imd dl_poly xmd gulp plot xml
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Ref. 2.1 http://www.webelements.com/silver/crystal_structure.html
Ref. 2.2 P.L. Williams, Y. Mishin and J.C. Hamilton, An Embedded-atom Potential for the Cu-Ag System, Modelling Simul. Mater. Sci. Eng. 14, 817 (2006)
Ref. 2.3 Y.S. Touloukian, R.K. Kirby, R.E. Taylor, P.D. Desai, Thermal Expansion, Metallic Elements and Alloys, Plenum Press, New York, 1975.
Ref. 2.4 Q.B. Bian, S.K. Bose and R.C. Shukla, Vibrational and Thermodynamic Properties of Metals from a Model Embedded-atom Potential, J. Phys. Chem. Solids, 69, 168 (2008) and reference 46 therein.
Ref. 2.5 B.J. Lee, J.H. Shim and M.I. Baskes, Semiempirical atomic potentials for the fcc metals Cu, Ag, Au, Ni, Pd, Pt, Al, and Pb based on first and second nearest-neighbor modified embedded atom method, Phys. Rev. B 68, 144112 (2003)
Ref. 2.6 J.J. Wollenberger, Physical Metallurgy, edited by R.W. Cahn and P. Hansen (Amsterdam, North-Holland, 1983), p.1139
Ref. 2.7 W.R. Tyson and W.A. Miller, Surface Sci. 62, 267 (1977)
Ref. 2.8 Y. Kimura, Y. Qi, T. Cagin, and W.A. Goddard III, The Quantum Sutton-Chen Many-body Potential for Properties of fcc Metals, MRS Symposium Ser. 554 (1999) 43
Ref. 2.9 http://en.wikipedia.org/wiki/Stacking-fault_energy
Ref. 3.1 Y.S. Touloukian, R.K. Kirby, R.E. Taylor, P.D. Desai, Thermal Expansion, Metallic Elements and Alloys, Plenum Press, New York, 1975.
Ref. 3.2 M.E. Straumanis and C.L. Woodward, Acta Crystallogr. A27 549 (1971)
Ref. 3.3 G. Simons and H. Wang, Single Crystal Elastic Constants and Calculated Aggregate Properties (MIT Press, Cambridge, MA, 1977)
Ref. 3.6 H.K. Mao, P.M. Bell, J.W. Shaner and D.J. Steinberg, Specific volume measurements of Cu, Mo, Pd and Ag and calibration of the ruby R1 fluorescence pressure gauge from 0.06 to 1 Mbar, J. Appl. Phys. 3276 (1978
Ref. 3.7 R.G. McQueen and S.P. Marsh, Equation of State for Nineteen Metallic Elements from Shock-Wave Measurements to Two Megabars, J. Appl. Phys. 31, 1253 (1960)
Ref. 3.8 PWSCF calculation. Ultrasoft pseudopotential Ag.pbe-d-rrkjus.UPF has been used, with a kinetic energy cutoff ecutwfc = 40.0 Ry. Kpoint selection: 11x11x11. Energy minimization of fcc Ag yields a lattice parameter of a = 4.160 Å. For ab initio phonon calculations shown above, the lattice parameter is set to be 4.160 Å.
Ref. 3.9 Q.B. Bian, S.K. Bose and R.C. Shukla, Vibrational and Thermodynamic Properties of Metals from a Model Embedded-atom Potential, J. Phys. Chem. Solids, 69, 168 (2008) and reference 46 therein.
fcc: c/a = 1.0
bcc: c/a = 0.707
Ref. 8.2. Y. Waseda, The Structure of Non-Crystalline Materials (McGraw-Hill, New York, 1980).
Ref. 8.3. M. M. G. Alemany, O. Diéguez, C. Rey, and L. J. Gallego, Molecular-dynamics study of the dynamic properties of fcc
transition and simple metals in the liquid phase using the second-moment approximation to the tight-binding method, Phys. Rev. B 60, 9208 - 9211 (1999)
Ref. 9.1. A.V. Gorshkov, Correlations of the self-diffusion coefficients and viscosity of elemental melts with properties of elements, Inorganic Materials, 2, 218 (2000) Doi: 10.1007/BF02758020