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Quantitative Analysis of Electron Beam Damage in Organic Thin Films
[Image: see text] In transmission electron microscopy (TEM) the interaction of an electron beam with polymers such as P3HT:PCBM photovoltaic nanocomposites results in electron beam damage, which is the most important factor limiting acquisition of structural or chemical data at high spatial resoluti...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2017
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5442601/ https://www.ncbi.nlm.nih.gov/pubmed/28553431 http://dx.doi.org/10.1021/acs.jpcc.7b01749 |
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author | Leijten, Zino J. W. A. Keizer, Arthur D. A. de With, Gijsbertus Friedrich, Heiner |
author_facet | Leijten, Zino J. W. A. Keizer, Arthur D. A. de With, Gijsbertus Friedrich, Heiner |
author_sort | Leijten, Zino J. W. A. |
collection | PubMed |
description | [Image: see text] In transmission electron microscopy (TEM) the interaction of an electron beam with polymers such as P3HT:PCBM photovoltaic nanocomposites results in electron beam damage, which is the most important factor limiting acquisition of structural or chemical data at high spatial resolution. Beam effects can vary depending on parameters such as electron dose rate, temperature during imaging, and the presence of water and oxygen in the sample. Furthermore, beam damage will occur at different length scales. To assess beam damage at the angstrom scale, we followed the intensity of P3HT and PCBM diffraction rings as a function of accumulated electron dose by acquiring dose series and varying the electron dose rate, sample preparation, and the temperature during acquisition. From this, we calculated a critical dose for diffraction experiments. In imaging mode, thin film deformation was assessed using the normalized cross-correlation coefficient, while mass loss was determined via changes in average intensity and standard deviation, also varying electron dose rate, sample preparation, and temperature during acquisition. The understanding of beam damage and the determination of critical electron doses provides a framework for future experiments to maximize the information content during the acquisition of images and diffraction patterns with (cryogenic) transmission electron microscopy. |
format | Online Article Text |
id | pubmed-5442601 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | American Chemical
Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-54426012017-05-26 Quantitative Analysis of Electron Beam Damage in Organic Thin Films Leijten, Zino J. W. A. Keizer, Arthur D. A. de With, Gijsbertus Friedrich, Heiner J Phys Chem C Nanomater Interfaces [Image: see text] In transmission electron microscopy (TEM) the interaction of an electron beam with polymers such as P3HT:PCBM photovoltaic nanocomposites results in electron beam damage, which is the most important factor limiting acquisition of structural or chemical data at high spatial resolution. Beam effects can vary depending on parameters such as electron dose rate, temperature during imaging, and the presence of water and oxygen in the sample. Furthermore, beam damage will occur at different length scales. To assess beam damage at the angstrom scale, we followed the intensity of P3HT and PCBM diffraction rings as a function of accumulated electron dose by acquiring dose series and varying the electron dose rate, sample preparation, and the temperature during acquisition. From this, we calculated a critical dose for diffraction experiments. In imaging mode, thin film deformation was assessed using the normalized cross-correlation coefficient, while mass loss was determined via changes in average intensity and standard deviation, also varying electron dose rate, sample preparation, and temperature during acquisition. The understanding of beam damage and the determination of critical electron doses provides a framework for future experiments to maximize the information content during the acquisition of images and diffraction patterns with (cryogenic) transmission electron microscopy. American Chemical Society 2017-05-09 2017-05-18 /pmc/articles/PMC5442601/ /pubmed/28553431 http://dx.doi.org/10.1021/acs.jpcc.7b01749 Text en Copyright © 2017 American Chemical Society This is an open access article published under a Creative Commons Non-Commercial No Derivative Works (CC-BY-NC-ND) Attribution License (http://pubs.acs.org/page/policy/authorchoice_ccbyncnd_termsofuse.html) , which permits copying and redistribution of the article, and creation of adaptations, all for non-commercial purposes. |
spellingShingle | Leijten, Zino J. W. A. Keizer, Arthur D. A. de With, Gijsbertus Friedrich, Heiner Quantitative Analysis of Electron Beam Damage in Organic Thin Films |
title | Quantitative Analysis of Electron Beam Damage in Organic
Thin Films |
title_full | Quantitative Analysis of Electron Beam Damage in Organic
Thin Films |
title_fullStr | Quantitative Analysis of Electron Beam Damage in Organic
Thin Films |
title_full_unstemmed | Quantitative Analysis of Electron Beam Damage in Organic
Thin Films |
title_short | Quantitative Analysis of Electron Beam Damage in Organic
Thin Films |
title_sort | quantitative analysis of electron beam damage in organic
thin films |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5442601/ https://www.ncbi.nlm.nih.gov/pubmed/28553431 http://dx.doi.org/10.1021/acs.jpcc.7b01749 |
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