotes the growth of high-aspect-ratio nanowires.
UR - http://www.scopus.com/inward/record.url?scp=85119249221&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85119249221&partnerID=8YFLogxK
U2 - 10.1021/acsnano.1c07425
DO - 10.1021/acsnano.1c07425
M3 - Article
C2 - 34739221
AN - SCOPUS:85119249221
SN - 1936-0851
VL - 15
SP - 18279
EP - 18288
JO - ACS Nano
JF - ACS Nano
IS - 11
ER -