 |
Atomic Reference Data
for Electronic Structure Calculations |
All data in the tables is given in Hartree energy units, in which numerical
values of unity are assigned to the mass m and charge e of the
electron and to the reduced Planck's constant
. In these units, the speed of light, c, is given by the
inverse of the fine structure constant. We have used the
1986 CODATA recommended value of the
fine structure constant to obtain the numerical value,
c = 137.0359895, used in the
RLDA AND
ScRLDA calculations.
Presentation of numerical data, element by element
The header line for each element takes the form
Atomic number Chemical symbol Ground electronic configuration
Four separate cases are then presented in successive columns:
- Local-density approximation (LDA),
- Local spin-density approximation (LSD),
- Relativistic local-density approximation (RLDA)
- Scalar-relativistic local-density approximation (ScRLDA).
Each column begins with the total energy in the given approximation and its
decomposition into four parts:
Etot = Total energy
Ekin = Kinetic energy
Ecoul = Electron-electron interaction energy (Hartree term)
Eenuc = Electron-nucleus interaction energy
Exc = Exchange-correlation energy
These energies are then followed by a list of orbital eigenvalues.
The orbital labels (e.g., 1s) are given to the left of all columns.
The orbital labels and eigenvalues are presented in alternating
boldface and plain type for ease of reading.
Conventions for orbital eigenvalues:
- The LDA and
ScRLDA approximations.
- These have only a single orbital eigenvalue for each (nl), which is
labelled on the left.
- The LSD approximation.
- For each (nl) there are two orbital eigenvalues, one for spin up and
one for spin down. They are presented here in spin order, i.e., the first
entry for each (nl) corresponds to spin down, the second to spin up.
Note that "down" is the direction of the majority spin.
- The RLDA approximation.
- This has a single eigenvalue for each s orbital, but for non-zero
l there are two eigenvalues, corresponding to the values of the sum of
spin and orbital angular momenta j = l ±1/2. The first
entry for a given (nl) in each column corresponds to
j = l - 1/2 ,
the second to j = l + 1/2 .
Presentation of numerical data in files
Those who wish to obtain all data in these tables may
retrieve
a compressed archive version of the original files. When decompressed and
untarred, the archive, dftdata.tar.gz yields a directory containing
one file and four subdirectories:
- dftdata/configurations
- dftdata/LDA/
- dftdata/LSD/
- dftdata/RLDA/
- dftdata/ScRLDA/
The configurations file contains the electronic configuration
information presented elsewhere in
this document. The directories each contain two subdirectories:
and each of these in turn contains the individual data files (92 files for
atoms, 91 for cations). The data file name format, common to all directories,
is "Atomic number" "Chemical symbol", e.g., 01H, 02He, 03Li,
etc. For example, the fully qualified path name of the data file for neutral
uranium treated in the RLDA approximation
will be:
dftdata/RLDA/neutrals/92U (show contents)
This file name convention facilitates simple report generation by standard
Unix commands; some examples are shown below.
The essential information within each data file is identical to that described
above. The first five lines contain the values of Etot,
Ekin, Ecoul, Eenuc, and Exc, with obvious labels; each subsequent
line contains an orbital eigenvalue with a label. The order of the orbital
eigenvalues is identical to that described above, but
the labelling scheme is different:
- The LDA
and ScRLDA approximations.
- These have only one orbital eigenvalue for each (nl), and so the
conventional spectroscopic notation is used as the label: 1s, 2s, 2p,,
etc.
- The LSD approximation.
- For each (nl) there are two orbital eigenvalues, one for spin down
and one for spin up. These are labelled as nlD and nlu,
i.e., 1sD, 1su, 2sD, 2su, etc. The capitalization of D is a
mnemonic device to emphasize that "down" spins constitute the majority.
- The RLDA approximation.
- For each (nl), we use the label nlP to designate the
orbital with j = l + 1/2, and nlM for the
orbital with j = l - 1/2 (mnemonic for
Plus and Minus). The P notation is retained for
s orbitals even though it is redundant.
Our data file name convention facilitates report generation by standard Unix
commands. Some simple examples follow:
- Generate list of LDA 3d orbital eigenvalues, ordered by Z
- With LDA/ as the current directory, execute
grep "3d" * | awk '{print $2}'
- Generate table of Hartree energies for all approximations,
ordered by Z
- With LDA/ as the current directory, execute
for each file (*)
echo $file | awk '{printf("%-6s", $1)}'
grep "Ecoul" $file | awk '{printf("%14.6f", $3)}'
grep "Ecoul" ../../LSD/neutrals/$file | awk '{printf("%14.6f", $3)}'
grep "Ecoul" ../../RLDA/neutrals/$file | awk '{printf("%14.6f", $3)}'
grep "Ecoul" ../../ScRLDA/neutrals/$file | awk '{printf("%14.6f\n", $3)}'
end
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Notation