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Pure tungsten (W) is a primary plasm-facing material (PFM) candidate because of its superior properties, but it still has some drawbacks. In order to solve these problems, various methods have been used to improve the performances of tungsten-based materials. Potassium (K) doping, as one of the typical dispersion-strengthening methods for W materials, improves low temperature brittleness, reduces the ductile-brittle transition temperature, and suppresses the recrystallization. Meanwhile, it also improves the thermal shock resistance and fracture toughness of the material by introducing nano-sized K bubbles. However, this method brings a large number of defects inevitably. In fact, the K bubbles and the dislocations which are pinned by these K bubbles can affect the morphology and evolution of hydrogen (H) and helium (He) atoms in the alloys. As a very sensitive method to detect vacancy-type defects in materials, positron annihilation spectroscopy is used to study the irradiation damage caused by H and He atoms in this paper. The calculation of positron lifetime shows that positrons are more sensitive to the vacancy-type defects. Bounding of H and He with vacancies reduces the positron lifetime because of the increase of valence electron density. Combining the calculated results with the positron annihilation lifetime spectrum (PLAS) results shows that the W-K alloy is easier to promote the H atoms to release. Besides, it also more likely to form larger He bubbles which can be estimated by positron lifetime values. The result is also confirmed by the measurements from the scanning electron microscope (SEM) and slow positron Doppler broadening spectroscopy (DBS). The defects in the W-K alloy such as K bubbles and their pinned dislocations can act as diffusion channels to promote the H atoms to release, which gives rise to a smoother surface under the pure H irradiation. Meanwhile, under the condition of the H+6%He irradiation, the K bubbles and their pinned dislocations in the W-K alloy become the capture center of He atoms, promote their nucleation and grow into larger He bubbles. Moreover, under the action of stress and temperature gradient, some of the He bubbles migrate to the surface and release, this process is conducive to the recovery of related defects and the reduction of radiation damage.
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Keywords:
- positron annihilation spectroscopy /
- neutral beam irradiation /
- potassium-tungsten alloy /
- potassium doping
[1] Ueda Y, Coenen J W, Temmerman G D, Doerner R P, Tsitrone E 2014 Fusion Eng. Des. 89 901Google Scholar
[2] Gumbsch P, Riedle J, Hartmaier A, Fischmeister H F. 1998 Science. 282 1293Google Scholar
[3] Gumbsch P 2003 J. Nucl. Mater. 323 304Google Scholar
[4] Giannattasio A, Yao Z, Tarleton E, Roberts S G 2010 Philos Mag. 90 3947Google Scholar
[5] Rupp D, Weygand S M 2010 Philos Mag. 90 4055Google Scholar
[6] Bonnekoh C, Lied P, Pantleon W, Karcher T, Leiste H, Hoffmann A, Reiser J, Roeth M 2020 Int. J. Refract. Met. Hard Mater. 93 105347Google Scholar
[7] Zhang X X, Yan Q Z, Yang C T, Wang T N, Xia M, Ge C C 2016 Rare Metals. 35 566Google Scholar
[8] Levin Z S, Brady B G, Foley D C, Hartwing K T 2019 Int. J. Refract. Met. Hard Mater. 83 104966Google Scholar
[9] Fan J L, Liu T, Cheng H C, Wang D L 2008 J. Mater. Process. Techol. 208 463Google Scholar
[10] Shen Y, Xu Z, Cui K, Yu J 2014 J. Nucl. Mater. 455 234Google Scholar
[11] Zhang X, Yan Q, Lang S, Xia M, Liu X, Ge C 2014 J. Nucl. Mater. 455 537Google Scholar
[12] Guan W, Nogami S, Fukuda M, Hasegawa A 2016 Fusion Eng. Des. 109-111 1538
[13] Schade P 2013 Int. J. Refract. Met. Hard Mater. 28 648
[14] Nogami S, Watanabe S, Reiser J, Rieth M, Sickinger S, Hasegawa A 2019 Fusion Eng. Des. 140 48Google Scholar
[15] Huang B, Chen L Q, Qiu W B, Yang X L, Shi K, Lian Y Y, Liu X, Tang J 2019 J. Nucl. Mater. 520 1Google Scholar
[16] Feng F, Lian Y, Wang J, Chen Z, Huang B 2019 Tungsten. 1 1Google Scholar
[17] Zibrov M, Egger W, Heikinheimo J, Mayer M, Toumisto F 2020 J. Nucl. Mater. 531 152017Google Scholar
[18] Ramachandran R, David C, Magudapathy P, Rajaraman R, Govindaraj R, Amarendra G 2019 Fusion Eng. Des. 142 55
[19] Greuner H, Boeswirth B, Boscary J, Mcneely P 2007 J. Nucl. Mater. 367-370B 1444
[20] Feng F, Liu X, Lian Y, Greuner H, Böswirth B, Wang J B, Chen Z 2019 J. Nucl. Mater. 516 178Google Scholar
[21] 王少阶, 陈志权, 王波, 吴奕初, 方鹏飞, 张永学 著 2008 应用正电子谱学 (武汉: 湖北科学技术出版社) 第57页
Wang S J, Chen Z Q, Wang B, Wu Y C, Fang P F, Zhang Y X 2008 Applied Positron Spectroscopy (Wuhan: Hubei Science and Technology Press) p57 (in Chinese)
[22] Puska M J, Nieminen R M 1983 J. Phys. F:Met. Phys. 13 333Google Scholar
[23] Campillo Robles J M, Ogando E, Plazaola F 2007 J. Phys. Condens. Matter 19 176222Google Scholar
[24] Arponen J, Pajanne E 1978 Ann Phys. 121 343
[25] Boroński E, Nieminen R M 1986 Phys.l Rev. B. 34 3820Google Scholar
[26] Lantto, Lauri J 1987 Phys. Rev. B. 36 5160Google Scholar
[27] Kimball G E, Shortley G H 1934 Phys. Rev. 45 343Google Scholar
[28] Clark S J, Segall M D, Pickard C J, Hasnip P J, Probert M I J, Refson K, Payne M C 2005 Zeitschrift Für Krist. 220 567
[29] Vanderbilt D 1990 Phys. Rev. B 41 7892Google Scholar
[30] Perdew J P, Chevary J A, Vosko S H, Jackson K A, Pederson M R, Singh D J, Fiolhais C 1992 Phys. Rev. B 46 6671Google Scholar
[31] Ropo M, Kokko K, Vitos L 2008 Phys. Rev. B Condens. Matter 77 195445Google Scholar
[32] Monkhorst M J, Pack J D 1976 Phys. Rev. B 13 5188Google Scholar
[33] Temmerman G D, Bystrov K, Doerner R P, Marot L, Wright G M, Woller K B, Whyte D G, Zielinski J J 2013 J. Nucl. Mater. 438 S78Google Scholar
[34] Staikov P, Djourelov N 2013 Physica. B 413 59Google Scholar
[35] Puska M J, Lanki P, Nieminen R M 1989 J. Phys. Condens. Matter 1 6081Google Scholar
[36] Zhu T, Wang B Y, Song L G, Liu X H, Song Y M, Liu Y L, Zhang P, Cao X Z, Xu Q 2020 Int. J. Hydrog. Energy 45 15571Google Scholar
[37] Lee S C, Choi J H, Lee J G 2009 J. Nucl. Mater. 383 244Google Scholar
[38] Troev T, Popov E, Staikov P, Nankov N, Yoshiie T 2009 Nncl Instrum Meth B 267 535Google Scholar
[39] 王少阶, 陈志权, 王波, 吴奕初, 方鹏飞, 张永学 著 2008 应用正电子谱学 (武汉: 湖北科学技术出版社) 第77−78页
Wang S J, Chen Z Q, Wang B, Wu Y C, Fang P F, Zhang Y X 2008 Applied Positron Spectroscopy (Wuhan: Hubei Science and Technology Press) pp77−78 (in Chinese)
[40] Yabuuchi A, Tanaka M, Kinomura A 2020 J. Nucl. Mater. 542 152473Google Scholar
[41] Shu X Y, Huang B, Liu D P, Fan H Y, Liu N, Tang J 2017 Fusion Eng Des 117 8Google Scholar
[42] Toyama T, Ami K, Inoue K, Nagai Y, Sato K, Xu Q, Hatano Y 2018 J. Nucl. Mater. 499 464Google Scholar
[43] Keriem M S Abd E, Werf D P van der, Pleiter F 1993 Phys. Rev. B. 47 14771Google Scholar
[44] Jensen K O, Nieminen R M 1987 Phys. Rev. B. 36 8219Google Scholar
[45] Subrahmanyam V S, Nambissan P M G, Sen P 1994 Solid State Commun. 89 523Google Scholar
[46] Jensen K O, Eldrup M, Singh B N, Horsewell A, Victoria M, Sommer W F 1987 Mater Sci Forum. 15-18 913Google Scholar
[47] Wang S W, Guo W G, Yuan Y, Gao N, Zhu X L, Cheng L, Cao X Z, Fu E G, Shi L Q, Gao F, Lu G H 2020 J. Nucl. Mater. 532 152051Google Scholar
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图 1 样品SEM图 (a) 未辐照WK样品; (b) 未辐照PW样品; (c) 辐照样品WK1; (d) 辐照样品PW1; (e) 辐照样品WK2 (右上角为红框区域局部放大图); (f)辐照样品PW2(右上角同(e))
Figure 1. SEM images: (a) nonirradiated Sample of WK; (b) nonirradiated Sample of PW; (c) sample WK1; (d) sample PW1; (e) sample WK2 (The upper right corner is a partial enlargement of the red box area); (f) sample PW2 (The same as (e)).
图 2 正电子湮没分布 (a)位错; (b)位错中弥散有氢原子; (c)位错中存在一个空位; (d)空位中存在一个钾原子; (e)晶界; (f)晶界中存在一个空位
Figure 2. Positron annihilation distribution: (a) dislocation; (b) hydrogen atoms are scattered in the dislocation; (c) dislocation with a vacancy; (d) vacancy with a potassium at dislocation; (e) grain boundary; (f) grain boundary with a vacancy.
表 1 中性束辐照条件
Table 1. Conditions of neutral beam irradiation.
编号 样品
种类功率
/(MW·m–2)入射
粒子加速电
压/kV注量/
1024 m–2表面温
度/℃WK1 WK 10 H 29 3.4 1000 PW1 PW 10 H 29 3.4 1000 WK2 WK 8 H+6%He 27 6.7 800 PW2 PW 8 H+6%He 27 6.7 800 表 2 位错模型参数
Table 2. Detailed parameters of dislocations models.
Dislocation Type Slip plane(z) Bugers vector[b] Dislocation line[y] b-y Angle/(°) Intact/ps Vac.1/ps SCREW ($\bar{1}01$) (111)/2 ($\bar{1}2\bar1$) 90 106.5 196.4 EDGE ($\bar{1} 01$) (111)/2 (111) 0 133.9 197.2 表 3 晶界模型参数
Table 3. Detailed parameters of grain boundary model.
GB Type Σ GB Plane Rotation axis Angle/(°) Intact/ps Vac.1/ps TILT 5 {$0\bar{1} 5$} x (100) 22.61 142.2 204.8 表 4 辐照样品正电子寿命
Table 4. Positron lifetime of irradiated samples.
编号 $ {\tau }_{1} $/ps $ {I}_{1} $/% $ {\tau }_{2} $/ps $ {I}_{2} $/% $ {\tau }_{m} $/ps $ {\tau }_{1}^{\mathrm{c}\mathrm{a}\mathrm{l}} $/ps WK1 133.0 ± 1.8 62.1 ± 1.0 325.1 ± 3.5 38.0 ± 1.0 205.9 ± 2.4 92.79 WK2 132.1 ± 1.3 70.6 ± 0.7 360.4 ± 3.5 29.4 ± 0.7 199.2 ± 1.9 95.23 PW1 123.1 ± 1.3 70.8 ± 0.7 343.3 ± 3.3 29.2 ± 0.7 187.4 ± 1.8 94.22 PW2 144.0 ± 1.8 66.2 ± 1.0 340.4 ± 4.1 33.8 ± 1.0 210.3 ± 2.6 95.75 -
[1] Ueda Y, Coenen J W, Temmerman G D, Doerner R P, Tsitrone E 2014 Fusion Eng. Des. 89 901Google Scholar
[2] Gumbsch P, Riedle J, Hartmaier A, Fischmeister H F. 1998 Science. 282 1293Google Scholar
[3] Gumbsch P 2003 J. Nucl. Mater. 323 304Google Scholar
[4] Giannattasio A, Yao Z, Tarleton E, Roberts S G 2010 Philos Mag. 90 3947Google Scholar
[5] Rupp D, Weygand S M 2010 Philos Mag. 90 4055Google Scholar
[6] Bonnekoh C, Lied P, Pantleon W, Karcher T, Leiste H, Hoffmann A, Reiser J, Roeth M 2020 Int. J. Refract. Met. Hard Mater. 93 105347Google Scholar
[7] Zhang X X, Yan Q Z, Yang C T, Wang T N, Xia M, Ge C C 2016 Rare Metals. 35 566Google Scholar
[8] Levin Z S, Brady B G, Foley D C, Hartwing K T 2019 Int. J. Refract. Met. Hard Mater. 83 104966Google Scholar
[9] Fan J L, Liu T, Cheng H C, Wang D L 2008 J. Mater. Process. Techol. 208 463Google Scholar
[10] Shen Y, Xu Z, Cui K, Yu J 2014 J. Nucl. Mater. 455 234Google Scholar
[11] Zhang X, Yan Q, Lang S, Xia M, Liu X, Ge C 2014 J. Nucl. Mater. 455 537Google Scholar
[12] Guan W, Nogami S, Fukuda M, Hasegawa A 2016 Fusion Eng. Des. 109-111 1538
[13] Schade P 2013 Int. J. Refract. Met. Hard Mater. 28 648
[14] Nogami S, Watanabe S, Reiser J, Rieth M, Sickinger S, Hasegawa A 2019 Fusion Eng. Des. 140 48Google Scholar
[15] Huang B, Chen L Q, Qiu W B, Yang X L, Shi K, Lian Y Y, Liu X, Tang J 2019 J. Nucl. Mater. 520 1Google Scholar
[16] Feng F, Lian Y, Wang J, Chen Z, Huang B 2019 Tungsten. 1 1Google Scholar
[17] Zibrov M, Egger W, Heikinheimo J, Mayer M, Toumisto F 2020 J. Nucl. Mater. 531 152017Google Scholar
[18] Ramachandran R, David C, Magudapathy P, Rajaraman R, Govindaraj R, Amarendra G 2019 Fusion Eng. Des. 142 55
[19] Greuner H, Boeswirth B, Boscary J, Mcneely P 2007 J. Nucl. Mater. 367-370B 1444
[20] Feng F, Liu X, Lian Y, Greuner H, Böswirth B, Wang J B, Chen Z 2019 J. Nucl. Mater. 516 178Google Scholar
[21] 王少阶, 陈志权, 王波, 吴奕初, 方鹏飞, 张永学 著 2008 应用正电子谱学 (武汉: 湖北科学技术出版社) 第57页
Wang S J, Chen Z Q, Wang B, Wu Y C, Fang P F, Zhang Y X 2008 Applied Positron Spectroscopy (Wuhan: Hubei Science and Technology Press) p57 (in Chinese)
[22] Puska M J, Nieminen R M 1983 J. Phys. F:Met. Phys. 13 333Google Scholar
[23] Campillo Robles J M, Ogando E, Plazaola F 2007 J. Phys. Condens. Matter 19 176222Google Scholar
[24] Arponen J, Pajanne E 1978 Ann Phys. 121 343
[25] Boroński E, Nieminen R M 1986 Phys.l Rev. B. 34 3820Google Scholar
[26] Lantto, Lauri J 1987 Phys. Rev. B. 36 5160Google Scholar
[27] Kimball G E, Shortley G H 1934 Phys. Rev. 45 343Google Scholar
[28] Clark S J, Segall M D, Pickard C J, Hasnip P J, Probert M I J, Refson K, Payne M C 2005 Zeitschrift Für Krist. 220 567
[29] Vanderbilt D 1990 Phys. Rev. B 41 7892Google Scholar
[30] Perdew J P, Chevary J A, Vosko S H, Jackson K A, Pederson M R, Singh D J, Fiolhais C 1992 Phys. Rev. B 46 6671Google Scholar
[31] Ropo M, Kokko K, Vitos L 2008 Phys. Rev. B Condens. Matter 77 195445Google Scholar
[32] Monkhorst M J, Pack J D 1976 Phys. Rev. B 13 5188Google Scholar
[33] Temmerman G D, Bystrov K, Doerner R P, Marot L, Wright G M, Woller K B, Whyte D G, Zielinski J J 2013 J. Nucl. Mater. 438 S78Google Scholar
[34] Staikov P, Djourelov N 2013 Physica. B 413 59Google Scholar
[35] Puska M J, Lanki P, Nieminen R M 1989 J. Phys. Condens. Matter 1 6081Google Scholar
[36] Zhu T, Wang B Y, Song L G, Liu X H, Song Y M, Liu Y L, Zhang P, Cao X Z, Xu Q 2020 Int. J. Hydrog. Energy 45 15571Google Scholar
[37] Lee S C, Choi J H, Lee J G 2009 J. Nucl. Mater. 383 244Google Scholar
[38] Troev T, Popov E, Staikov P, Nankov N, Yoshiie T 2009 Nncl Instrum Meth B 267 535Google Scholar
[39] 王少阶, 陈志权, 王波, 吴奕初, 方鹏飞, 张永学 著 2008 应用正电子谱学 (武汉: 湖北科学技术出版社) 第77−78页
Wang S J, Chen Z Q, Wang B, Wu Y C, Fang P F, Zhang Y X 2008 Applied Positron Spectroscopy (Wuhan: Hubei Science and Technology Press) pp77−78 (in Chinese)
[40] Yabuuchi A, Tanaka M, Kinomura A 2020 J. Nucl. Mater. 542 152473Google Scholar
[41] Shu X Y, Huang B, Liu D P, Fan H Y, Liu N, Tang J 2017 Fusion Eng Des 117 8Google Scholar
[42] Toyama T, Ami K, Inoue K, Nagai Y, Sato K, Xu Q, Hatano Y 2018 J. Nucl. Mater. 499 464Google Scholar
[43] Keriem M S Abd E, Werf D P van der, Pleiter F 1993 Phys. Rev. B. 47 14771Google Scholar
[44] Jensen K O, Nieminen R M 1987 Phys. Rev. B. 36 8219Google Scholar
[45] Subrahmanyam V S, Nambissan P M G, Sen P 1994 Solid State Commun. 89 523Google Scholar
[46] Jensen K O, Eldrup M, Singh B N, Horsewell A, Victoria M, Sommer W F 1987 Mater Sci Forum. 15-18 913Google Scholar
[47] Wang S W, Guo W G, Yuan Y, Gao N, Zhu X L, Cheng L, Cao X Z, Fu E G, Shi L Q, Gao F, Lu G H 2020 J. Nucl. Mater. 532 152051Google Scholar
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