Citation: | He Yudan, Jin Lei, Zhang Jiqiang, Luo Bingchi, Li Kai, Wu Weidong, Luo Jiangshan. Thickness dependence of microstructure and properties in Be2C coatings as a promising ablation material[J]. Matter and Radiation at Extremes, 2019, 4(4): 045403. doi: 10.1063/1.5087112 |
[1] |
K. Lan, J. Liu, Z. C. Li, X. F. Xie, W. Y. Huo et al., “Progress in octahedral spherical hohlraum study,” Matter Radiat. Extremes 1, 8–27 (2016).10.1016/j.mre.2016.01.003 doi: 10.1016/j.mre.2016.01.003
|
[2] |
B. A. Hammel1 and National Ignition Campaign Team, “The NIF ignition program: Progress and planning,” Plasma Phys. Controlled Fusion 48, B497–B506 (2006).10.1088/0741-3335/48/12b/s47 doi: 10.1088/0741-3335/48/12b/s47
|
[3] |
S. W. Haan, J. D. Lindl, D. A. Callahan, D. S. Clark, J. D. Salmonson, B. A. Hammel et al., “Point design targets, specifications, and requirements for the 2010 ignition campaign on the National Ignition Facility,” Phys. Plasmas 18, 051001 (2011).10.1063/1.3592169 doi: 10.1063/1.3592169
|
[4] |
A. L. Kritcher, D. Clark, S. Haan, S. A. Yi, A. B. Zylstra et al., “Comparison of plastic, high density carbon, and beryllium as indirect drive NIF ablators,” Phys. Plasmas 25, 056309 (2018).10.1063/1.5018000 doi: 10.1063/1.5018000
|
[5] |
D. S. Clark, A. L. Kritcher, S. A. Yi, A. B. Zylstra, S. W. Haan et al., “Capsule physics comparison of National Ignition Facility implosion designs using plastic, high density carbon, and beryllium ablators,” Phys. Plasmas 25, 032703 (2018).10.1063/1.5016874 doi: 10.1063/1.5016874
|
[6] |
J. L. Kline, S. A. Yi, A. N. Simakov, R. E. Olson, D. C. Wilson et al., “First beryllium capsule implosions on the National Ignition Facility,” Phys. Plasmas 23, 056310 (2016).10.1063/1.4948277 doi: 10.1063/1.4948277
|
[7] |
A. Nikroo, K. C. Chen, M. L. Hoppe, H. Huang, J. R. Wall, H. Xu et al., “Progress toward fabrication of graded doped beryllium and CH capsules for the National Ignition Facility,” Phys. Plasmas 13, 056302 (2006).10.1063/1.2179054 doi: 10.1063/1.2179054
|
[8] |
J. L. Kline and J. D. Hager, “Aluminum X-ray mass-ablation rate measurements,” Matter Radiat. Extremes 2, 16–21 (2017).10.1016/j.mre.2016.09.003 doi: 10.1016/j.mre.2016.09.003
|
[9] |
A. J. MacKinnon, N. B. Meezan, J. S. Ross, S. L. Pape, L. B. Hopkins, L. Divol et al., “High-density carbon ablator experiments on the National Ignition Facility,” Phys. Plasmas 21, 056318 (2014).10.1063/1.4876611 doi: 10.1063/1.4876611
|
[10] |
O. A. Hurricane, D. A. Callahan, D. T. Casey, P. M. Celliers, C. Cerjan et al., “Fuel gain exceeding unity in an inertially confined fusion implosion,” Nature 506, 343–348 (2014).10.1038/nature13008 doi: 10.1038/nature13008
|
[11] |
H. S. Park, O. A. Hurricane, D. A. Callahan, D. T. Casey, E. L. Dewald et al., “High-adiabat high-foot inertial confinement fusion implosion experiments on the National Ignition Facility,” Phys. Rev. Lett. 112, 055001 (2014).10.1103/physrevlett.112.055001 doi: 10.1103/physrevlett.112.055001
|
[12] |
Y. D. He, J. S. Luo, K. Li, B. C. Luo, J. Q. Zhang, W. D. Wu et al., “Influence of CH4–Ar ratios on the composition, microstructure and optical properties of Be2C films synthesized by DC reactive magnetron sputtering,” RSC Adv. 6, 39444–39451 (2016).10.1039/c6ra02141g doi: 10.1039/c6ra02141g
|
[13] |
Y. D. He, J. Q. Zhang, B. C. Luo, K. Li, L. Chen et al., “Effect of substrate temperature on the microstructure and properties of Be2C films: Aim to advance its applications as ICF ablator,” J. Alloys Compd. 728, 71–77 (2017).10.1016/j.jallcom.2017.08.185 doi: 10.1016/j.jallcom.2017.08.185
|
[14] |
W. S. Shih, Plasma-Deposited Beryllium Carbide Coatings for Application to Inertial Confinement Fusion (University of Missouri, Rolla, MO, 1997).
|
[15] |
Y. X. Xie, R. B. Stephens, N. C. Morosoff, and W. J. Jame, “A very suitable coating material for ICF capsule nonstoichiometric beryllium carbide composite,” J. Fusion Energy 17, 259–260 (1998).10.1023/a:1021822715909 doi: 10.1023/a:1021822715909
|
[16] |
E. H. Lundgren, A. C. Forsman, M. L. Hoppe, K. A. Moreno, and A. Nikroo, “Fabrication of pressurized 2 mm beryllium targets for ICF experiments,” Fusion Sci. Technol. 51, 576–580 (2007).10.13182/fst51-756 doi: 10.13182/fst51-756
|
[17] |
P. M. Vaghefi, A. Baghizadeh, M. G. Willinger, M. J. Pereira, D. A. Mota et al., “Thickness dependence of microstructure in thin La0.7Sr0.3MnO3 films grown on (100) SrTiO3 substrate,” J. Phys. D: Appl. Phys. 50, 395301 (2017).10.1088/1361-6463/aa80bf doi: 10.1088/1361-6463/aa80bf
|
[18] |
A. Namoune, T. Touam, and A. Chelouche, “Thickness, annealing and substrate effects on structural, morphological, optical and waveguiding properties of RF sputtered ZnO thin films,” J. Mater. Sci: Mater. Electron. 28, 12207–12219 (2017).10.1007/s10854-017-7036-x doi: 10.1007/s10854-017-7036-x
|
[19] |
Y. X. Xie, N. C. Morosoff, and W. J. James, “XPS characterization of beryllium carbide thin films formed via plasma deposition,” J. Nucl. Mater. 289, 48–51 (2001).10.1016/s0022-3115(00)00682-6 doi: 10.1016/s0022-3115(00)00682-6
|
[20] |
C. D. Wagner, W. M. Riggs, L. E. Davis, J. F. Moulder, and G. E. Muilenberg, Handbook of X-ray Photoelectron Spectroscopy (Perkin-Elmer Corporation, Physical Electronics Division, 1979).
|
[21] |
H. J. Bunge, Texture Analysis in Materials Science: Mathematical Methods (Elsevier, 2013).
|
[22] |
B. C. Luo, K. Li, X. L. Tan, J. Q. Zhang, J. S. Luo, W. D. Wu et al., “Influences of in situ annealing on microstructure, residual stress and electrical resistivity for sputter-deposited Be coating,” J. Alloys Compd. 607, 150–156 (2014).10.1016/j.jallcom.2014.03.128 doi: 10.1016/j.jallcom.2014.03.128
|
[23] |
J. Biener, D. D. Ho, C. Wild, E. Woerner, M. M. Biener, B. S. El-dasher et al., “Diamond spheres for inertial confinement fusion,” Nucl. Fusion 49, 112001 (2009).10.1088/0029-5515/49/11/112001 doi: 10.1088/0029-5515/49/11/112001
|
[24] |
J. D. Lindl, Inertial Confinement Fusion: The Quest for Ignition and Energy Gain Using Indirect Drive (AIP, 1998).
|
[25] |
B. C. Luo, L. Kai, X. L. Kai, J. Q. Zhang, Y. D. He, J. S. Luo et al., “Sputtering pressure influence on growth morphology, surface roughness, and electrical resistivity for strong anisotropy beryllium film,” Chin. Phys. B 23, 066804 (2014).10.1088/1674-1056/23/6/066804 doi: 10.1088/1674-1056/23/6/066804
|
[26] |
T. G. Mayerhöfer, H. Mutschke, and J. Popp, “Employing theories far beyond their limits—The case of the (Boguer-) Beer-Lambert law,” Chem. Phys. Chem. 17, 1948–1955 (2016).10.1002/cphc.201600114 doi: 10.1002/cphc.201600114
|
[27] |
J. Tauc and A. Menth, “States in the gap,” J. Non-Cryst. Solids 8(10), 569–585 (1972).10.1016/0022-3093(72)90194-9 doi: 10.1016/0022-3093(72)90194-9
|
[28] |
A. Dasa, A. K. Chikkala, G. P. Bharti, R. R. Behera, R. S. Mamilla, A. Khare et al., “Effect of thickness on optical and microwave dielectric properties of hydroxyapatite films deposited by RF magnetron sputtering,” J. Alloys Compd. 739, 729–736 (2018).10.1016/j.jallcom.2017.12.293 doi: 10.1016/j.jallcom.2017.12.293
|
[29] |
C. H. Lee, W. R. L. Lambrecht, and B. Segall, “Electronic structure of Be2C,” Phys. Rev. B 51(16), 10392–10398 (1995).10.1103/physrevb.51.10392 doi: 10.1103/physrevb.51.10392
|
[30] |
C. T. Tzeng, K. D. Tsuei, and W. S. Lo, “Experimental electronic structure of Be2C,” Phys. Rev. B 58(11), 6837–6843 (1998).10.1103/physrevb.58.6837 doi: 10.1103/physrevb.58.6837
|
[31] |
M. Zhang, M. J. Xu, M. K. Lia, Q. F. Zhang, Y. M. Lua, J. W. Chen et al., “SnO2 epitaxial films with varying thickness on c-sapphire: Structure evolution and optical band gap modulation,” Appl. Surf. Sci. 423, 611–618 (2017).10.1016/j.apsusc.2017.06.250 doi: 10.1016/j.apsusc.2017.06.250
|
[32] |
Y. Wang, W. Tang, J. Liu, and L. Zhang, “Stress-induced anomalous shift of optical band gap in Ga-doped ZnO thin films: Experimental and first-principles study,” Appl. Phys. Lett. 106, 162101 (2015).10.1063/1.4918933 doi: 10.1063/1.4918933
|