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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 .
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 elswhere 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 was 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 ofEtot, 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
foreach 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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Up: Atomic Reference Data for Electronic Structure Calculations
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