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March 16, 2015 21:52
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| Z: 46 | |
| Name: Palladium | |
| Symbol: Pd | |
| XC-functional: PBE | |
| Equation: Schrödinger | |
| Grid points: 2000 (0.00000, 0.00015, 0.00031, ..., 44.139, 47.558) | |
| Exponents: 50 (0.010, 0.014, ..., 76055.183, 105800.000) | |
| Basis functions: 37, 41, 44 (s, p, d) | |
| Solving non-relativistic Schrödinger equation using Gaussian basis-set: | |
| ............................................. | |
| Converged in 44 steps | |
| state occupation eigenvalue <r> | |
| nl [Hartree] [eV] [Bohr] | |
| ----------------------------------------------------- | |
| 1s 2.000 -861.849720 -23452.13373 0.033 | |
| 2s 2.000 -123.980898 -3373.69326 0.144 | |
| 2p 6.000 -115.217325 -3135.22421 0.123 | |
| 3s 2.000 -22.653043 -616.42091 0.390 | |
| 3p 6.000 -19.155972 -521.26074 0.382 | |
| 3d 9.500 -12.718196 -346.07986 0.355 | |
| 4s 2.000 -3.137922 -85.38723 0.968 | |
| 4p 6.000 -2.048795 -55.75057 1.044 | |
| 4d 10.000 -0.352013 -9.57876 1.463 | |
| 5s 0.000 -0.231791 -6.30737 3.266 | |
| 5p 0.000 -0.102168 -2.78014 4.536 | |
| Energies: [Hartree] [eV] | |
| -------------------------------------------- | |
| kinetic +4930.697853 +134171.17012 | |
| coulomb (e-e) +2009.968892 +54694.05879 | |
| coulomb (e-n) -11733.920324 -319296.34853 | |
| xc -140.123847 -3812.96545 | |
| total -4933.377426 -134244.08506 | |
| Exact exchange energy: -137.618796 Hartree, -3744.79952 eV | |
| Solving scalar-relativistic Schrödinger equation using finite difference: | |
| ............................................................... | |
| Converged in 62 steps | |
| state occupation eigenvalue <r> | |
| nl [Hartree] [eV] [Bohr] | |
| ----------------------------------------------------- | |
| 1s 2.000 -888.833267 -24186.39370 0.032 | |
| 2s 2.000 -130.428894 -3549.15224 0.138 | |
| 2p 6.000 -117.015156 -3184.14571 0.121 | |
| 3s 2.000 -23.943247 -651.52917 0.378 | |
| 3p 6.000 -19.534299 -531.55553 0.377 | |
| 3d 9.500 -12.559360 -341.75772 0.355 | |
| 4s 2.000 -3.390636 -92.26393 0.938 | |
| 4p 6.000 -2.120704 -57.70733 1.031 | |
| 4d 10.000 -0.346563 -9.43046 1.477 | |
| 5s 0.000 -0.253222 -6.89052 3.115 | |
| 5p 0.000 -0.106863 -2.90789 4.433 | |
| Energies: [Hartree] [eV] | |
| -------------------------------------------- | |
| kinetic +5227.692849 +142252.81848 | |
| coulomb (e-e) +2035.298008 +55383.29937 | |
| coulomb (e-n) -12159.552424 -330878.39199 | |
| xc -143.182585 -3896.19797 | |
| total -5039.744151 -137138.47211 | |
| Exact exchange energy: -140.557383 Hartree, -3824.76257 eV | |
| Generating PAW PBE setup for Pd | |
| Shape function: exp(-alpha*r^2), alpha=1.9 Bohr^-2 | |
| Core electrons: 35.5 | |
| Valence electrons: 10.0 | |
| Constructing smooth local potential for r < 2.400 | |
| Constructing smooth pseudo core density for r < 2.304 | |
| Pseudo core electrons: 1.344578 | |
| Projectors: | |
| state occ energy norm rcut | |
| nl [Hartree] [eV] [electrons] [Bohr] | |
| ---------------------------------------------------------- | |
| 5s 0.00 -0.253222 -6.89052 1.042 2.40 | |
| s 0.746778 20.32087 2.40 | |
| 5p 0.00 -0.106863 -2.90789 0.996 2.40 | |
| p 0.893137 24.30351 2.40 | |
| 4d 10.00 -0.346563 -9.43046 0.400 2.40 | |
| d 0.653437 17.78093 2.40 | |
| Checking eigenvalues of Pd pseudo atom using a Gaussian basis set: | |
| AE [eV] PS [eV] error [eV] | |
| 1s 2 -24186.394 | |
| 2s 2 -3549.152 | |
| 3s 2 -651.529 | |
| 4s 2 -92.264 | |
| 5s 0 -6.891 -6.886 0.005 | |
| -1.046 -1.108 -0.062 | |
| -0.122 -0.170 -0.048 | |
| 1.352 1.269 -0.083 | |
| 4.030 3.898 -0.132 | |
| 8.799 8.570 -0.229 | |
| 17.349 16.929 -0.420 | |
| 2p 6 -3184.146 | |
| 3p 6 -531.556 | |
| 4p 6 -57.707 | |
| 5p 0 -2.908 -2.902 0.005 | |
| -0.561 -0.565 -0.003 | |
| 0.252 0.212 -0.039 | |
| 1.676 1.645 -0.031 | |
| 4.039 3.977 -0.062 | |
| 7.853 7.762 -0.090 | |
| 14.097 13.969 -0.128 | |
| 3d 9 -341.758 | |
| 4d 10 -9.430 -9.427 0.004 | |
| -0.424 -0.422 0.002 | |
| 0.130 0.104 -0.026 | |
| 1.121 1.112 -0.010 | |
| 2.738 2.725 -0.012 | |
| 5.235 5.238 0.003 | |
| 9.077 9.093 0.015 | |
| EXX (core-core): -134.628617694 Hartree |
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