Partial Densities of States and CoreLevel Spectroscopy
This tutorial explains how to generate total and partial densitiesofstates (DOS) with the Questaal package, using the band codes lmf, lm, and tbe. It is demonstrated in the tutorial for the total DOS in Co. DOS can be decomposed in multiple ways. Questaal has two forms: projection onto partial waves in augmentation spheres (see demonstration for Cr_{3}Si_{6}), and by Mulliken analysis. Partial wave and Mulliken decomposition are compared in the Fe tutorial.
Corelevel spectroscopy [1] describes the excitation of an core electron, calculated by Fermi’s golden rule which involves the matrix element of the dipole operator with the core and valence wave functions. It is closely related to the partial DOS and is computed in much the same way, as described in the Fe tutorial. The CLS should be calculated in the presence of a core hole, where the density redistributes. This is done in the CrN tutorial.
Other forms DOS that Questaal can calculate, but not described in this tutorial are:
 The Green’s function packages lmgf and lmpg compute partial DOS.
 The DOS the is the independentparticle approximation to the spectral function. The spectral function for the interacting case can be calculated in the GW framework, and also the DMFT framework. The noninteracting and interacting forms are compared at the GW level in this tutorial.
 The optics modes in the lmf and lm codes also enable you to resolve DOS in other forms
Table of Contents
 Preliminaries
 Introduction
 Making total DOS using band programs lmf, lm, or tbe
 1. Total DOS in elemental Co
 2. Partial DOS in Cr3Si6
 3. DOS and Corelevel Spectroscopy in Fe
 4. Corelevel spectroscopy in the presence of a core hole in CrN
 Further exercises
 References
 Total DOS in Co
Set up input file
blm mag ctrl=ctrl wsitex noshorten co
lmfa basfile=basp co
blm mag ctrl=ctrl wsitex noshorten gmax=8.5 nk=2000 co
Selfconsistent density
lmfa basfile=basp co
lmf ctrl.co
Total Co dos
lmf ctrl.co quit=dos dos@npts=2001@window=1,1
echo 5 8 10 10  pldos esclxy=13.6 ef=0 fplot lst=1 lst2 dos.co
fplot pr10 f plot.dos
open fplot.ps
 Partial DOS in Cr_{3}Si_{6}
Set up input file and selfconsistent density:
blm loc=0 mto=1 ctrl=ctrl wsitex cr3si6
lmfa basfile=basp cr3si6
blm loc=0 mto=1 ctrl=ctrl wsitex gmax=7.1 nk=200 cr3si6
lmfa basfile=basp cr3si6
lmf cr3si6
Partial DOS
rm mixm.cr3si6
lmf cr3si6 quit=rho pdos~nl=3
lmdos cr3si6 dos:npts=1001:window=1,1 pdos~nl=3
echo 40 5 .5 .5  pldos ef=0 fplot lst="5:9;14:18;23:27" dos.cr3si6
fplot pr10 f plot.dos
open fplot.ps
echo .5 3 6 6  pldos fplot~long~open~tmy=.125~dmin=0.20~xl=E esclxy=13.6 ef=0 lst="1;2,3,4;5;6;7;8;9;28;29:31" dos.cr3si6
fplot pr10 f plot.dos
open fplot.ps
 DOS and Corelevel Spectroscopy in Fe
Set up input file and selfconsistent density
blm mag ctrl=ctrl wsitex noshorten fe
lmfa basfile=basp fe
blm mag ctrl=ctrl wsitex noshorten gmax=8.3 nk=16 nit=20 fe
lmfa basfile=basp fe
lmf ctrl.fe
Mulliken DOS
lmf fe quit=rho vso=f mull~mode=2~nl=3
lmdos fe vso=f mull~mode=2~nl=3 dos:npts=1001:window=.7,.8
cp dos.fe dosmull.fe
echo .5 5 6 5  pldos esclxy=13.6 ef=0 fplot lst="9;11;13;15;17" lst2 dosmull.fe
fplot pr10 f plot.dos
open fplot.ps
Partial DOS, and comparison to Mulliken DOS
lmf fe quit=rho vso=f pdos~mode=2~nl=3
lmdos fe vso=f pdos~mode=2~nl=3 dos:npts=1001:window=.7,.8
cp dos.fe dospdos.fe
echo .999 6 6 5  pldos esclxy=13.6 ef=0 fplot~ext=mull~dmin=.4~tmy=.25 lst="1;3,5,7;9,11,15;13,17" lst2 dosmull.fe
echo .999 6 6 5  pldos esclxy=13.6 ef=0 fplot~ext=pdos~dmin=.4~tmy=.25 lst="1;3,5,7;9,11,15;13,17" lst2 dospdos.fe
awk '{if ($NF == "dosp.pdos") {print; sub("pdos","mull");sub("{ltdos}","2,bold=3,col=1,0,0");print} else if ($NF == "dosp2.pdos") {print; sub("pdos","mull");sub("{ltdos}","2,bold=3,col=1,0,0");print} else {print}}' plot.dos > plot.dos2
fplot pr10 f plot.dos2
open fplot.ps
Corelevel spectroscopy
lmf fe quit=rho cls:1,1,2 vmet=2 dos:npts=1001:window=.7,.8
mv dos.fe tdos.fe
lmdos cls dos:wtfn=cls:npts=1001:window=.7,.8 fe
mv dos.fe doscls.fe
catdos doscls.fe s1/10 tdos.fe
echo .5 10 6 6  pldos esclxy=13.6 fplot lst="1,3,5;7" lst2 dos.dat
fplot pr10 f plot.dos
open fplot.ps
 Corelevel spectroscopy in the presence of a core hole in CrN
Set up selfconsistent density
cp ~/lm/fp/test/ctrl.crn .
lmfa gas
mpirun n 8 lmf crn vnit=50
Corelevel spectroscopy
mpirun n 8 lmf rs=1,0 cls:5,0,1 vnit=1 vmetal=2 vnk=8 crn
lmdos dos:cls:window=0,1:npts=1001 cls crn vnk=8
echo .25 8 0 1  pldos fplot lst="1;3;5" lst2="2;4;6" dos.crn
fplot disp pr10 f plot.dos
open fplot.ps
Preliminaries
This tutorial assumes you have cloned and built the Questaal repository (located here). For the purpose of demonstration, ~/lm will refer to toplevel (source) directory of the cloned repository. In practice, this directory can be named differently. Questaal executables such lmf, lmdos, pldos, and catdos are required assumed to be in your path.
You will also need a postscript viewer. This document assumes you are using the applestyle open command to view postscript files.
Introduction
The densityofstates $D(E)$ is given by a sum over states i as [2]
$D(E) = \sum\nolimits_i\delta(E{}E_i) \qquad (1)$Band methods lmf, lm, and tbe work in a different manner than the Green’s function methods, lmgf and lmpg. They can evaluate Eq. (1) directly by approximating the δfunction with a Gaussian function. This method (sometimes called gaussian sampling) is simple and safe but is slow to converge with k. Convergence can be greatly accelerated with Methfessel and Paxton’s polynomial generalization of the Gaussian, but it is more cumbersome than the tetrahedron method, which is also implemented in the band programs. We use the tetrahedron method here.
This tutorial lmf to generate DOS, but lm and tbe perform similar functions.
Programs lm, lmf, and tbe have a facility to resolve, or decompose, the eigenfunction of a particular eigenfunction $\psi_i(E_i,\mathbf{r})$ into component parts. Note that an eigenstate is normalized: $\smallint\psi_i(E_i,\mathbf{r})^2d^3\mathbf{r}{=}1$. Decomposition amounts to resolving the unit norm of the wave function in different ways. A myriad of ways are possible [3]: Questaal offers two kinds, “partial waves” and “Mulliken analysis.” Corelevel spectroscopy (rather closely related to the partial wave analysis), is also explained here.
Partial Waves
The eigenfunction inside an augmentation sphere is given by solutions to the radial wave equation $\phi_l(E,r)$. The full energydependence of $\phi_l(E,r)$ is approximated by to linear order, expanded to first order in a Taylor series in energy. Thus, inside an augmentation sphere there are two partial waves for a particular site R and angular momentum l that contribute to the DOS: $\phi_{\mathbf{R}l}(\mathbf{r})$ and the energy derivative $\dot\phi_{\mathbf{R}l}(\mathbf{r})$. The ($\phi_{\mathbf{R}l}$,$\dot\phi_{\mathbf{R}l}$) pair are assumed to completely span the hilbert space inside augmentation sphere R (unless there is an additional wave from a local orbital). See this page for the definition of the lmf basis set.
Denoting the l and m quantum numbers by a compound index L, and labeling $\phi_{\mathbf{R}l}$ and $\dot\phi_{\mathbf{R}l}$ respectively as $\phi_{0\mathbf{R}l}$ and $\phi_{1\mathbf{R}l}$, the eigenfunction can be projected onto an augmentation sphere centered at R as
$P_\mathbf{R}\, \psi_i(E_i,\mathbf{r}) = \sum\limits_{\alpha L} {A_{\alpha\mathbf{R}L}^{(i)}} \, \phi_{\alpha\mathbf{R}l}(r) Y_L(\mathbf{\hat r}) \qquad (2)$$P_\mathbf{R}$ denotes a projection onto augmentation sphere R, $\alpha$ ranges from 0 to 1 (and if local orbitals are present, encompasses them), $L$ up to the augmentation cutoff lmxa.
Coefficients ${A_{\alpha\mathbf{R}L}^{(i)}}$ (which is determined from a solution of the secular matrix) then represent a particular kind of decomposition of $\psi _i(E,\mathbf{r})$. Assuming the ($\phi$, $\dot\phi$) basis is complete, this decomposition is independent of basis set. However, it does depend on the augmentation radius. In sum Eq. (2) can be expressed in terms of the energydependent partial wave as
$P_\mathbf{R}\, \psi _i(E,\mathbf{r}) = \sum\limits_{\alpha L} {C_{\mathbf{R}L}^{(i)}} \, \phi_{\mathbf{R}l}(E,r) Y_L(\mathbf{\hat r}) \qquad (3)$where $\phi_{\mathbf{R}l}(E,r)$ is a linear combination of $\phi$, $\dot\phi$ (and possibly local orbitals) normalized so that $\smallint \phi_i(E,\mathbf{r})Y_L(\mathbf{\hat r})^2d^3\mathbf{r}{=}1$.
The ${C_{\mathbf{R}L}^{(i)}}$ make up partial contributions to $D(E)$, Eq. (1). The contribution to $D(E)$ from a particular partial wave $\phi_{\mathbf{R}l}$ is well defined, positive and less than 1, since contributions from all partial waves at most sum to one and the interstitial also adds a positive a contribution.
Notes:

In the ASA, with spacefilling spheres, the sum of partial waves comprises the total wave function, and the separate contributions to sum to 1.

tbe is not an augmented wave method; this kind of decomposition is not possible.
Mulliken Analysis
Mulliken analysis is a decomposition of an eigenfunction into the separate orbital contributions. The eigenfunction is written as a linear combination of lmf basis functions $\chi_{\alpha\mathbf{R}L}(\mathbf{r})$
$\psi_i(E_i,\mathbf{r}) = \sum\limits_{\alpha\mathbf{R}L} {z_{\alpha\mathbf{R}L}^{(i)}\,\chi_{\alpha\mathbf{R}L}(\mathbf{r})} \qquad (4)$The $\chi_{\alpha\mathbf{R}L}$ are augmented smooth Hankel functions.
We can decompose $D(E)$ through coefficients $z_{\alpha\mathbf{R}L}^{(i)}$. In this case the $z_{\alpha\mathbf{R}L}^{(i)}$ are eigenvectors of the lmf hamiltonian: they diagonalize both the hamiltonian and overlap. In matrix form
$(z^{(i)})^{\dagger} \, H \, z^{(i)} = E_i \quad \mathrm{and} \quad (z^{(i)})^{\dagger} \, O \, z^{(i)} = 1 \qquad (5)$If the overlap matrix were diagonal, it is evident from Eq. (5) that the eigenvectors would satisfy $\sum\nolimits_{\alpha {\mathbf{R}}L} [z_{\alpha \mathbf{R}L}^{(i)}]^\dagger z_{\alpha {\mathbf{R}}L} = 1$. The overlap is not diagonal; however there is a generalization
$\sum\nolimits_{\alpha {\mathbf{R}}L} {(z_{\alpha \mathbf{R}L}^{(i)}})^{1} z_{\alpha {\mathbf{R}}L}^{} = 1 \qquad (6)$$z_{\alpha \mathbf{R}L}^{(i)}$ is a vector; there is one eigenvector $z^{(i)}$ for each of the ${\alpha\mathbf{R}L}$ components. Thus $z$ is a square matrix that can be inverted.
The sum over components ${\alpha\mathbf{R}L}$ in Eq. (5) evaluates to 1 for a particular state $i$, so we can decompose or resolve the unit norm into separate elements, resolving by $\alpha$, $\mathbf{R}$ and $L$. Decomposition by $\alpha$ is not so meaningful (lmf contracts over $\alpha$; while lm and tbe only have a single $\alpha$), but resolving by $\mathbf{R}$ or $L$ can offer a great deal of physical insight. This decomposition is used to assign color weights in band plots. Examples can be found in the plbnds manual and in the lmf band plotting tutorial. How to do it in the partial dos context will be shown below.
How information is assembled for analysis
The following outlines the general procedure for making partial wave analysis. Steps are explained in more detail later, in the examples.
Both Mulliken and partial pave analysis enable decomposition of the unit norm into partial contributions associated with a particular site R and L=lm character. The band programs (lm, lmf, and tbe) will accumulate weights for a partial wave or Mulliken analysis in the course of a usual band pass, by adding a commandline switch pdos or mull. Both switches have numerous options that can select or group a subset of all states, to contract over m (leaving the resolution by R and l) or over both l and m, resolving by R only. This is described in more detail below. The band program will write a file moms.ext to disk with information about the partial decomposition.
With moms.ext in hand, run lmdos with exactly the same switch pdos or mull, including any modifiers. This should generate a file dos.ext with the requisite information. By default this file will take traditional standard format for DOS files; but you can change the format.
The pldos utility is designed to read DOS files, and select out or combined particular DOS, and either make a postscript file directly (for quick and dirty results) or format the data in easily read formats.
Notes on Partial wave and Mulliken analysis, and their relative merits

Mulliken analysis has somewhat imprecise meaning, as the results are dependent on the user’s choice of basis. However, to the basis functions do resemble atomic orbitals, especially for d and f electrons, they are a useful tool.

As noted above, partial wave analysis is approximately independent of basis, except for the choice of augmentation radius. As such, it is often preferable to Mulliken analysis.

The Jigsaw Puzzle Orbital basis is very short ranged, so association with a particular atomic orbital is more clear. The distinction between partial wave and Mulliken analysis will be much smaller.

In the ASA, with spacefilling spheres, the sum of partial waves comprises the total wave function, and the separate contributions to sum to 1.

lm typically generate the moments file moms.ext automatically as part of the band pass. However the moments are generated for inequivalent classes only; the weights are ordered by class instead of by site. You can run lmpg after a band pass (without argument pdos) to generate partial DOS for each class (typically resolved by l but not by m).

tbe is not an augmented wave method; partial wave decomposition is not possible.
Making total DOS using band programs lmf, lm, or tbe
The simplest DOS is the total DOS/cell (not resolved into any components). This is automatically generated when you turn on SAVDOS=T in category BZ. A band program (lmf, lm, or tbe) will generate DOS in a particular energy window, on a uniform mesh of points.
Note: you can also cause lmf to generate dos using the commandline argument dos. Modifiers to this switch allow you to control the energy mesh (and format) of the dos file.
lmf will generate DOS in a particular energy window. Tag BZ_DOS specifies the energy window, BZ_NPTS the number of points.
If BZ_DOS is specified in the input file, lmf will use the specified window. Otherwise lmf will select the window as follows. It makes a rough estimate of the Fermi level from the first k point, subtracts 0.5 Ry from the first eigenvalue, and adds 0.5 Ry to the estimate for the Fermi level.
However, if you further use the commandline switch nofixef0
, default values are used. You can find them with
lmf input  grep BZ_DOS
If BZ_NPTS is specified, it uses the specified value for the number of points. Otherwise it uses a default, which you can find by invoking
lmf input  grep BZ_NPTS
lmf writes the DOS to dos.ext, normally in the traditional standard format for dos files. You can reformat it yourself to use your favorite graphics package, or use pldos utility to format the dos into standard Questaal format for twodimensional arrays, which are more easily read by other graphics packages.
At this stage, you can use your favorite graphics package to draw a figure from files dosp.dat and dosp2.dat. Alternatively pldos will have written an fplot script; you can immediately create a postscript file using fplot.
1. Total DOS in elemental Co
Building a Co input file
Copy the contents of the box below into file init.co.
LATTICE
% const a=4.730 c=7.690
ALAT={a} PLAT= 1.0 0.0 0.0 0.5 0.8660254 0.0 0.0 0.0 {c/a}
SPEC
ATOM=Co MMOM=0,0,1.6
SITE
ATOM=Co X=0 0 0
ATOM=Co X=1/3 1/3 1/2
Construct the input file in the usual manner, see for example the Si tutorial or the PbTe tutorial:
blm mag ctrl=ctrl wsitex noshorten co
lmfa basfile=basp co
blm mag ctrl=ctrl wsitex noshorten gmax=8.5 nk=2000 co
See this page for commandline arguments to blm and this page for arguments to lmfa.
The mesh density cutoff set by gmax=8.5
can not be determined in advance, but a good value can be obtained from the output of lmfa, as explained in the introductory tutorials. blm is run twice, once to set up lmfa, and again to set the final version of the input file, ctrl.co.
nk=2000
sets the number of k points. The negative value is a flag telling lmf to find a set of (n_{1},n_{2},n_{3}) divisions of the reciprocal lattice such that the number of microcells n_{1}×n_{2}×n_{3} is approximately 2000, while rendering the microcells as close to equidimension as possible (G_{i}/n_{i} as uniform as possible). 2000 points makes a reasonably fine mesh, good enough to generate a reasonably smooth DOS with the tetrahedron method. Coarser meshes will cause the dos to be much less smooth and this is especially severe if the integration is performed by simple sampling integration.
Selfconsistent Co density
Make the density selfconsistent:
$ lmfa basfile=basp co
$ lmf ctrl.co
You should get a reasonably selfconsistent density in 10 iterations. The last line of the file save.ext should read
c mmom=3.1596775 ehf=5564.3100279 ehk=5564.310028
The magnetic moment/atom is then calculated to be 3.1596775/2, close to the experimental moment (1.6 μ_{B}).
Total DOS in Co
Use the command line argument dos to generate the total DOS with lmf:
$ lmf ctrl.co quit=dos dos@npts=2001@window=1,1
quit=dos
tells lmf to stop after the dos is generated.
Near the end of the standard output the following line should appear:
... Generating total DOS
The pldos utility will extract and reconfigure the contents of dos.co, saving the data in a more palatable format :
echo 5 8 10 10  pldos esclxy=13.6 ef=0 fplot lst=1 lst2 dos.co ↑ ↑ ↑ ↑ dmx ht emin emax
pldos reads data in the traditional dos file format the band codes normally use. It can make a postscript figure directly, or be used as a preparatory step for fplot or another graphics package. We do the latter here.
pldos takes four arguments from standard input:
 dmx DOS upper bound in the figure
 ht approximate height of figure, in cm
 emin minimum energy to draw (left point of abscissa)
 emax maximum energy to draw (right point of abscissa)
Note: no interactive input is required from the command as written above. However, you can run pldos in an interactive mode by entering simply pldos dos.co
.
Switches to pldos have the following effect:
 −esclxy=13.6 scales the abscissa (energy) to convert it from Ry to eV, and the ordinate (dos) converting it from Ry^{−1} to eV^{−1}.
 −ef=0 Shift the abscissa, putting the Fermi energy at 0.
 −fplot Set up input for fplot. This entails the following:
 Create file dosp.dat for the spin1 dos, written in the standard Questaal format for 2D arrays.
 Create a corresponding file dosp2.dat for the spin2 dos (applicable only to spin polarized cases).
Note: The spin2 dos are scaled by −1 to make it convenient for drawing the figure (see below).  Create an fplot script plot.dos
 −lst=1 Select which channels in the dos file (dos.co) to combine for the majority spin.
In this case there is only a single channel per spin; but when the dos is resolved into components there will be many.  −lst2 Select which channels in the dos file (dos.co) to combine for the second spin.
−lst2 without arguments tells pldos to copy the list from lst, incrementing each element by 1.
Since (majority,minority) dos are interleaved, it simply generates the spin2 channels counterpart to spin1.  dos.co causes pldos to read DOS from dos.co, formatted in the way lmf usually writes dos files.
The order of switches is not important, but the file name specifying DOS must come last.
File dosp.dat contains the spin1 dos (majority in this case), and dosp2.dat the negative of the spin2 (minority) dos, written in Questaal’s standard 2D array format.
Use your favorite graphics package to draw a figure from files dosp.dat and dosp2.dat. Alternatively, use fplot : pldos has already created a script plot.dos for fplot. Create a handsome picture with the following
$ fplot pr10 f plot.dos
$ open fplot.ps
The majority spin dos is shown above y=0, the minority spin below it. (Energy is on the x axis with the Fermi level at 0.) Co d bands dominate near the Fermi level E_{F}: they form two broad peaks with the majority d falling completely below E_{F} and the minority d straddling it.
Add this line to ctrl.co :
BZ SAVDOS=t NPTS=2001 DOS=1,1 NEVMX=999
Copy the original dos.co to a backup and invoke lmf without a commandline argument a
mv dos.co dos.bk
lmf ctrl.co quit=dos
diff dos.co dos.bk
The last line compares the two dos. There should be no difference.
However, remove tag NEVMX=999 and remake the dos. Now a small difference appears near emax. lmf does not necessarily compute all the eigenvalues and eigenvectors. When NEVMX is present it specifies how many eigenfunctions to make. Now all eigenvalues are found since the rank of the hamiltonian is 36, much less than 999, and there is no loss. (Command line switch dos also causes lmf to generate all the eigenvalues.)
2. Partial DOS in Cr3Si6
Input file and selfconsistency in Cr3Si6
Cr_{3}Si_{6} (AKA CrSi_{2}) is a transition metal silicide with a small band gap [4], measured to be between 0.27 and 0.67 eV. The three Cr and six Si atoms are symmetryequivalent.
To set up the computational conditions, copy the following box into init.cr3si6.
# Init file for Cr3Si6
LATTICE
ALAT=8.37 PLAT= sqrt(3/4) 0.5 0.0 0.0 1.0 0.0 0.0 0.0 1.43369176
SITE
ATOM=Cr X= 1/2 1/2 1/6
ATOM=Cr X= 0 1/2 1/6
ATOM=Cr X= 1/2 0 1/2
ATOM=Si X= 1/3 1/6 1/6
ATOM=Si X=1/3 1/6 1/6
ATOM=Si X=1/6 1/6 1/6
ATOM=Si X= 1/6 1/6 1/6
ATOM=Si X= 1/6 1/3 1/2
ATOM=Si X=1/6 1/3 1/2
In this tutorial we will use a small, singlekappa basis. It is not necessary, but it speeds up the calculation with minimal effect on the accuracy since the system is fairly closepacked.
The following steps up the input file and generate a selfconsistent density. The purpose for the first invocation of the (blm,lmfa) pair is solely to determine gmax:
$ blm loc=0 mto=1 ctrl=ctrl wsitex cr3si6
$ lmfa basfile=basp cr3si6
$ blm loc=0 mto=1 ctrl=ctrl wsitex gmax=7.1 nk=200 cr3si6
$ lmfa basfile=basp cr3si6
$ lmf cr3si6
 loc=0 suppresses lmfa’s search for deep lying states to be treated as local orbitals.
 mto=1 specifies a singlekappa LMTO basis (minimal basis).
 nk=200 specifies a somewhat coarse k mesh of 7×7×4 divisions (24 inequivalent points)
 ctrl=ctrl tells blm to write the input file directly ctrl.cr3si6.
 wsitex tells blm to write the coordinates in the site as multiples of the lattice vectors, as they are in the init file.
 –basfile=basp tells lmfa to write the basp file directly to basp.cr3si6.
When lmf’s completes execution you should find that the 10^{th} and final iteration is (nearly) selfconsistent with and RMS DQ=1.46e5. You should find that the last line of file save.cr3si6 is
x ehf=9761.745587 ehk=9761.7455858
Partial DOS in Cr3Si6
Note: A figure for partial DOS similar to the one generated here is shown in the pldos manual. Other features of the pdos switch and switches to pldos are used there.
DOS can be decomposed by site R, by R and l within R, and by R and both l and m within R.
First, try using pdos without any modifiers
$ rm mixm.cr3si6
$ lmf cr3si6 quit=rho pdos
At the beginning of the band pass you should see this line
sumlst: Partial DOS mode 2 (all sites lmprojected) 9 sites 171 channels
Each of the 9 sites will decomposed into DOS, resolved by both l and m. There is a grand total of 171 channels, because DOS are expanded to lmxa=4 for Cr (25 channels) and lmxa=3 for Si (16 channels), as the input file specifies. This is overkill: l>2 for Cr and l>1 for Si is of limited interest. Run lmf again, this time limiting the maximum number of l’s to 3 at any site. Now the number of channels should be 81
$ rm mixm.cr3si6
$ lmf cr3si6 quit=rho pdos~nl=3
Data is written into file moms.cr3si6. Next run lmdos:
$ lmdos cr3si6 dos:npts=1001:window=1,1 pdos~nl=3
You must include the pdos switch in exactly the same way you used it to make moms.cr3si6.
If you leave off the dos switch you will be prompted for three numbers that define the energy mesh (number of points, minimum and maximum energies).
lmdos should generate the following output:
ASADOS: reading weights from file MOMS
expecting file to be resolved by l and m
file has 81 channel(s)
Using npts=1001 emin=1 emax=1
IOMOMQ: read 24 qp efermi=0.160300 vmtz=0.000000
Don’t worry that the output refers to “ASADOS.” lmdos handles both ASA and FP cases. Next comes a list of channels indicating how the grand total of 171 channels is divided up.
Channels in dos file generated by LMDOS:
site class label spin1
1 1 Cr 1:9
2 1 Cr 10:18
3 1 Cr 19:27
4 2 Si 28:36
5 2 Si 37:45
6 2 Si 46:54
7 2 Si 55:63
8 2 Si 64:72
9 2 Si 73:81
Also the three Cr and six Si atoms should be equivalent by symmetry; however the orbitals of a given l transform into one another for the different sites. The sum over all m for a particular l should be the same for symmetry equivalent atoms.
The steps following combine the 5 Cr d orbitals on each atom, into three panels (panel 1 for the first Cr, panel 2 for the second Cr, panel 3 for the third Cr). Then we can check to see how well this invariance is kept.
$ echo 40 5 .5 .5  pldos ef=0 fplot lst="5:9;14:18;23:27" dos.cr3si6
This sets up DOS in three panels. lst tells lmdos which DOS to combine into a single data set, and how many data sets to make. It uses “;“ as a separator to tell lmdos to start a new data set. Each data set gets its own panel. DOS in channels 5:9, 14:18, and 23:27 are each added together to create DOS respectively for the first, second, and third panels. Note from the table above that these channels correspond to d orbitals for the first, second and third Cr atoms.
DOS is drawn on a Ry energy scale in this case. pldos creates a data file dosp.dat in the standard Questaal format for twodimensional arrays. pldos also generates a script file plot.dos readable by fplot. To see a picture do:
$ fplot pr10 f plot.dos
$ open fplot.ps
You can compare directly the last three columns in dosp.dat, to check how similar they are. This is easily accomplished with the mcx calculator:
$ mcx dosp.dat e2 x2x3 x2x4
The differences are much smaller than the dos itself; but evidently there is some difference. This is largely an artifact of incomplete k convergence. Repeat the calculation with more k points
lmf cr3si6 quit=rho pdos~nl=3 vnkabc=1000
lmdos cr3si6 dos:npts=1001:window=1,1 pdos~nl=3 vnkabc=1000
echo 40 5 .5 .5  pldos ef=0 fplot lst="5:9;14:18;23:27" dos.cr3si6
mcx dosp.dat e2 x2x3 x2x4
and the error becomes much smaller.
The Co $3z^2{}1$ orbital (the $m{=}0$ d orbital) also should not depend on the Cr atom. This orbital is the middle one (7 for Cr_{1}, 16 for Cr_{2}, 25 for Cr_{3}). Do the following:
$ echo 20 5 .5 .5  pldos ef=0 fplot lst="7;16;25" dos.cr3si6
$ fplot pr10 f plot.dos
$ open fplot.ps
The three panels should look nearly identical.
The following creates a figure with the following panels:
 The s Co orbital (first atom)
 The sum of Co p orbitals (first atom)
 The 5 Co d orbitals, each given its own panel (first atom)
 The Si s orbital (fourth atom)
 The sum of Si p orbitals (fourth atom)
This makes a grand total of 9 panels.
The command below sets up figure in eV units.
echo .5 3 6 6  pldos fplot~long~open~tmy=.125~dmin=0.20~xl=E esclxy=13.6 ef=0 lst="1;2,3,4;5;6;7;8;9;28;29:31" dos.cr3si6
Modifiers to the −fplot switch alter plot.dos, to “prettify” the figure when fplot generates it. To see what they do, run pldos with no arguments.
Make and display a postscript figure:
fplot pr10 f plot.dos
open fplot.ps
You should see a figure like the one shown below.
The first and second panels (Cr s and p) show very little DOS near the Fermi level. Panels 3 through 7 show the five Cr d DOS; they dominate the electronic structure near the Fermi level (shown by the blue dotdashed line). The Si p also makes a significant contribution.
From an aesthetic perspective, the autogenerated script plot.dos makes a reasonable figure but some tweaking is needed.
 number labelling for adjacent panels collide with each other. This can easily be rectified by editing plot.dos and making a global change dmax=0.5 → dmax=0.499.

Labels are needed and the energy axis label (xl E) needs some improvement. Try one of:
xl '&\{E} (eV)' xl "~\{w} (eV)" lbl 3.8,.25 rd '~\{w} (eV)'
3. DOS and Corelevel Spectroscopy in Fe
Input file and Selfconsistent density in Fe
Copy the following into init.fe. As an initial guess, we use a trial moment of 2 μ_{B}. (Fe has a moment of 2.2 μ_{B} in the ground state).
LATTICE
% const a=5.4235
ALAT={a} PLAT= 0.5 0.5 0.5 0.5 0.5 0.5 0.5 0.5 0.5
SPEC
ATOM=Fe MMOM=0,0,2
SITE
ATOM=Fe X=0 0 0
Construct the input file. The first two lines are present to determine a value for gmax.
$ blm mag ctrl=ctrl wsitex noshorten fe
$ lmfa basfile=basp fe
$ blm mag ctrl=ctrl wsitex noshorten gmax=8.3 nk=16 nit=20 fe
Make the Fe density selfconsistent:
$ lmfa basfile=basp fe
$ lmf ctrl.fe
You should find that the at the last (11^{th}) iteration the density is selfconsistent with a magnetic moment of 2.23 μ_{B}.
Note: the magnetic moment is not variational in the density, so the value is more sensitive to k convergence than the total energy. With 13 divisions you should find a value of 2.168 μ_{B}; with 24 divisions you should find a value of 2.218 μ_{B}.
Mulliken analysis in Fe
Here we perform Mulliken analysis. Use mull~mode=0
to resolve by R only – not meaningful here since there is only a single site; Use mull~mode=1
to resolve by R and l. We use mull~mode=2~nl=3
to resolve by both l and m, and limit the number of l to spd.
$ lmf fe quit=rho vso=f mull~mode=2~nl=3
$ lmdos fe vso=f mull~mode=2~nl=3 dos:npts=1001:window=.7,.8
$ cp dos.fe dosmull.fe
You should see this table just before lmdos exits:
Channels in dos file generated by LMDOS:
site class label spin1 spin2
1 1 Fe 1:17:2 2:18:2
Spin channels are interleaved, so odd channels hold spin1 (majority spin) and even channels minority spin Mulliken dos.
Draw a figure showing each of the 5 d channels
$ echo .5 5 6 5  pldos esclxy=13.6 ef=0 fplot lst="9;11;13;15;17" lst2 dosmull.fe
$ fplot pr10 f plot.dos
$ open fplot.ps
The figure is drawn with the convention that spin1 DOS is shown above y=0, spin2 DOS below it.
Mulliken DOS are confined to a window of about (−4,3) eV. Note that the three $t_{2g}$ and two $e_g$ states should be identical. The former are xy, yz, and xz states, which correspond to orbitals 5,6,8 in Questaal’s ordering, and the latter 3z^{2}−1 and x^{2}−y^{2} states correspond to orbitals 7,9. With the interleaving of spins, the spin 1 $t_{2g}$ states correspond to channels (9,11,15) and $e_g$ to channels (13,17) in dosmull.fe. You can see that panels 1,2,4 appear identical, as do panels 3,5 [5].
lmf symmetrizes the Mulliken DOS by rotating each irreducible k point to all points in the star, so that the full Brillouin zone is used. The DOS should be the same whether symmetry operations are used or not.
To test to what extent this is actually the case, remake the DOS just calculated, but this time writing to an mcxreadable format:
lmdos fe vso=f mull~mode=2~nl=3 dos:npts=1001:window=.7,.8:rdm
cp dos.fe dosmullsym.fe
Remake the DOS without symmetry operations:
lmf fe quit=rho vso=f nosym mull~mode=2~nl=3
lmdos fe vso=f nosym mull~mode=2~nl=3 dos:npts=1001:window=.7,.8:rdm
cp dos.fe dosmullnosym.fe
Find the globally maximum change in DOS in any channel:
mcx dosmullsym.fe dosmullnosym.fe  abs max:g
This shows that there are some numerical errors even in something that should be formally exact.
For a visual comparison, try the following, which compare the minorityspin d channels with and without symmetry
fplot colsy 1+10:1+18:2 dosmullsym.fe colsy 1+10:1+18:2 lt 2,col=1,0,0 dosmullnosym.fe
open fplot.ps
The list of columns (1+10:1+18:2) follows standard Questaal syntax for integer lists, and correspond to columns 11,13,15,17,19 (in this format columns are shifted by one to accommodate the energy in the first column.)
The red and black curves should be nearly identical. Also the three $t_{2g}$ and two $e_g$ states should be identical. Visually inspect the difference in $t_{2g}$ the $e_g$ states as follows:
$ fplot colsy 11 dosmullsym.fe lt 2,col=1,0,0 colsy 13 dosmullsym.fe lt 3,col=0,1,0 colsy 17 dosmullsym.fe
$ open fplot.ps
$ fplot y 0,10 colsy 15 dosmullsym.fe lt 2,col=1,0,0 colsy 19 dosmullsym.fe
$ open fplot.ps
The wave function rotator has not yet been implemented in the noncollinear case [5]. To see the effect of SO coupling, the original calculation (without SO coupling) must be run without symmetry operations to compare against the result with SO coupling:
The following steps accomplish this:
lmf fe quit=rho vso=f nosym mull~mode=2~nl=3
lmdos fe vso=f nosym mull~mode=2~nl=3 dos:npts=1001:window=.7,.8:rdm
cp dos.fe dosmullnoso.fe
lmf fe quit=rho vso=t nosym mull~mode=2~nl=3
lmdos fe vso=t nosym mull~mode=2~nl=3 dos:npts=1001:window=.7,.8:rdm
cp dos.fe dosmullso.fe
Without spin orbit coupling, the xy and xz DOS should be identical. But SO coupling reduces the symmetry and this is no longer the case. Make the following figure:
$ fplot frme 0,1,0,.7 frmt th=3,1,1 colsy 11 dosmullnoso.fe colsy 11 lt 2,col=1,0,0 dosmullso.fe colsy 13 lt 3,col=0,1,0 dosmullso.fe
It draws the xy without SO in black, the xy with SO in red, and the xz with SO as a dotted green line. You can see how SO modifies the xy orbital. SO modifies the xz orbital in a similar, but slightly different manner, owing to the reduction in symmetry.
Partial DOS in Fe
The partial DOS proceeds in much the same way as Mulliken analysis just presented.
lmf fe quit=rho vso=f pdos~mode=2~nl=3
lmdos fe vso=f pdos~mode=2~nl=3 dos:npts=1001:window=.7,.8
cp dos.fe dospdos.fe
You can draw the partial DOS in the same manner as the Mulliken DOS. In the steps below we combine the two so the similarities and differences can be compared.
$ echo .999 6 6 5  pldos esclxy=13.6 ef=0 fplot~ext=mull~dmin=.4~tmy=.25 lst="1;3,5,7;9,11,15;13,17" lst2 dosmull.fe
$ echo .999 6 6 5  pldos esclxy=13.6 ef=0 fplot~ext=pdos~dmin=.4~tmy=.25 lst="1;3,5,7;9,11,15;13,17" lst2 dospdos.fe
$ awk '{if ($NF == "dosp.pdos") {print; sub("pdos","mull");sub("{ltdos}","2,bold=3,col=1,0,0");print} else if ($NF == "dosp2.pdos") {print; sub("pdos","mull");sub("{ltdos}","2,bold=3,col=1,0,0");print} else {print}}' plot.dos > plot.dos2
$ fplot pr10 f plot.dos2
$ open fplot.ps
The first command makes four panels consisting of $s$, $p_x{+}p_y{+}p_z$, $t_{2g}$ and $e_{g}$ Mulliken channels; the second does the same for partial wave decomposition. awk combines the two kinds of data to make a single fplot script, plot.dos2. fplot creates the postscript figure.
Mulliken and partial wave analysis show modest differences in the $s$ and $p$ channels, while the $d$ channels are nearly identical.
Corelevel spectroscopy in Fe
Tell lmf to compute EELS, (also called corelevel spectroscopy) by adding cls to the commandline. This switch acts in a manner roughly similar to the mull and pdos switches. In the CLS case, matrix element $\langle\psi_c\mathbf{r}\psi_v\rangle$ of the core level with the valence states are calculated, and the number of channels is the number of corelevel states. The weights file is written to cls.fe, and includes the matrix element.
You must specify a particular core level. There are several ways to do it. Here we consider the excitation from the 2p level, which can be specified as cls:1,1,2 for atom 1, l=1, n=2.
Run the following to simultaneously generate cls.fe (cls) for CLS and the total dos (dos). The two will be compared later.
$ lmf fe quit=rho cls:1,1,2 vmet=2 dos:npts=1001:window=.7,.8
$ mv dos.fe tdos.fe
The cls tag requires BZ_METAL=2 or BZ_METAL=3.
The second command renames the file containing the total DOS, since that file will be overwritten CLS.
You should see a table of matrix elements printed just before lmf exits
CLS atom 1 (Fe) n=2 l=1
Spin 1 ..
vcdmel: ecor0=50.757934 ecore=50.757934
(not including electrostatic potential shift)
l <ucore> <score> <urcore> <srcore>
0 0.013933 0.008083 0.037621 0.018932
1 0.000471 0.000136 0.057507 0.014659
...
Make the CLS and rename the file:
$ lmdos cls dos:wtfn=cls:npts=1001:window=.7,.8 fe
$ mv dos.fe doscls.fe
lmdos converts the cls weights into kintegrated spectra in much the same way it converts the moms into DOS. You must supply lmdos with a switch telling it that this is a CLS calculation and also tell it to read data from file cls.
cls.fe should contain three channels per spin for x, y, and z. Concatenate it and the DOS into a single file. They have different units, so the latter is scaled by 1/10 to make them about the same size:
$ catdos doscls.fe s1/10 tdos.fe
catdos concatenates the two DOS, writing the output to file dos.dat with 8 channels. The first 6 channels are the CLS, the last two are the total DOS.
Draw two panels, one with the three CLS combined and the other with DOS
$ echo .5 10 6 6  pldos esclxy=13.6 fplot lst="1,3,5;7" lst2 dos.dat
$ fplot pr10 f plot.dos
$ open fplot.ps
The two panels look very similar.
 Notes:

 the final state is better described in terms the selfconsistent density in the presence of a core hole (sudden approximation). In other words, you should compute the matrix elements with the core partially occupied. We ignore that step here, but see this tutorial.
 the m resolved CLS should be calculated without symmetry operations, since the code does not rotate irreducible k points to the star of k [4] for CLS. See Further exercises.
4. Corelevel spectroscopy in the presence of a core hole in CrN
EELS, also known as corelevel spectroscopy, involves the excitation of a core electron to an excited state. In this tutorial we demonstrate corelevel spectroscopy for the N 1$s$ state, in CrN [5].
The selfconsistent calculation proceeds with an electron missing from the N 1$s$ core, which corresponds to the ‘sudden approximation’ (system relaxes instantaneously from electron ejected out of a core hole).
CrN input file
The electron should be ejected from a single, isolated N atom. We must use periodic boundary conditions, so we simulate it with a supercell of 4 N atoms, with one (Nh) differentiated as having a core hole.
This tutorial uses an alreadybuilt file from the source directory ~/lm. This file is essentially similar to the input used in Ref [5]. A tutorial detailing the steps required to generate a basic input file can be found here.
$ cp ~/lm/fp/test/ctrl.crn .
Inspect ctrl.crn, and note in particular this line in species Nh:
CHOLE=1s CHQ=1,1
These tags tell lmf to fractionally occupy the Nh $1s$ state, with one missing electron and a magnetic moment of −1.
Selfconsistent density in CrN
This test runs a little slowly, so we use lmf in the MPI mode. If you only have the serial mode installed, just remove mpirun 8
.
$ lmfa gas
$ mpirun n 8 lmf crn vnit=50
In the output of lmfa, the part concerning Nh, you should see a table like this:
Species Nh: Z=7 Qc=1 R=1.800000 Q=0 mom=1
mesh: rmt=1.800000 rmax=23.783012 a=0.03 nr=223 nr(rmax)=309
Add core hole: kcor=1 lcor=0 qcor=1 amom=1
Pl= 2.5 2.5 3.5 4.5 spn 2 2.5 2.5 3.5 4.5
Ql= 1.0 2.0 0.0 0.0 spn 2 1.0 2.0 0.0 0.0
The core charge has only one electron; the net magnetic moment of the system is −1 because the core hole has a magnetic moment.
lmf also indicates that a core hole is present. These lines of its output:
site 5 z= 7.0 rmt= 1.80000 nr=223 a=0.030 nlml=16 rg=0.450 Vfloat=T
core hole: kcor=1 lcor=0 qcor=1 amom=1
indicate that the core hole is present on atom 5 with principal and l quantum numbers 1 and 0, respectively.
lmf should converge to selfconsistency in 32 iterations and terminate with the following:
c nit=50 mmom=.775742 ehf=8797.2800063 ehk=8797.2800322
Corehole spectroscopy
You must specify a particular core level, which can be done in several ways. For CLS of the $1s$ state on Nh (the fifth atom), do:
mpirun n 8 lmf rs=1,0 cls:5,0,1 vnit=1 vmetal=2 vnk=8 crn
lmdos dos:cls:window=0,1:npts=1001 cls crn vnk=8
lmf makes weights and stores dos decorated by matrix elements in cls.crn. Some matrix elements are printed just before lmf exits:
CLS atom 5 (Nh) n=1 l=0
Spin 1 ..
vcdmel: ecor0=29.419700 ecore=29.419695
(not including electrostatic potential shift)
l <ucore> <score> <urcore> <srcore>
0 0.000090 0.000273 0.086293 0.081045
...
lmdos converts cls.crn weights into kintegrated spectra. You must supply lmdos with a switch telling it that this is a CLS calculation and also tell it to read data from file cls cls.crn. This file should contain three channels per spin. Convert the result into a more convenient form using the pldos utility:
$ echo .25 8 0 1  pldos fplot lst="1;3;5" lst2="2;4;6" dos.crn
It generates dosp.dat, easily read by standard graphics packages, and a script plot.dos file readable by the fplot graphics package in particular. Make and view a postscript figure of the CLS DOS:
$ fplot disp pr10 f plot.dos
$ open fplot.ps
Further exercises

For Cr_{3}Si_{6}, try improving the basis and see the effect on the DOS. Remove switches loc=0 mto=1 from the command line when running blm.

The x, y and z components of the CLS in Fe should be equivalent, but they are not, because wave functions are not rotated [5].
Rerun the calculation suppressing symmetry operations (lmf nosym and lmdos nosym) and confirm that they are essentially identical. Try also the CrN case. There the symmetry operations have no effect.
References

A. T. Paxton, M. van Schilfgaarde, M. MacKenzie and A. J. Craven, ``The Nearedge Structure in EnergyLoss Spectroscopy: ManyElectron and Magnetic Effects in Transition Metal Nitrides and Carbides,’’ J. Phys. Cond. Mat.12, 729 (2000).

Equation (1) only applies to noninteracting effective hamiltonians. In the interacting case the δfunction gets broadened, as described in this tutorial. It is similarly broadened in the Coherent Potential Approximation.

One decomposition of the DOS is to resolve the charge density by energy, or just evaluate the charge density for a single state. We do not consider such a decomposition in this tutorial.

That the Fe xy, xz, and yz DOS come out the same is nontrivial. To resolve DOS by m the full Brillouin zone must be used. lmf rotates the eigenstate at an irreducible point in the Brillouin to each point in the star of k, to accumulate partial DOS.
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