Analysis of depth-sectioning STEM for thick samples and 3D imaging

被引:36
作者
Bosch, Eric G. T. [1 ]
Lazic, Ivan [1 ]
机构
[1] Thermo Fisher Sci, Achtseweg,Noord 5, NL-5651 GG Eindhoven, Noord Brabant, Netherlands
关键词
STEM; Depth sectioning STEM; Thick samples; 3D imaging; iDPC-STEM; TRANSMISSION ELECTRON-MICROSCOPY; S-STATE MODEL; TOMOGRAPHY; RESOLUTION; CONTRAST; ATOMS; RECONSTRUCTION; PROSPECTS; CRYSTALS;
D O I
10.1016/j.ultramic.2019.112831
中图分类号
TH742 [显微镜];
学科分类号
摘要
We derive a model that describes 3D volume imaging in depth-sectioning STEM that is valid for all STEM techniques under three well-defined conditions: linearity, undisturbed probe and elastic scattering. The resulting undisturbed probe model generalizes the widely used idea that the undisturbed probe intensity in three dimensions can be used as the point spread function for depth-sectioning ADF-STEM to all STEM techniques including (A)BF- and iDPC-STEM. The model provides closed expressions for depth-sectioning STEM, which follow directly from the 2D expressions for thin samples, and thereby enables analysis of the 3D resolution. Using the model we explore the consequences of the resulting 3D contrast transfer function (CTF) for the z-resolution at different length scales and illustrate this with experiments. We investigate the validity and limitations of the model using multi-slice simulations showing that it is valid and quantitatively accurate for relatively thick amorphous samples but not for crystalline samples in zone-axis due to channeling. We compare depth-sectioning in iDPC and ADF-STEM and show that iDPC-STEM can extract information from deeper into the sample, all the way fill the bottom of the sample, thereby effectively allowing a thickness measurement. Also the difference in optimal focus conditions between iDPC- and ADF-STEM is explained. Finally, we propose practical criteria for deciding whether a sample is thin or thick.
引用
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页数:22
相关论文
共 42 条
[1]  
[Anonymous], 2010, ADV COMPUTING ELECT, DOI DOI 10.1007/978-1-4419-6533-2_12
[2]  
[Anonymous], 2011, ELECT ENERGY LOSS SP
[3]   STEM tomography for thick biological specimens [J].
Aoyama, Kazuhiro ;
Takagi, Tomoko ;
Hirase, Ai ;
Miyazawa, Atsuo .
ULTRAMICROSCOPY, 2008, 109 (01) :70-80
[4]   A new approach for electron tomography: Annular dark-field transmission electron microscopy [J].
Bals, S ;
Van Tendeloo, G ;
Kisielowski, C .
ADVANCED MATERIALS, 2006, 18 (07) :892-+
[5]   Three-dimensional imaging by optical sectioning in the aberration-corrected scanning transmission electron microscope [J].
Behan, G. ;
Cosgriff, E. C. ;
Kirkland, Angus I. ;
Nellist, Peter D. .
PHILOSOPHICAL TRANSACTIONS OF THE ROYAL SOCIETY A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 2009, 367 (1903) :3825-3844
[6]   Depth sectioning of aligned crystals with the aberration-corrected scanning transmission electron microscope [J].
Borisevich, Albina Y. ;
Lupini, Andrew R. ;
Travaglini, Samuel ;
Pennycook, Stephen J. .
JOURNAL OF ELECTRON MICROSCOPY, 2006, 55 (01) :7-12
[7]   Depth sectioning with the aberration-corrected scanning transmission electron microscope [J].
Borisevich, AY ;
Lupini, AR ;
Pennycook, SJ .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 2006, 103 (09) :3044-3048
[8]   Analysis of HR-STEM theory for thin specimen [J].
Bosch, Eric G. T. ;
Lazic, Ivan .
ULTRAMICROSCOPY, 2015, 156 :59-72
[9]   Large angle illumination enabling accurate structure reconstruction from thick samples in scanning transmission electron microscopy [J].
Brown, H. G. ;
Ishikawa, R. ;
S'anchez-Santolino, G. ;
Shibata, N. ;
Ikuhara, Y. ;
Allen, L. J. ;
Findlay, S. D. .
ULTRAMICROSCOPY, 2019, 197 :112-121
[10]   Three-dimensional imaging in double aberration-corrected scanning confocal electron microscopy, Part I: Elastic scattering [J].
Cosgriff, E. C. ;
D'Alfonso, A. J. ;
Allen, L. J. ;
Findlay, S. D. ;
Kirkland, A. I. ;
Nellist, P. D. .
ULTRAMICROSCOPY, 2008, 108 (12) :1558-1566