On the origin of primary 1/2 a0 <111> and a0 <100> loops in irradiated Fe(Cr) alloys

被引:70
|
作者
Schaublin, R. [1 ,2 ]
Decamps, B. [3 ]
Prokhodtseva, A. [4 ,5 ]
Loffler, J. F. [1 ]
机构
[1] Swiss Fed Inst Technol, Dept Mat, Lab Met Phys & Technol, CH-8093 Zurich, Switzerland
[2] Swiss Fed Inst Technol, Sci Ctr Opt & Electron Microscopy, CH-8093 Zurich, Switzerland
[3] Univ Paris Sud 11, CNRS IN2P3, CSNSM, UMR 8609, Bat 108, F-91405 Orsay, France
[4] EPFL, Ctr Rech Phys Plasmas, Assoc Euratom Confederat Suisse, CH-5232 Villigen, Switzerland
[5] FEI Czech Republ Sro, Vlastimila Pecha 12, Brno 62700, Czech Republic
基金
瑞士国家科学基金会;
关键词
Ultra-high purity Fe and Fe(Cr); Transmission electron microscopy; Radiation damage; Dislocation loops; Materials for future fusion reactor; PRIMARY DAMAGE FORMATION; HEAVY-ION IRRADIATIONS; FE-CR; DISLOCATION LOOPS; ALPHA-IRON; DEFECT ACCUMULATION; ELECTRON-MICROSCOPE; MOLECULAR-DYNAMICS; RADIATION-DAMAGE; THIN-FOILS;
D O I
10.1016/j.actamat.2017.02.041
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The radiation-induced primary dislocation loops in thin foils of ultra-high purity Fe and Fe(Cr) model alloys were investigated using ion irradiation in situ in a TEM. In the '111 mechanism' the induced nanometric loops of type a(0) <100> stem from mutual interaction of 1/2 a(0) <111> loops following their thermal diffusion. In the present work the conditions for this mechanism to occur are scrutinized. The effect of He, irradiation dose, dose rate, temperature and Cr content on the production of loops is assessed. Fe, Fe-5, -10 and -14Cr were irradiated with 500 keV Fe+ and 10 keV He+ ions up to 1 dpa and 1000 appm He at room and liquid nitrogen temperature. The initial loop population consists of 1/2 a(0) <111> and a(0) <100> loops, with no visible 1/2 a(0) <110>'s. Helium appears to stabilize 1/2 a(0) <111>'s by impeding their motion, as in its presence they are more numerous relative to a(0) <100>'s. At 1 dpa Cr plays a similar role. This is supported by (i) irradiations of Fe at three different dose rates, as only 1/2 a(0) <111>'s are observed after the fastest irradiation, and (ii) irradiation at liquid nitrogen temperature. The later leads to a majority of 1/2 a(0) <111>'s, while upon warming up to RT a(0) <100>'s become more numerous. All this supports the idea of the '111 mechanism'. However, surprisingly, at 0.05 dpa Cr actually favours the formation of a(0) <100> loops, irrespective of its influence on the mobility of the 1/2 a(0) <111>'s. (C) 2017 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.
引用
收藏
页码:427 / 439
页数:13
相关论文
共 50 条
  • [1] The elasticity of the 1/2 a0 <111> and a0 <100> dislocation loop in α-Fe thin foil
    Wu, Wenwang
    Schaublin, Robin
    JOURNAL OF NUCLEAR MATERIALS, 2018, 510 : 61 - 69
  • [2] Origin of A0, A1 and A3 conformational substates of carbonmonoxy myoglobin
    Stavrov, S. S.
    EUROPEAN BIOPHYSICS JOURNAL WITH BIOPHYSICS LETTERS, 2013, 42 : S106 - S106
  • [3] Rotational analysis of the H1(u)<-A0(g)(+/-) (1,0) bands of (Hg-202)(2)
    Czajkowski, A
    Kedzierski, W
    Atkinson, JB
    Krause, L
    JOURNAL OF MOLECULAR SPECTROSCOPY, 1997, 181 (01) : 1 - 10
  • [4] Improved full one-loop corrections to A0 → (q)over-tilde1(q)over-tilde2 and (q)over-tilde2 → (q)over-tilde1 A0
    Weber, C
    Eberl, H
    Majerotto, W
    PHYSICS LETTERS B, 2003, 572 (1-2) : 56 - 67
  • [6] On factorizable solution of the differential equation (f′)2=a0(z)(f-a1(z))2f
    Yuan, WJ
    He, YZ
    CHINESE SCIENCE BULLETIN, 1997, 42 (21): : 1779 - 1782
  • [7] THE ROTATIONALLY RESOLVED H1(U) [-A0(G)(+/-) ELECTRONIC-SPECTRUM OF HG-2
    CZAJKOWSKI, A
    KEDZIERSKI, W
    ATKINSON, JB
    KRAUSE, L
    CHEMICAL PHYSICS LETTERS, 1995, 238 (4-6) : 327 - 332
  • [8] Schrödinger Equation Solutions for the Central Field Power Potential Energy II. V(r) = −V0(r/a0)2ν−2, 0 ≤ ν ≤ 1, the Bound States
    Paul Caylor McKinney
    Journal of Mathematical Chemistry, 2002, 32 : 405 - 410
  • [9] Phonon density of states in Fe/Cr(0 0 1) superlattices and Tb-Fe thin-film alloys
    Sturhahn, W.
    Roehlsberger, R.
    Alp, E.E.
    Ruckert, T.
    Schrör, H.
    Keune, W.
    Journal of Magnetism and Magnetic Materials, 1999, 198 : 590 - 592
  • [10] Schrödinger Equation Solutions for the Central Field Power Potential Energy I. V(r) = V0(r/a0)2ν−2, ν ≥ 1
    Paul Caylor McKinney
    Journal of Mathematical Chemistry, 2002, 32 : 381 - 404