Journal of Inorganic Materials ›› 2022, Vol. 37 ›› Issue (1): 51-57.DOI: 10.15541/jim20210179
Special Issue: 【材料计算】计算材料(202409)
• RESEARCH ARTICLE • Previous Articles Next Articles
PENG Junhui1,2(), TIKHONOV Evgenii1(
)
Received:
2021-03-20
Revised:
2021-04-30
Published:
2022-01-20
Online:
2021-12-30
Contact:
TIKHONOV Evgenii, assistant professor. E-mail: tikhonov.e@nwpu.edu.cn
About author:
PENG Junhui(1989-), male, PhD candidate. E-mail: pjh1989@yeah.net
Supported by:
CLC Number:
PENG Junhui, TIKHONOV Evgenii. Vacancy on Structures, Mechanical and Electronic Properties of Ternary Hf-Ta-C System: a First-principles Study[J]. Journal of Inorganic Materials, 2022, 37(1): 51-57.
Fig. 1 Crystal structure prediction and (Hf, Ta)C1-x vacancy ordered structure (a) Enthalpy convex-hull of ternary Hf-Ta-C system (black sphere indicating stable structure, while others indicating metastable structure, and red square representing the structure with high enthalpy above the convex-hull, but not considered here); (b) Simulated X-ray diffractions of (Hf, Ta)C1-x vacancy ordered structures with a copper Kα X-ray source
Compound | Space group | Lattice constants/nm | Above convex-hull /(eV·atom-1) | ΔHf /(eV·atom-1) | CN | x |
---|---|---|---|---|---|---|
Hf5TaC5 | Cm | a=0.567, b=0.976, c=0.929, β=145.1° | 0 | -0.8925 | 5, 5 | 1/6 |
Hf3TaC3 | P-1 | a=0.567, b=0.648, c=0.565 α=89.4°, β=69.6°, γ=91.3° | 0.0007 | -0.8408 | 5/4, 4 | 1/4 |
Hf6Ta2C7 | P-1 | a=0.565, b=0.562, c=0.653 α=90.4°, β=72.4°, γ=99.8° | 0 | -0.8868 | 6/5, 5 | 1/8 |
Hf2TaC2 | P-1 | a=0.566, b=0.554, c=0.560 α=119.4°, β=98.4°, γ=102.4° | 0.0012 | -0.7842 | 4, 4 | 1/3 |
Hf4Ta2C5 | P-1 | a=0.559, b=0.561, c=0.559 α=109.1°, β=100.1°, γ=60.3° | 0 | -0.8604 | 5, 5 | 1/6 |
Hf3Ta3C5 | Cm | a=0.558, b=0.963, c=0.644, β=125.2° | 0.0009 | -0.8161 | 5, 5 | 1/6 |
Hf2Ta4C5 | C2/m | a=0.551, b=0.963, c=0.551, β=71.3° | 0 | -0.7735 | 5, 5 | 1/6 |
HfTa5C5 | Cm | a=0.548, b=0.954, c=0.548, β=109.2° | 0 | -0.7033 | 5, 5 | 1/6 |
Table 1 Space groups, lattice constants, enthalpy above the convex-hull, formation enthalpy (ΔHf), concentration of vacancy (x) and coordination number (CN) of Hf or Ta for ternary (Hf, Ta)C1-x vacancy ordered structures
Compound | Space group | Lattice constants/nm | Above convex-hull /(eV·atom-1) | ΔHf /(eV·atom-1) | CN | x |
---|---|---|---|---|---|---|
Hf5TaC5 | Cm | a=0.567, b=0.976, c=0.929, β=145.1° | 0 | -0.8925 | 5, 5 | 1/6 |
Hf3TaC3 | P-1 | a=0.567, b=0.648, c=0.565 α=89.4°, β=69.6°, γ=91.3° | 0.0007 | -0.8408 | 5/4, 4 | 1/4 |
Hf6Ta2C7 | P-1 | a=0.565, b=0.562, c=0.653 α=90.4°, β=72.4°, γ=99.8° | 0 | -0.8868 | 6/5, 5 | 1/8 |
Hf2TaC2 | P-1 | a=0.566, b=0.554, c=0.560 α=119.4°, β=98.4°, γ=102.4° | 0.0012 | -0.7842 | 4, 4 | 1/3 |
Hf4Ta2C5 | P-1 | a=0.559, b=0.561, c=0.559 α=109.1°, β=100.1°, γ=60.3° | 0 | -0.8604 | 5, 5 | 1/6 |
Hf3Ta3C5 | Cm | a=0.558, b=0.963, c=0.644, β=125.2° | 0.0009 | -0.8161 | 5, 5 | 1/6 |
Hf2Ta4C5 | C2/m | a=0.551, b=0.963, c=0.551, β=71.3° | 0 | -0.7735 | 5, 5 | 1/6 |
HfTa5C5 | Cm | a=0.548, b=0.954, c=0.548, β=109.2° | 0 | -0.7033 | 5, 5 | 1/6 |
Compound | C11 /GPa | C22 /GPa | C33 /GPa | C44 /GPa | C55 /GPa | C66 /GPa | C12 /GPa | C13 /GPa | C23 /GPa | B /GPa | G /GPa | E /GPa | Hv /GPa | G/B | μ |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Hf5TaC5 | 422.9 | 446.8 | 432.1 | 177.0 | 177.0 | 156.1 | 105.3 | 129.0 | 122.5 | 223.8 | 162.7 | 393.0 | 24.09 | 0.7271 | 0.2074 |
Hf3TaC3 | 382.3 | 407.8 | 403.3 | 156.7 | 156.7 | 121.6 | 102.9 | 123.1 | 121.8 | 209.3 | 141.4 | 346.1 | 19.88 | 0.6754 | 0.2244 |
Hf6Ta2C7 | 454.5 | 482.0 | 472.3 | 180.9 | 180.9 | 171.3 | 122.2 | 135.9 | 114.0 | 239.1 | 170.6 | 413.4 | 24.23 | 0.7133 | 0.2119 |
Hf2TaC2 | 365.7 | 399.7 | 384.9 | 136.2 | 136.2 | 108.5 | 121.0 | 118.9 | 112.0 | 205.7 | 128.8 | 319.8 | 16.85 | 0.6265 | 0.2409 |
Hf4Ta2C5 | 443.4 | 423.5 | 441.2 | 175.4 | 175.4 | 160.2 | 122.8 | 135.9 | 140.4 | 233.9 | 162.6 | 395.9 | 22.68 | 0.6949 | 0.2179 |
Hf3Ta3C5 | 431.3 | 443.6 | 433.6 | 185.4 | 185.4 | 153.1 | 129.2 | 149.3 | 154.0 | 241.4 | 157.2 | 387.5 | 20.34 | 0.6513 | 0.2325 |
Hf2Ta4C5 | 476.5 | 446.7 | 477.6 | 199.4 | 199.4 | 161.1 | 141.9 | 163.7 | 155.6 | 257.9 | 168.3 | 414.6 | 21.34 | 0.6525 | 0.2320 |
HfTa5C5 | 491.9 | 473.8 | 484.4 | 209.8 | 209.8 | 171.5 | 149.6 | 165.6 | 166.9 | 268.2 | 175.7 | 432.6 | 22.08 | 0.6551 | 0.2312 |
Table 2 Calculated elastic constants (Cij) and mechanical properties-bulk modulus (B), shear modulus (G/), elastic modulus (E), Poisson’s ratio (μ), Vickers hardness (Hv) and Pugh’s ratio (G/B) of (Hf, Ta)C1-x vacancy ordered structures
Compound | C11 /GPa | C22 /GPa | C33 /GPa | C44 /GPa | C55 /GPa | C66 /GPa | C12 /GPa | C13 /GPa | C23 /GPa | B /GPa | G /GPa | E /GPa | Hv /GPa | G/B | μ |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Hf5TaC5 | 422.9 | 446.8 | 432.1 | 177.0 | 177.0 | 156.1 | 105.3 | 129.0 | 122.5 | 223.8 | 162.7 | 393.0 | 24.09 | 0.7271 | 0.2074 |
Hf3TaC3 | 382.3 | 407.8 | 403.3 | 156.7 | 156.7 | 121.6 | 102.9 | 123.1 | 121.8 | 209.3 | 141.4 | 346.1 | 19.88 | 0.6754 | 0.2244 |
Hf6Ta2C7 | 454.5 | 482.0 | 472.3 | 180.9 | 180.9 | 171.3 | 122.2 | 135.9 | 114.0 | 239.1 | 170.6 | 413.4 | 24.23 | 0.7133 | 0.2119 |
Hf2TaC2 | 365.7 | 399.7 | 384.9 | 136.2 | 136.2 | 108.5 | 121.0 | 118.9 | 112.0 | 205.7 | 128.8 | 319.8 | 16.85 | 0.6265 | 0.2409 |
Hf4Ta2C5 | 443.4 | 423.5 | 441.2 | 175.4 | 175.4 | 160.2 | 122.8 | 135.9 | 140.4 | 233.9 | 162.6 | 395.9 | 22.68 | 0.6949 | 0.2179 |
Hf3Ta3C5 | 431.3 | 443.6 | 433.6 | 185.4 | 185.4 | 153.1 | 129.2 | 149.3 | 154.0 | 241.4 | 157.2 | 387.5 | 20.34 | 0.6513 | 0.2325 |
Hf2Ta4C5 | 476.5 | 446.7 | 477.6 | 199.4 | 199.4 | 161.1 | 141.9 | 163.7 | 155.6 | 257.9 | 168.3 | 414.6 | 21.34 | 0.6525 | 0.2320 |
HfTa5C5 | 491.9 | 473.8 | 484.4 | 209.8 | 209.8 | 171.5 | 149.6 | 165.6 | 166.9 | 268.2 | 175.7 | 432.6 | 22.08 | 0.6551 | 0.2312 |
Fig. 2 Phonon dispersion curves of (a) Hf5TaC5, (b) Hf3TaC3, (c) Hf6Ta2C7, (d) Hf2TaC2, (e) Hf4Ta2C5, (f) Hf3Ta3C5, (g) Hf2Ta4C5, and (h) HfTa5C5 They are all dynamical stable because no imaginary frequencies were found in Brillouin zone
Fig. 3 Crystal structures of (a) Hf5TaC5, (b) Hf3TaC3, (c) Hf6Ta2C7, (d) Hf2TaC2, (e) Hf4Ta2C5, (f) Hf3Ta3C5, (g) Hf2Ta4C5, and (h) HfTa5C5 All sharing the rock-salt structure; Black square represents the structural vacancy
Fig. 4 Effect of vacancy on mechanical properties for ternary Hf-Ta-C system (a) Bulk modulus (B); (b) Shear modulus (G); (c) Elastic modulus (E); (d) Vickers hardness (HV); (e) Pugh’s ratio (G/B); (f) Poisson’s ratio (μ)
Fig. 5 Density of state (DOS) and partial DOS (PDOS) normalized by per (Hf, Ta)C1-x of (a) Hf5TaC5, (b) Hf3TaC3, (c) Hf6Ta2C7, (d) Hf2TaC2, (e) Hf4Ta2C5, (f) Hf3Ta3C5, (g) Hf2Ta4C5, and (h) HfTa5C5(The Fermi level being set at 0 eV) DOS is density of state / (states/eV); TDOS is total DOS; Hf, Ta, C are PDOS of Hf atom, Ta atom and C atom, respectively Colorful figures are available on the website
[1] |
KURBATKINA V V, PATSERA E I, LEVASHOV E A, et al. Self-propagating high-temperature synthesis of single-phase binary tantalum-hafnium carbide (Ta, Hf)C and its consolidation by hot pressing and spark plasma sintering. Ceramics International, 2018, 44(4):4320-4329.
DOI URL |
[2] | ANDRIEVSKII R A, STRELNIKOVA N S, POLTORATSKII N I, et al. Melting point in systems ZrC-HfC, TaC-ZrC, TaC-HfC. Powder Metallurgy and Metal Ceramics, 1967, 6:65-67. |
[3] | RUDY E. Ternary phase equilibria in transition metal-boron- carbon-silicon systems. Part II. Ternary systems, Vol. I. Air Force Materials Laboratory: Wright-Patterson Air Force Base, 1965: 35-73. |
[4] |
CEDILLOS-BARRAZA O, MANARA D, BOBORIDIS K, et al. Investigating the highest melting temperature materials: a laser melting study of the TaC-HfC system. Scientific Reports, 2016, 6:37962.
DOI URL |
[5] |
ZHANG X H, HILMAS G E, FAHRENHOLTZ W G, et al. Hot pressing of tantalum carbide with and without sintering additives. Journal of the American Ceramic Society, 2007, 90(2):393-401.
DOI URL |
[6] |
CEDILLOS-BARRAZA O, GRASSO S, NASIRI N A, et al. Sintering behaviour, solid solution formation and characterisation of TaC, HfC and TaC-HfC fabricated by spark plasma sintering. Journal of the European Ceramic Society, 2016, 36(7):1539-1548.
DOI URL |
[7] |
SMITH C J, YU X X, GUO Q, et al. Phase, hardness, and deformation slip behavior in mixed HfxTa1-xC. Acta Materialia, 2018, 145:142-153.
DOI URL |
[8] |
PENG J, TIKHONOV E. xTaxC and HfC1-xNx. Computational Materials Science, 2021, 195:110464.
DOI URL |
[9] |
ZHANG J, WANG S, LI W. Consolidation and characterization of highly dense single-phase Ta-Hf-C solid solution ceramics. Journal of the American Ceramic Society, 2019, 102:58-62.
DOI URL |
[10] |
GABALLA O, COOK B A, RUSSELL A M. Reduced-temperature processing and consolidation of ultra-refractory Ta4HfC5. International Journal of Refractory Metals and Hard Materials, 2013, 41:293-299.
DOI URL |
[11] |
GHAFFARI S A, FAGHIHI-SANI M A, GOLESTANI-FARD F, et al. Spark plasma sintering of TaC-HfC UHTC via disilicides sintering aids. Journal of the European Ceramic Society, 2013, 33(8):1479-1484.
DOI URL |
[12] |
PABLO G, LUIS Y, MERCY S, et al. Characterization of the micro-abrasive wear in coatings of TaC-HfC/Au for biomedical implants. Materials, 2017, 10(8):842.
DOI URL |
[13] |
ZHANG C, GUPTA A, SEAL S, et al. Solid solution synthesis of tantalum carbide-hafnium carbide by spark plasma sintering. Journal of the American Ceramic Society, 2017, 100:1853-1862.
DOI URL |
[14] |
FOROUGHI P, ZHANG C, AGARWAL A, et al. Controlling phase separation of TaxHf1-xC solid solution nanopowders during carbothermal reduction synthesis. Journal of the American Ceramic Society, 2017, 100:5056-5065.
DOI URL |
[15] |
KIM J, KWON H, KIM B, et al. Finite temperature thermal expansion and elastic properties of (Hf1-xTax)C ultrahigh temperature ceramics. Ceramics International, 2019, 45:10805-10809.
DOI URL |
[16] | GUSEV A I, REMPEL A A, MAGERL A J. Disorder and order in strongly nonstoichiometric compounds. Berlin Heidelberg: Springer, 2001: 179-243. |
[17] |
HOLLECK H. Material selection for hard coatings. Journal of Vacuum Science and Technology A, 1986, 4(6):2661-2669.
DOI URL |
[18] |
ZENG Q, PENG J, OGANOV A R, et al. Prediction of stable hafnium carbides: stoichiometries, mechanical properties, and electronic structure. Physical Review B, 2013, 88:214107.
DOI URL |
[19] |
YU X X, WEINBERGER C R, THOMPSON G B. Ab initio investigations of the phase stability in tantalum carbides. Acta Materialia, 2014, 80:341-349.
DOI URL |
[20] |
OGANOV A R, GLASS C W. Crystal structure prediction using ab initio evolutionary techniques: principles and applications. Journal of Chemical Physics, 2006, 124(24):244704.
DOI URL |
[21] |
LYAKHOV A O, OGANOV A R, STOKES H T, et al. New developments in evolutionary structure prediction algorithm USPEX. Computer Physics Communications, 2013, 184:1172-1182.
DOI URL |
[22] |
OGANOV A R, LYAKHOV A O, VALLE M. How evolutionary crystal structure prediction works and why. Accounts of Chemical Research, 2011, 44(3):227-237.
DOI URL |
[23] |
KRESSE G, FURTHMULLER J. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. Physical Review B, 1996, 54(16):11169-11186.
DOI URL |
[24] |
BLOCHL P E. Projector augmented-wave method. Physical Review B, 1994, 50(24):17953-17979.
DOI URL |
[25] |
PERDEW J P, RUZSINSZKY A, CSONKA G I, et al. Restoring the density-gradient expansion for exchange in solids and surfaces. Physical Review Letters, 2008, 100(13):136406.
DOI URL |
[26] |
TOGO A, OBA F, TANAKA I. First-principles calculations of the ferroelastic transition between rutile-type and CaCl2-type SiO2 at high pressures. Physical Review B, 2008, 78:134106.
DOI URL |
[27] |
MOMMA K, IZUMI F. VESTA 3 for three-dimensional visualization of crystal, volumetric and morphology data. Journal of Applied Crystallography, 2011, 44:1272-1276.
DOI URL |
[28] |
COWLEY R A. Acoustic phonon instabilities and structural phase transitions. Physical Review B, 1976, 13(11):4877-4885.
DOI URL |
[29] |
HILL R. The elastic behavior of a crystalline aggregate. Proceedings of the Physical Society Section A, 1952, 65(5):349-354.
DOI URL |
[30] |
CHEN X Q, NIU H, LI D, et al. Modeling hardness of polycrystalline materials and bulk metallic glasses. Intermetallics, 2011, 19(9):1275-1281.
DOI URL |
[31] | PUGH S F. Relations between the elastic moduli and the plastic properties of polycrystalline pure metals. Philosophical Magazine, 1954, 45(367):823-843. |
[32] |
RAZUMOVSKIY V I, POPOV M N, DING H, et al. Formation and interaction of point defects in group IVb transition metal carbides and nitrides. Computational Materials Science, 2015, 104:147-154.
DOI URL |
[33] |
ZHANG Y, LIU B, WANG J. Self-assembly of carbon vacancies in sub-stoichiometric ZrC1-x. Scientific Reports, 2015, 5:18098.
DOI URL |
[1] | YAN Yuxing, WANG Fan, ZHANG Juexuan, LI Fushao. First Principles Study of Electronic Structure and Optical Properties of ZnNb2O6 with Vacancy Defects [J]. Journal of Inorganic Materials, 2021, 36(3): 269-276. |
Viewed | ||||||
Full text |
|
|||||
Abstract |
|
|||||