High-Resolution TEM. Williams, D. B. & Carter, C. B. In Williams, D. B. & Carter, C. B., editors, Transmission Electron Microscopy: A Textbook for Materials Science, volume 28, pages 483–509. Springer US, Boston, MA, 2009. ![High-Resolution TEM [link]](https://bibbase.org/img/filetypes/link.svg "link")
Paper doi abstract bibtex We will now rethink what we mean by a TEM, in a way that is more suitable for HRTEM, where the purpose is to maximize the useful detail in the image. (Note the word useful here.) You should think of the microscope as an optical device that transfers information from the specimen to the image. The optics consists of a series of lenses and apertures aligned along the optic (symmetry) axis. What we would like to do is to transfer all the information from the specimen to the image, a process known as mapping. There are two problems to overcome and we can never be completely successful in transferring all the information. First, as you know from Chapter 6, the lens system is not perfect so the image is distorted and you lose some data because the lens has a finite size (Abbe’s theory). The second problem is we have to interpret the image using an atomistic model for the material.
@incollection{williams_high-resolution_2009,
address = {Boston, MA},
title = {High-{Resolution} {TEM}},
volume = {28},
isbn = {978-0-387-76501-3},
url = {https://doi.org/10.1007/978-0-387-76501-3_28},
abstract = {We will now rethink what we mean by a TEM, in a way that is more suitable for HRTEM, where the purpose is to maximize the useful detail in the image. (Note the word useful here.) You should think of the microscope as an optical device that transfers information from the specimen to the image. The optics consists of a series of lenses and apertures aligned along the optic (symmetry) axis. What we would like to do is to transfer all the information from the specimen to the image, a process known as mapping. There are two problems to overcome and we can never be completely successful in transferring all the information. First, as you know from Chapter 6, the lens system is not perfect so the image is distorted and you lose some data because the lens has a finite size (Abbe’s theory). The second problem is we have to interpret the image using an atomistic model for the material.},
language = {en},
urldate = {2021-09-02},
booktitle = {Transmission {Electron} {Microscopy}: {A} {Textbook} for {Materials} {Science}},
publisher = {Springer US},
author = {Williams, David B. and Carter, C. Barry},
editor = {Williams, David B. and Carter, C. Barry},
year = {2009},
doi = {10.1007/978-0-387-76501-3_28},
keywords = {HRTEM Image, High Spatial Frequency, Objective Lens, Spherical Aberration, Transfer Function},
pages = {483--509},
}
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