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These pages provide an access point to data contained in CCFE published journal papers.  By selecting a paper, and then a specific figure or table, you can request the related underlying data if it is available for release.

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Publication Figures

Publication Date:
2017-03-03

First Author:
M. Yu. Lavrentiev

Title:
Chromium-vacancy clusters in dilute bcc Fe-Cr alloys: an ab initio study

Paper Identifier:
CP/17/25

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Figure Reference Title Description Number of Figure Data Items Identifier Download Figure Details
Figure 1e Figure 1. Configurations containing two (NN (a) and 2NN (b)), three (c) and four (d,e) vacancies investigated by ab initio calculations. Fe atoms are shown as light brown spheres, vacancies as grey spheres. 0 CF/17/26 Download
Figure 1a Figure 1a Figure 1. Configurations containing two (NN (a) and 2NN (b)), three (c) and four (d,e) vacancies investigated by ab initio calculations. Fe atoms are shown as light brown spheres, vacancies as grey spheres. 0 CF/17/27 Download
Figure 1b Figure 1. Configurations containing two (NN (a) and 2NN (b)), three (c) and four (d,e) vacancies investigated by ab initio calculations. Fe atoms are shown as light brown spheres, vacancies as grey spheres. 0 CF/17/28 Download
Figure 1c Figure 1. Configurations containing two (NN (a) and 2NN (b)), three (c) and four (d,e) vacancies investigated by ab initio calculations. Fe atoms are shown as light brown spheres, vacancies as grey spheres. 0 CF/17/29 Download
Figure 1d Figure 1. Configurations containing two (NN (a) and 2NN (b)), three (c) and four (d,e) vacancies investigated by ab initio calculations. Fe atoms are shown as light brown spheres, vacancies as grey spheres. 0 CF/17/30 Download
Figure 2 Figure 2. Magnetic moments (?B) of Fe atoms in the vicinity of a four vacancy cluster adopting a “square” configuration. 0 CF/17/31 Download
Figure 3 Figure 3. Binding energy Eb of vacancy-chromium clusters as a function of the number of Cr atoms in the first coordination shell around a vacancy (in eV). 0 CF/17/32 Download
Figure 4a Figure 4. Configurations with the highest binding energy, containing from 1 to 4 Cr atoms (green spheres) around a vacancy (grey sphere). 0 CF/17/33 Download
Figure 4b Figure 4. Configurations with the highest binding energy, containing from 1 to 4 Cr atoms (green spheres) around a vacancy (grey sphere). 0 CF/17/34 Download
Figure 4c Figure 4. Configurations with the highest binding energy, containing from 1 to 4 Cr atoms (green spheres) around a vacancy (grey sphere). 0 CF/17/35 Download
Figure 4d Figure 4. Configurations with the highest binding energy, containing from 1 to 4 Cr atoms (green spheres) around a vacancy (grey sphere). 0 CF/17/36 Download
Figure 5 Figure 5. Plot illustrating agreement between DFT binding energy data on single vacancy-Cr clusters and a linear fit with respect to the number of the nearest, third and fifth nearest Cr-Cr neighbours. 0 CF/17/37 Download
Figure 6 Figure 6. Average value of magnetic moment of Cr atoms (?B) around a single vacancy as a function of the binding energy of the cluster (eV). The straight line is a linear fit . 0 CF/17/38 Download
Figure 7a Figure 7. Configurations containing two vacancies in the nearest (a-c) or second (d-e) nearest neighbour position also containing a single Cr atom. 0 CF/17/39 Download
Figure 7b Figure 7. Configurations containing two vacancies in the nearest (a-c) or second (d-e) nearest neighbour position also containing a single Cr atom. 0 CF/17/40 Download
Figure 7c Figure 7. Configurations containing two vacancies in the nearest (a-c) or second (d-e) nearest neighbour position also containing a single Cr atom. 0 CF/17/41 Download
Figure 7d Figure 7. Configurations containing two vacancies in the nearest (a-c) or second (d-e) nearest neighbour position also containing a single Cr atom. 0 CF/17/42 Download
Figure 7e Figure 7. Configurations containing two vacancies in the nearest (a-c) or second (d-e) nearest neighbour position also containing a single Cr atom. 0 CF/17/43 Download
Figure 8a Figure 8. Lowest (a, c) and highest (b, d) energy configurations containing two vacancies and two Cr atoms. Vacancies are either in the nearest (a, b), or second nearest (c,d) neighbour position with respect to each other. 0 CF/17/44 Download
Figure 8b Figure 8. Lowest (a, c) and highest (b, d) energy configurations containing two vacancies and two Cr atoms. Vacancies are either in the nearest (a, b), or second nearest (c,d) neighbour position with respect to each other. 0 CF/17/45 Download
Figure 8c Figure 8. Lowest (a, c) and highest (b, d) energy configurations containing two vacancies and two Cr atoms. Vacancies are either in the nearest (a, b), or second nearest (c,d) neighbour position with respect to each other. 0 CF/17/46 Download
Figure 8d Figure 8. Lowest (a, c) and highest (b, d) energy configurations containing two vacancies and two Cr atoms. Vacancies are either in the nearest (a, b), or second nearest (c,d) neighbour position with respect to each other. 0 CF/17/47 Download
Figure 9 Figure 9. Average magnetic moment of a Cr atom (?B) in the vicinity of two vacancies as a function of the binding energy of the cluster (eV). 0 CF/17/48 Download
Table 1 Table 1. Binding energies of clusters of 2, 3, and 4 vacancies (eV) obtained in the present study and compared with calculations performed by others. Values in parentheses obtained in this work are calculated using larger simulation boxes containing 5×5×5 unit cells. In the paper by Masuda [11], the values in parentheses were obtained for unrelaxed atomic configurations. 0 CF/17/49 Download
Table 2 Table 2. Binding energies for vacancy-Cr pairs (eV) as functions of separation. 0 CF/17/50 Download
Formula 5 It is possible to approximate the binding energy of a single vacancy cluster containing from 1 to 8 Cr atoms by the following analytical linear expression (5) where N(2NN), N(3NN), N(5NN) are the numbers of the second, third and fifth nearest Cr-Cr neighbours in a configuration, respectively. 0 CF/17/51 Download

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    Culham Centre for Fusion Energy, Culham Science Centre, Abingdon, Oxfordshire, OX14 3DB, UK. This work is funded by the UK Engineering and Physical Sciences Research Council (EPSRC) and EURATOM

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