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Abstracts Book - IMRC 2018

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• SD4-O015 Invited Talk<br />

UNDERSTANDING AMORPHOUS MESOPOROUS SILICA<br />

SUPERSTRUCTURES BY ABERRATION-CORRECTED STEM<br />

Sebastian Calderon 1 , Tânia Ribeiro 2 , José Paulo Farinha 2 , Carlos Baleizão 2 , Paulo Ferreira 1,3<br />

1 International Iberian Nanotechnology Laboratory - INL, Advanced Electron Microscopy,<br />

Imaging and Spectroscopy, Portugal. 2 IST, University of Lisbon, Centro de Química-Física<br />

Molecular and Institute of Nanosciences and Nanotechnology, Portugal. 3 University of Texas at<br />

Austin, Materials Science and Engineering, United States.<br />

Mesoporous silica nanoparticles (NPs) have been intensively studied due to their<br />

potential use in catalysis and biomedicine, including cancer treatment and drug<br />

delivery applications. However, when mesoporous particles are produced at the<br />

nanoscale, the pore configuration is modified. In order to determine the pore<br />

morphology and structure, advanced microscopy techniques are required.<br />

This work combines molecular dynamics techniques, electron microscopy<br />

computer simulations and aberration-corrected STEM imaging to provide an<br />

insight into the structure of amorphous SiO2 NPs. The amorphous silica model<br />

is prepared using a simple melt-quench molecular dynamics (MD) method, while<br />

the reconstruction of the mesoporous NPs is carried out using an isotropic unit<br />

cell to avoid false symmetry in the final model. For the high-resolution STEM<br />

simulations, the QSTEM software package is used based on a multisliced<br />

technique. Finally, for comparison with the simulated images high angular<br />

annular dark field (HAADF) STEM images were taken using an aberration<br />

corrected FEI Titan ChemiSTEM microscope, operated at 200 kV.<br />

The amorphous models are analyzed using the radial distribution function (RDF)<br />

and mass density, demonstrating a good agreement with the experimental<br />

results. Depending on the quenching model, the local density can be modified<br />

obtaining isotropic values between 2.2 and 4 g cm-3, with radial distribution<br />

function similar to the bulk values reported experimentally. The highest<br />

probability of finding Si-O pairs is at 1.58 Å, O-O is at 2.62 Å and Si-Si 3.08 Å. The<br />

multisliced STEM images demonstrate that the density of the models do not<br />

have a significant impact on the STEM images for isolated SiO2 phases. However,<br />

a detailed analysis reveals that the intensities of the systems shows that denser<br />

SiO2 structures results in a more intense signal, due to the increase in the<br />

scattering power.

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