Type of presentation: Oral

IT-10-O-2812 Fast tomography acquisition for in situ 3D analysis of nanomaterials under variable gas and temperature conditions in Environmental-TEM

EPICIER T.1, 2, ROIBAN L.1, LI S.2, AOUINE M.2, SANTOS AIRES F. C.2, TUEL A.2, FARRUSSENG D.2
1MATEIS, INSA de Lyon, Université Lyon I, 69621 Villeurbanne Cedex, France, 2IRCELYON,Université Lyon I, 2, Av. A. Einstein, 69626 Villeurbanne Cedex, France
lucian.roiban@insa-lyon.fr

In the last two decades, tilted tomography in a transmission electron microscope (TEM) has become a widely used approach in order to quantify the three dimensional (3D) distribution of features in materials and nanomaterials[1, 2]. During the tilt series acquisition, a projection of the area of interest is recorded at each angle over a large angular amplitude, the final resolution along Z axis being directly related to the maximal tilting angle. The tilt series acquisition is usually performed automatically; depending on the employed acquisition method (automatic focusing, and cross-correlation based tracking), the total acquisition time typically ranges between 30 minutes to several hours. Such conditions are totally incompatible with in-situ experiments, where the materials are subject to changes under external mechanical or electrical solicitations as well as variable temperature and gas flow. Following the 3D evolution in such a context can be attempted by a ‘before/after’ strategy, where a first tomography analysis is performed on the object prior to any solicitation, then a second one after the solicitation as performed to track fuel cell nanocatalysts during electrochemical aging [3]. The recent development of commercial Environmental TEM (ETEM) [4] offers a wide range of in situ environmental studies of nanomaterials, such as oxidation / reduction at high temperature: this opens new opportunities to (try to) investigate in situ the 3D structure of nanomaterials. In this context, we are currently optimizing a fast acquisition method for tomography studies, based on video acquisition of tilted series in less than 1-4 minutes. We have applied this approach to the study of metallic Ag nanoparticles (NPs) encaged in silicalite hollow shells (silica-cages) for application in selective catalysis [5]. Single-tilt tomography and ETEM experiments were performed on a Cs-corrected TITAN ETEM, 80-300 kV, recently installed at CLYM in Lyon. Results are illustrated by figures 1 (fast acquisition performed over an angular amplitude of 116° in 3 minutes and 40 seconds) and figure 2 (ETEM experiments up to 700°C and oxygen partial pressure of 2 mbar). References [1] P.A. Midgley, R.E. Dunin-Borkowski, Nature Mat., 8 (2009) 271-280. <span>[2] T. Epicier, chap. 3 ‘Imagerie 3D en mécanique des matériaux’, ed. J.Y. Buffière, E. Maire, Hermès - Lavoisier, Paris, (2014). <span>[3] J. Jinschek, Microscopy and Analysis, Nanotechn. Issue November (2012) 5-10. <span>[4] Y. Yu, H.L. Xin, R. Hovden, D. Wang, E.D. Rus, J.A. Mundy, D.A. Muller, H.D. Abruña, Nano Lett., 12 9 (2012) 4417-4423. <span>[5] S. Li, L. Burel, C. Aquino, A. Tuel, F. Morfin, J.L. Rousset, D. Farrusseng, Chem. Comm. 49 (2013) 8507-8509.

 


Thanks are due to CLYM (www.clym.fr) for guidance of the ETEM project financed by CNRS, Région Rhône-Alpes, ‘GrandLyon’ and French Ministry of Research and Higher Education. The authors thank N. Blanchard and C. Langlois for fruitful discussions and L. Burel for her assistance.

Fig. 1: Fast single-tilt tomography; a-b): video frames extracted at 78° and - 38.5° from a continuous tilting series acquired in bright field mode in less than 4 minutes; c): surface rendering of the silica-cages (green) and size histogram of Ag NPs (red); only 3% are outside of the silica cages. Acquisition conditions: high vacuum, 20°C, 300 kV.

Fig. 2: a): Assembly of silica cages containing Ag NPs at 20°C under high vacuum; b): same area at 700°C under high vacuum: the Ag NPs have grown but are mostly still inside the silica-cages; c): other area at 450°C under 2 10-2 mbar of O2 flow: note that all Ag NPs are out of the cages on the carbon supporting film, contrarily to b).