Abstract
The MeV electron irradiation by high-voltage electron microscopy (HVEM) can introduce the simplest type of irradiation defects in materials, and sometimes leads to a phase transition with negligible temperature change and contamination. This technique makes it possible to continuously observe the phase transition process using electron microscopy simultaneously as defects are introduced. Therefore, HVEM can provide a unique opportunity to carry out in-depth studies on the phase transition introduced by the accumulation of defects under a significantly simplified condition. In this paper, the following phase transitions related to non-equilibrium phases under MeV electron irradiation are discussed: (1) solid state amorphization (SSA) in metallic compounds, (2) crystallization of metallic glasses, and (3) crystal-to-amorphous-to-crystal (C–A–C) transition.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
References
Cohen MH, Turnbull D (1959) J Chem Phys 31:1164–1169
Cohen MH, Grest GS (1979) Phys Rev B 20:1077–1098
Egami T, Maeda K, Vitek V (1980) Philos Mag A 41:88–901
Egami T, Srolovitz D (1982) J Phys F Met Phys 12:2141–2164
Srolovitz D, Egami T, Vitek V (1982) Phys Rev B 24:6936–6944
Egami T, Maed K, Srolovitz D, Vitek V (1980) J Phys 41(C8):272–275
Egami T, Poon SJ, Zhang Z, Keppens V (2007) Phys Rev B 76:024203_1-024203_6
Fujita H (1989) J Electron Microsc Tech 3:243–304
Fujita H (1989) J Electron Microsc Tech 12:201–218
Seeger A (1999) J Electron Microsc 48:301–305
Mori H (2001) J Electron Microsc 60:S189–S197
Yasuda H (2011) Kenbikyo 46:160–164 (in Japanese)
Petrusenko Y, Bakai A, Borysenko V, Astakhov A, Barankov D (2009) Intermetallics 17:246–248
Nagase T, Hosokawa T, Umakoshi Y (2010) Intermetallics 18:767–772
Nagase T, Umakoshi Y (2010) Intermetallics 18:1803–1808
Ranganathan S (2003) Curr Sci 85:1404–1406
Cantor B, Chang ITH, Night PK, Vincent AJ (2004) Mater Sci Eng A 375:213–218
Yeh JW, Chen SK, Lin SJ, Gan JY, Chin TS, Shun TT, Tsau CH, Chang SY (2004) Adv Eng Mater 6:299–303
Nagase T, Sanda T, Nino A, Qin W, Yasuda H, Mori H, Umakoshi Y, Szpunar JA (2012) J Non-Cryst Solids 358:502–518
Urban K (1979) Phys Status Solidi A 56:157–168
Urban K (1980) Electron Microsc 4:188–195
Fujita H (1989) Hiheikou-zairyo no Riron to Gijyutsu-Seminar Text of Japan Inst Metals. JIM, Sendai 73–82 (in Japanese)
Seitz F, Koehler JS (1956) In: Seitz F, Tumbull D (eds) Solid state physics, vol 2. Academic, New York
Corbett JW (1966) Electron radiation damage in semiconductors and metals. Academic, New York
Oen OS (1988) Nucl Instrum Methods Phys Res B 33:744–747
Carpenter GJC, Schulson EM (1981) Scr Metall 15:549–554
Carpenter GJC, Schulson EM (1978) J Nucl Mater 73:180–189
Yasuda H, Mori H (1999) J Electron Microsc 48:581–584
Mori H, Fujita H (1982) Jpn J Appl Phys 21:L494–L496
Thomas G, Mori H, Fujita H, Sinclair R (1982) Scr Metall 16:589–592
Mogro-Campero A, Hall EL, Walter JL, Ratkowski AJ (1982) In: Picraux ST, Choyke WJ (eds) Metastable materials formation by ion-implantation. North-Holland, New York, pp 203–208
Mori H, Fujita H (1991) Ultramicroscopy 39:355–360
Nagase T, Sasaki A, Yasuda HY, Mori H, Terai T, Kakeshita T (2011) Intermetallics 19:1313–1318
Nagase T, Takizawa K, Wakeda M, Shibutani Y, Umakoshi Y (2010) Intermetallics 18:441–450
Suryanarayana C (2001) Prog Mater Sci 46:1–84
Mizutani U, Hoshino Y, Yamada H (1986) Amorphous-Gokin Sakusei no Tebiki. Agne, Tokyo (in Japanese)
Mori H (1993) In: Sakurai Y, Hamakawa Y, Masumoto T, Shirae K, Suzuki K (eds) Current topics in amorphous materials, physics and technology. Elsevier Science, Amsterdam, pp 120–126
Sakata T, Mori H, Fujita H (1989) J Chem Soc Jpn Int 97:1382–1388
Mori H, Fujita H (1992) In: Yavari AR (ed) Electron irradiation induced crystal-to-amorphous transition in metallic and non-metallic compounds in ordering and disordering in alloys. Applied Science, London, pp 277–286
Inui H, Mori H, Fujita H (1989) Acta Mater 37:1337–1342
Okamoto PR, Lam NQ, Rehn LE (1999) Physics of crystal-to-glass transformations. In: Ehrenreich H, Spaepen F (eds) Solid state physics, vol 52. Academic, San Diego
Takeuchi A, Inoue A (2000) Mater Trans 41:1372–1378
Takeuchi A, Inoue A (2005) Mater Trans 46:2817–2829
Nagase T, Hosokawa T, Takizawa K, Umakoshi Y (2009) Intermetallics 17:657–668
Nagase T, Umakoshi Y (2003) Scr Mater 48:1237–1242
Nagase T, Umakoshi Y, Sumida N (2002) Mater Sci Eng A 323:218–225
Nagase T, Nino A, Hosokawa T, Umakoshi Y (2007) Mater Trans 48:1651–1658
Anada S, Nagase T, Yasuda H, Mori H (to be submitted)
Imafuku M, Sato S, Koshiba H, Matsubara E, Inoue A (2000) Mater Trans JIM 41:1526–1529
Acknowledgments
This study was supported by Priority Assistance for the Formation of Worldwide Renowned Centers of Research—The Global COE Program (Project: Center of Excellence for Advanced Structural and Functional Materials Design) of the Ministry of Education, Culture, Sports, Science and Technology, Japan. The author greatly thanks Prof. H. Mori and Prof. Y. Umakoshi in Osaka University for the fruitful discussions, valuable suggestions, and comments. Many experimental results about irradiation-induced amorphization and crystallization were obtained by Dr. A. Nino in Akita University, Dr. W. Qin in University of Saskatchewan, T. Hosokawa, A. Sasaki and T. Sanda. The recent experimental results about the irradiation-induced C–A–C transition were obtained by S. Anada in Osaka University.
Author information
Authors and Affiliations
Corresponding author
Editor information
Editors and Affiliations
Appendix: Technical Terms
Appendix: Technical Terms
-
(1)
Anti-free volume-like defect [6, 13–15]
-
In an amorphous phase, not only vacancy-type defects but also interstitial-type defects can be considered, as shown in Fig. 12.1a. Anti-free volume-like defects correspond to interstitial-type defects. Petrusenko et al. reported MeV electron irradiation damage and suggested the existence of vacancy-type defects and interstitial-type defects in metallic glasses based on the experimental results. The recovery of introduced defects in metallic glasses has two threshold temperatures because of the changes in the relaxation mechanism under 298 K: the first was related to with complexes containing interstitial-type defects in metallic glass, while the second was a result of the relaxation of vacancy-containing complexes [14].
-
-
(2)
High-entropy materials (HE materials) [16–18]
-
This class of alloys consists of multi-component materials with an approximately equiatomic ratio of components. Thus, these alloys have a high entropy of mixing, which distinguishes them from conventional alloys. Solid solutions with multi-principal elements have generally been found to be more stable than intermetallic compounds at elevated temperatures because of their large entropies of mixing. Some researchers have defined a high-entropy material as one that has at least five principal elements, each of which has an atomic concentration between 5 % and 35 %; for example, the Fe20Ni20Cu20Co20Cr20 alloy.
-
Rights and permissions
Copyright information
© 2013 Springer Japan
About this chapter
Cite this chapter
Nagase, T. (2013). Advanced Materials Design by Irradiation of High Energy Particles. In: Kakeshita, T. (eds) Progress in Advanced Structural and Functional Materials Design. Springer, Tokyo. https://doi.org/10.1007/978-4-431-54064-9_12
Download citation
DOI: https://doi.org/10.1007/978-4-431-54064-9_12
Published:
Publisher Name: Springer, Tokyo
Print ISBN: 978-4-431-54063-2
Online ISBN: 978-4-431-54064-9
eBook Packages: Chemistry and Materials ScienceChemistry and Material Science (R0)