Direct observation of mono-vacancy and self-interstitial recovery in tungsten
Source abstract
Abstract
Reliable and accurate knowledge of the physical properties of elementary point defects is crucial for predictive modeling of the evolution of radiation damage in materials employed in harsh conditions. We have applied positron annihilation spectroscopy to directly detect mono-vacancy defects created in tungsten through particle irradiation at cryogenic temperatures, as well as their recovery kinetics. We find that efficient self-healing of the primary damage takes place through Frenkel pair recombination already at 35 K, in line with an upper bound of 0.1 eV for the migration barrier of self-interstitials. Further self-interstitial migration is observed above 50 K with activation energies in the range of 0.12–0.42 eV through the release of the self-interstitial atoms from impurities and structural defects and following recombination with mono-vacancies. Mono-vacancy migration is activated at around 550 K with a migration barrier of EmV=1.85±0.05 eV.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Fusion materials and technologies · Nuclear materials and radiation effects · Muon and positron interactions and applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Applied Physics, Aalto University 1 , P.O. Box 15100, FI-00076 Aalto, Finland
Department of Physics, University of Helsinki 2 , P.O. Box 43, FI-00014 Helsinki, Finland
IPFN, Instituto Superior Técnico, Universidade de Lisboa 3 , 1049-001 Lisboa, Portugal
Funding
Academy of Finland
References (36)
Show source-provided references
1. Science · 2010 · 327 · 158710.1126/science.1188088 ↗
2. Science · 2007 · 318 · 95610.1126/science.1145386 ↗
3. Phys. Rev. B · 2011 · 84 · 10410910.1103/physrevb.84.104109 ↗
4. Nat. Commun. · 2013 · 4 · 228810.1038/ncomms3288 ↗
5. Appl. Phys. Lett. · 1999 · 74 · 272010.1063/1.123948 ↗
6. Scr. Mater. · 2015 · 94 · 110.1016/j.scriptamat.2014.07.020 ↗
7. Phys. Rev. Lett. · 2016 · 116 · 13550410.1103/physrevlett.116.135504 ↗
8. Phys. Rev. Lett. · 2016 · 116 · 24550110.1103/physrevlett.116.245501 ↗
9. Phys. Rev. Lett. · 2017 · 118 · 20550110.1103/physrevlett.118.205501 ↗
10. J. Nucl. Mater. · 2009 · 390-391 · 110.1016/j.jnucmat.2009.01.037 ↗
11. Radiat. Eff. · 1978 · 38 · 5310.1080/00337577808233209 ↗
12. Philos. Mag. Lett. · 2011 · 91 · 8610.1080/09500839.2010.533133 ↗
13. Sci. Rep. · 2016 · 6 · 2609910.1038/srep26099 ↗
14. J. Nucl. Mater. · 2008 · 376 · 21610.1016/j.jnucmat.2008.03.002 ↗
15. Phys. Status Solidi C · 2009 · 6 · 232910.1002/pssc.200982114 ↗
16. J. Nucl. Mater. · 2013 · 433 · 30510.1016/j.jnucmat.2012.09.001 ↗
17. J. Nucl. Mater. · 2015 · 463 · 100910.1016/j.jnucmat.2014.11.033 ↗
18. Rev. Mod. Phys. · 2013 · 85 · 158310.1103/revmodphys.85.1583 ↗
19. Nucl. Instrum. Methods Phys. Res., Sect. A · 2007 · 572 · 97810.1016/j.nima.2006.11.065 ↗
20. Nucl. Instrum. Methods Phys. Res., Sect. A · 2005 · 538 · 77810.1016/j.nima.2004.08.102 ↗
21. Phys. Rev. B · 1995 · 52 · 811210.1103/physrevb.52.8112 ↗
22. Phys. Rev. B · 2011 · 83 · 23521210.1103/physrevb.83.235212 ↗
23. Phys. Rev. B · 2017 · 95 · 18410310.1103/physrevb.95.184103 ↗
24. J. Phys. IV France · 1995 · 05 · C1-13510.1051/jp4:1995115 ↗
25. Radiat. Eff. Defects Solids · 1992 · 124 · 21510.1080/10420159208220193 ↗
26. Nucl. Instrum. Methods Phys. Res., Sect. B · 2009 · 267 · 53510.1016/j.nimb.2008.11.045 ↗
27. 1995
28. Stavola · 1998 · 209
29. 1988
30. Philos. Mag. A · 1980 · 41 · 9110.1080/01418618008241833 ↗
31. J. Phys.: Condens. Matter · 2015 · 27 · 25500710.1088/0953-8984/27/25/255007 ↗
32. Phys. Rev. B · 2010 · 82 · 09410210.1103/physrevb.82.094102 ↗
33. Phys. Rev. B · 2006 · 73 · 02010110.1103/physrevb.73.020101 ↗
34. Phys. Rev. Lett. · 2008 · 101 · 11550410.1103/physrevlett.101.115504 ↗
35. J. Phys.: Condens. Matter · 2014 · 26 · 37570110.1088/0953-8984/26/37/375701 ↗
36. Nucl. Instrum. Methods Phys. Res., Sect. B · 2010 · 268 · 181810.1016/j.nimb.2010.02.091 ↗