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1 Supporting Information Investigation of ion induced bending mechanism for nanostructures Nitul S Rajput * , Zhen Tong * and Xichun Luo * Department of Design, Manufacture and Engineering management, University of Strathclyde, Glasgow G1 1XQ, United Kingdom Caption for movie Movie S1 The Scanning Ion Microscopy (SIM) video shows the bending of a Si nanowire upon irradiating by a 16 keV, 21 pA Ga ion beam. The nanowire bends towards the side of the ion beam direction. Molecular Dynamics simulation: For the simulation, we have used Large-scale Atomic/Molecular Massively Parallel Simulator (LAMMPS), a classical molecular dynamics code managed and distributed by Sandia National Laboratories, US. 1 As described in the main manuscript, the cylindrical § Corresponding address: Prof. Xichun Luo. Email:[email protected]

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    Supporting Information

    Investigation of ion induced bending mechanism

    for nanostructures

    Nitul S Rajput*, Zhen Tong* and Xichun Luo*§

    *Department of Design, Manufacture and Engineering management, University of

    Strathclyde, Glasgow G1 1XQ, United Kingdom

    Caption for movie Movie S1 The Scanning Ion Microscopy (SIM) video shows the bending of a Si

    nanowire upon irradiating by a 16 keV, 21 pA Ga ion beam. The nanowire bends towards

    the side of the ion beam direction.

    Molecular Dynamics simulation: For the simulation, we have used Large-scale Atomic/Molecular Massively Parallel

    Simulator (LAMMPS), a classical molecular dynamics code managed and distributed by

    Sandia National Laboratories, US.1 As described in the main manuscript, the cylindrical

    § Corresponding address: Prof. Xichun Luo. Email:[email protected]

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    nanopillar was built with a diameter of 21.7 nm and height of 43.4 nm. The pillar was

    composed of 806, 466 atoms in total.

    For the visualization of the atoms, Visual Molecular Dynamics (VMD) was used.2

    The Tersoff.ZBL Potential function gives the energy E of a system of atoms as:

    12 iji j i

    E V≠

    = ∑∑ (1)

    (1 ( )) ( )ZBL Tersoffij ijij ij ijF Ff fV V Vr r= − + (2)

    ( )

    1( )1 F ij CijF A r r

    f re− −

    =+

    (3)

    where the 𝑉!"!"# and 𝑉!"!"#$%&& indicate ZBL portion and Tersoff portion, respectively.

    The distance between atoms i and j is rij. The fF term is a Fermi-like function used to

    smoothly connect the ZBL repulsive potential with the Tersoff potential. There are two

    parameters used to adjust it: AF and rC. AF controls how "sharp" the transition is between

    the two portions, and rC is essentially the cutoff distance for the ZBL potential. The

    parameters of Tersoff.ZBL Potential function used in present MD simulation are shown

    in Table S1.

    Parameters Ga Si m 1 1 γ 1 1 λ! 0 0 c 7.6298×10!! 1.0039×10! d 1.9796×10! 1.6217×10!

    cos θ! 7.1459×10!! −5.9825×10!! N 3.47290 7.8734×10!! β 2.3586×10!! 1.1000×10!!

    λ! Å!! 1.7154 1.7322 B eV 1.14786×10! 4.7118×10! R Å 2.8 2.7

    D 0.1 0.15 λ! Å!! 3.2834 2.4799

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    A eV 2.83982×10! 1.8308×10! Zi 31 14 Zj 31 14

    Table S1: The parameters used in the potential function Tersoff.ZBL in the present MD

    simulation.

    Supplementary Figures:

    Figure S1: High resolution TEM image of a FIB fabricated Si NW depicts the presence of

    several crystalline planes at random orientations in the wire. The inset shows a

    convergent beam electron diffraction (CBED) pattern collected from the NW.

    10 nm

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    Figure S2: Bright field TEM image of a NW showing deposition of thick amorphous

    layers on some portions of the wire; (a) before and (b) after excessive e-beam irradiation.

    References:

    (1) http://lammps.sandia.gov/index.html.

    (2) Humphrey W.; Dalke A.; Schulten, K. J. Molec. Graphics 1996, 14.1, 33.

    100 nm 100 nm

    (b) (a)

    Amorphous layers