Citation: | Hu Qingyang, Mao Ho-kwang. Born’s valence force-field model for diamond at terapascals: Validity and implications for the primary pressure scale[J]. Matter and Radiation at Extremes, 2021, 6(6): 068403. doi: 10.1063/5.0069479 |
[1] |
M. Born and T. von Kármán, “Über schwingungen in raumgittern,” Phys. Z. 13, 297 (1912).
|
[2] |
P. N. Keating, “Effect of invariance requirements on the elastic strain energy of crystals with application to the diamond structure,” Phys. Rev. 145, 637–645 (1966).10.1103/PhysRev.145.637
|
[3] |
R. Vogelgesang, A. K. Ramdas, S. Rodriguez, M. Grimsditch, and T. R. Anthony, “Brillouin and Raman scattering in natural and isotopically controlled diamond,” Phys. Rev. B 54, 3989–3999 (1996).10.1103/PhysRevB.54.3989
|
[4] |
V. E. Bean et al., “Another step toward an international practical pressure scale: 2nd AIRAPT IPPS task group report,” Physica B+C 139–140, 52–54 (1986).10.1016/0378-4363(86)90521-8
|
[5] |
G. Shen et al., “Toward an international practical pressure scale: A proposal for an IPPS ruby gauge (IPPS-Ruby2020),” High Press. Res. 40, 299–314 (2020).10.1080/08957959.2020.1791107
|
[6] |
D. E. Fratanduono et al., “Establishing gold and platinum standards to 1 terapascal using shockless compression,” Science 372, 1063 (2021).10.1126/science.abh0364
|
[7] |
C.-S. Zha, H.-k. Mao, and R. J. Hemley, “Elasticity of MgO and a primary pressure scale to 55 GPa,” Proc. Natl. Acad. Sci. U. S. A. 97, 13494 (2000).10.1073/pnas.240466697
|
[8] |
M. Murakami and N. Takata, “Absolute primary pressure scale to 120 GPa: Toward a pressure benchmark for Earth’s lower mantle,” J. Geophys. Res.: Solid Earth 124, 6581–6588, https://doi.org/10.1029/2019JB017635 (2019).10.1029/2019JB017635
|
[9] |
F. Soubiran and B. Militzer, “Anharmonicity and phase diagram of magnesium oxide in the megabar regime,” Phys. Rev. Lett. 125, 175701 (2020).10.1103/PhysRevLett.125.175701
|
[10] |
K. P. Esler et al., “Fundamental high-pressure calibration from all-electron quantum Monte Carlo calculations,” Phys. Rev. Lett. 104, 185702 (2010).10.1103/PhysRevLett.104.185702
|
[11] |
K. K. Zhuravlev, A. F. Goncharov, S. N. Tkachev, P. Dera, and V. B. Prakapenka, “Vibrational, elastic, and structural properties of cubic silicon carbide under pressure up to 75 GPa: Implication for a primary pressure scale,” J. Appl. Phys. 113, 113503 (2013).10.1063/1.4795348
|
[12] |
S. Zhang et al., “Discovery of carbon-based strongest and hardest amorphous material,” Natl. Sci. Rev. (Published Online), (2021).10.1093/nsr/nwab140
|
[13] |
Z. Pan, H. Sun, Y. Zhang, and C. Chen, “Harder than diamond: Superior indentation strength of wurtzite BN and lonsdaleite,” Phys. Rev. Lett. 102, 055503 (2009).10.1103/PhysRevLett.102.055503
|
[14] |
A. A. Correa, S. A. Bonev, and G. Galli, “Carbon under extreme conditions: Phase boundaries and electronic properties from first-principles theory,” Proc. Natl. Acad. Sci. U. S. A. 103, 1204–1208 (2006).10.1073/pnas.0510489103
|
[15] |
G. Kresse and D. Joubert, “From ultrasoft pseudopotentials to the projector augmented-wave method,” Phys. Rev. B 59, 1758–1775 (1999).10.1103/PhysRevB.59.1758
|
[16] |
G. Kresse and J. Furthmüller, “Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set,” Phys. Rev. B 54, 11169–11186 (1996).10.1103/PhysRevB.54.11169
|
[17] |
J. P. Perdew et al., “Restoring the density-gradient expansion for exchange in solids and surfaces,” Phys. Rev. Lett. 100, 136406 (2008).10.1103/PhysRevLett.100.136406
|
[18] |
J. P. Perdew and Y. Wang, “Accurate and simple analytic representation of the electron-gas correlation energy,” Phys. Rev. B 45, 13244–13249 (1992).10.1103/PhysRevB.45.13244
|
[19] |
D. M. Ceperley and B. J. Alder, “Ground state of the electron gas by a stochastic method,” Phys. Rev. Lett. 45, 566–569 (1980).10.1103/PhysRevLett.45.566
|
[20] |
Y. Le Page and P. Saxe, “Symmetry-general least-squares extraction of elastic data for strained materials from ab initio calculations of stress,” Phys. Rev. B 65, 104104 (2002).10.1103/PhysRevB.65.104104
|
[21] |
R. Hill, “The elastic behaviour of a crystalline aggregate,” Proc. Phys. Soc., Sect. A 65, 349–354 (1952).10.1088/0370-1298/65/5/307
|
[22] |
T. H. K. Barron and M. L. Klein, “Second-order elastic constants of a solid under stress,” Proc. Phys. Soc. 85, 523–532 (1965).10.1088/0370-1328/85/3/313
|
[23] |
G. W. Watson, P. Tschaufeser, A. Wall, R. A. Jackson, and S. C. Parker, in Computer Modeling in Inorganic Crystallography, edited by C. R. A. Catlow (Academic Press, 1997), pp. 55–81.
|
[24] |
S.-H. Yoo et al., “Finite-size correction for slab supercell calculations of materials with spontaneous polarization,” npj Comput. Mater. 7, 58 (2021).10.1038/s41524-021-00529-1
|
[25] |
F. Occelli, P. Loubeyre, and R. LeToullec, “Properties of diamond under hydrostatic pressures up to 140 GPa,” Nat. Mater. 2, 151–154 (2003).10.1038/nmat831
|
[26] |
H. J. McSkimin and P. Andreatch, “Elastic moduli of diamond as a function of pressure and temperature,” J. Appl. Phys. 43, 2944–2948 (1972).10.1063/1.1661636
|
[27] |
J. S. Tse and W. B. Holzapfel, “Equation of state for diamond in wide ranges of pressure and temperature,” J. Appl. Phys. 104, 043525 (2008).10.1063/1.2969909
|
[28] |
Y. Yi, V. Coropceanu, and J.-L. Brédas, “Nonlocal electron–phonon coupling in the pentacene crystal: Beyond the Γ-point approximation,” J. Chem. Phys. 137, 164303 (2012).10.1063/1.4759040
|
[29] |
Y. Akahama and H. Kawamura, “Pressure calibration of diamond anvil Raman gauge to 410 GPa,” J. Phys.: Conf. Ser. 215, 012195 (2010).10.1088/1742-6596/215/1/012195
|
[30] |
N. Dubrovinskaia, L. Dubrovinsky, R. Caracas, and M. Hanfland, “Diamond as a high pressure gauge up to 2.7 Mbar,” Appl. Phys. Lett. 97, 251903 (2010).10.1063/1.3529454
|
[31] |
B. Li et al., “Diamond anvil cell behavior up to 4 Mbar,” Proc. Natl. Acad. Sci. U. S. A. 115, 1713 (2018).10.1073/pnas.1721425115
|
[32] |
Y. Fei et al., “Toward an internally consistent pressure scale,” Proc. Natl. Acad. Sci. U. S. A. 104, 9182–9186 (2007).10.1073/pnas.0609013104
|
[33] |
D. Ikuta et al., “Large density deficit of Earth’s core revealed by a multi-megabar primary pressure scale,” arXiv:2104.02076 (2021).
|
[34] |
L. Dubrovinsky et al., “The most incompressible metal osmium at static pressures above 750 gigapascals,” Nature 525, 226–229 (2015).10.1038/nature14681
|
[35] |
M. Hou et al., “Superionic iron oxide–hydroxide in Earth’s deep mantle,” Nat. Geosci. 14, 174–178 (2021).10.1038/s41561-021-00696-2
|
[36] |
Q. Hu et al., “Mineralogy of the deep lower mantle in the presence of H2O,” Natl. Sci. Rev. 8, nwaa098 (2021).10.1093/nsr/nwaa098
|
[37] |
M. Somayazulu et al., “Evidence for superconductivity above 260 K in lanthanum superhydride at megabar pressures,” Phys. Rev. Lett. 122, 027001 (2019).10.1103/PhysRevLett.122.027001
|
[38] |
Y. Sun, J. Lv, Y. Xie, H. Liu, and Y. Ma, “Route to a superconducting phase above room temperature in electron-doped hydride compounds under high pressure,” Phys. Rev. Lett. 123, 097001 (2019).10.1103/PhysRevLett.123.097001
|
[39] |
P. Loubeyre, F. Occelli, and P. Dumas, “Synchrotron infrared spectroscopic evidence of the probable transition to metal hydrogen,” Nature 577, 631–635 (2020).10.1038/s41586-019-1927-3
|
[40] |
S. Tateno, K. Hirose, Y. Ohishi, and Y. Tatsumi, “The structure of iron in Earth’s inner core,” Science 330, 359 (2010).10.1126/science.1194662
|
[41] |
J. Badro, A. S. Côté, and J. P. Brodholt, “A seismologically consistent compositional model of Earth’s core,” Proc. Natl. Acad. Sci. U. S. A. 111, 7542 (2014).10.1073/pnas.1316708111
|