# Input File Description ## Program: ld1.x / / Quantum Espresso (version: 6.4)
> > ### TABLE OF CONTENTS INTRODUCTION &INPUT title | zed | atom | xmin | dx | rmax | beta | tr2 | iswitch | nld | rlderiv | eminld | emaxld | deld | rpwe | rel | lsmall | max_out_wfc | noscf | lsd | dft | latt | isic | rytoev_fact | cau_fact | vdw | prefix | verbosity | file_charge | config | relpert | rel_dist | write_coulomb AllElectronCards nwf | nl | n | l | oc | isw | jj &INPUTP zval | pseudotype | file_pseudopw | file_recon | lloc | rcloc | nlcc | new_core_ps | rcore | tm | rho0 | lpaw | which_augfun | rmatch_augfun | rmatch_augfun_nc | lsave_wfc | lgipaw_reconstruction | use_paw_as_gipaw | author | file_chi | file_beta | file_qvan | file_screen | file_core | file_wfcaegen | file_wfcncgen | file_wfcusgen PseudoPotentialGenerationCards nwfs | nls | nns | lls | ocs | ener | rcut | rcutus | jjs | &TEST nconf | file_pseudo | ecutmin | ecutmax | decut | rm | configts | lsdts | frozen_core | rcutv PseudoPotentialTestCards nwfts | elts | nnts | llts | octs | enerts | rcutts | rcutusts | iswts | jjts | Notes Output files written Recipes to reproduce old all-electron atomic results with the ld1 program ### INTRODUCTION
> >     Input data cards for ld1.x program:

> >     Always present:
> >       1   namelist &input
> >       1.1 optional cards for all-electron calculations

> >     Needed for PP generation:
> >       2   namelist &inputp
> >       2.1 additional cards for PP generation

> >     Needed for pseudo-potential (PP) test. optional for PP generation:
> >       3   namelist &test
> >       3.1 optional cards for PP test
## Namelist: &INPUT
This namelist is always needed !
title | CHARACTER
Status: | OPTIONAL
>      A string describing the job.
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Either:
zed | REAL
See: | atom
>     The nuclear charge (1 < zed < 100).

>     IMPORTANT:
>     Specify either zed OR atom, not both!
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atom | CHARACTER
See: | zed
>     Atomic symbol: atom='H', 'He', 'Be', etc.

>     IMPORTANT:
>     Specify either atom OR zed, not both!
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Radial grid parameters:
xmin | REAL
Default: | -7.0 if iswitch>1 or rel=0, -8.0 otherwise
See: | dx
>      Radial grid parameter.
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dx | REAL
Default: | 0.0125 if iswitch>1, 0.008 otherwise
>     Radial grid parameter.

>     The radial grid is: r(i+1) = exp(xmin+i*dx)/zed  a.u.
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rmax | REAL
Default: | 100.0 a.u.
>      Outermost grid point.
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beta | REAL
Default: | 0.2
>      parameter for potential mixing
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tr2 | REAL
Default: | 1e-14
>      convergence threshold for scf
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iswitch | INTEGER
Default: | 1
>     1    all-electron calculation
>     2    PP test calculation
>     3    PP generation
>     4    LDA-1/2 correction, needs a previously generated PP file
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Parameters for logarithmic derivatives:
nld | INTEGER
>      the number of logarithmic derivatives to be calculated
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rlderiv | REAL
>      radius (a.u.) at which logarithmic derivatives are calculated
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eminld, emaxld | REAL
>     Energy range (min, max energy, in Ry) at which
>     logarithmic derivatives are calculated.
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deld | REAL
>     Delta e (Ry) of energy for logarithmic derivatives.
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rpwe | REAL
Default: | rlderiv
>      radius (a.u.) at which partial wave expansions are calculated
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    If the above parameters are not specified, logarithmic
    derivatives and partial wave expansions are not calculated.
rel | INTEGER
Default: | 0 for Z <= 18; 1 for Z > 18
>     0 ... non relativistic calculation
>     1 ... scalar relativistic calculation
>     2 ... full relativistic calculation with spin-orbit
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lsmall | LOGICAL
Default: | .false.
>     if .true. writes on files the small component
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max_out_wfc | INTEGER
Default: | 7
>     Maximum number of atomic wavefunctions written in the output
>     file.
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noscf | LOGICAL
Default: | .false.
>     if .true. the charge is not computed. The occupations are
>     not used and the eigenvalues and eigenfunctions are those
>     of a hydrogen-like atom.
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lsd | INTEGER
Default: | 0
>     0 ... non spin polarized calculation
>     1 ... spin-polarized calculation

>     BEWARE:
>     not allowed if iswitch=3 (PP generation) or with full
>     relativistic calculation
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dft | CHARACTER
>     Exchange-correlation functional.

>     Examples:
>     'PZ'    Perdew and Zunger formula for LDA
>     'PW91'  Perdew and Wang GGA
>     'BP'    Becke and Perdew GGA
>     'PBE'   Perdew, Becke and Ernzerhof GGA
>     'BLYP'  ...

>     For the complete list, see module "functionals" in ../Modules/
>     The default is 'PZ' for all-electron calculations,
>     it is read from the PP file in a PP calculation.
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latt | INTEGER
Default: | 0
>     0 ... no Latter correction
>     1 ... apply Latter correction
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isic | INTEGER
Default: | 0
Status: | only for all-electron calculation
>     0 ... no Self-interaction correction
>     1 ... apply Self-interaction correction
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rytoev_fact | REAL
Default: | as specified in file Modules/constants.f90
>     Factor used to convert Ry into eV.
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cau_fact | REAL
Default: | as specified in file Modules/constants.f90
>     Speed of light in a.u..

>     (Be careful the default value is always used in the
>      relativistic exchange.)
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vdw | LOGICAL
Default: | .false.
Status: | Gradient-corrected DFT not yet implemented.
>     If .true., the frequency dependent polarizability and van der
>     Waals coefficient C6 will be computed in Thomas-Fermi and
>     von Weizsaecker approximation(only for closed-shell ions).
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prefix | CHARACTER
Default: | 'ld1'
>     Prefix for file names - only for output file names
>     containing the orbitals, logarithmic derivatives, tests
>     See below for file names and the content of the file.
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verbosity | CHARACTER
Default: | 'low'
>     'low' or 'high'

>     if 'high' with iswitch=2,3 prints separately core and
>     valence contributions to the energies. Print the
>     frozen-core energy.
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file_charge | CHARACTER
Default: | ' '
>     Name of the file where the code writes the all-electron
>     total charge. No charge is written if file_charge=' '.
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config | CHARACTER
Default: | ' '
>     A string with the electronic configuration.

>     Example:
>       '[Ar] 3d10 4s2 4p2.5'

>     * If lsd=1, spin-up and spin-down state may appear twice
>       with the respective occupancy: 3p4 3p2 = 4 up,
>       2 down. Otherwise, the Hund's rule is assumed.

>     * If rel=2, states with jj=l-1/2 are filled first.
>       If a state appears twice, the first one has jj=l-1/2,
>       the second one jj=l+1/2 (except S states)
>       (Use rel_dist if you want to average the electrons
>       over all available states.)

>     * If config='default' the code uses zed to set the ground
>       state electronic configuration for the atom.

>     Negative occupancies are used to flag unbound states;
>     they are not actually used.
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relpert | LOGICAL
Default: | .false.
>     If .true. the relativistic corrections to the non-relativistic
>     Kohn-Sham energy levels (rel=0 .and. lsd=0) are computed using
>     first-order perturbation theory in all-electron calculations.
>     The corrections consist of the following terms:
>        E_vel: velocity (p^4) correction
>        E_Dar: Darwin term
>        E_S-O: spin-orbit coupling
>     The spin-orbit term vanishes for s-electron states and gives
>     rise to a splitting of (2*l+1)*E_S-O for the other states.
>     The separate contributions are printed only if verbosity='high'.

>     Formulas and notation are based on the Herman-Skillman book:
>     F. Herman and S. Skillman, "Atomic Structure Calculations",
>     Prentice-Hall, Inc., Englewood Cliffs, New Jersey, 1963
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rel_dist | CHARACTER
Default: | 'energy'
>     'energy' or 'average'

>     * if 'energy' the relativistic l-1/2 states are filled first.

>     * if 'average' the electrons are uniformly distributed
>       among all the states with the given l.
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write_coulomb | LOGICAL
Default: | .false.
>     If .true., a fake pseudo-potential file with name X.UPF,
>     where X is the atomic symbol, is written. It contains
>     the radial grid and the wavefunctions as specified in input,
>     plus the info needed to build the Coulomb potential
>     for an all-electron calculation - for testing only.
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## Card: AllElectronCards
If config is empty the electronic configuration is read from the following cards:
> IF `rel < 2 :`
> > ### Syntax: nwf
> > nl(1) | n(1) | l(1) | oc(1) | isw(1)
> > nl(2) | n(2) | l(2) | oc(2) | isw(2)
> > . . .
> > nl(nwf) | n(nwf) | l(nwf) | oc(nwf) | isw(nwf)
> ELSEIF `rel = 2 :`
> > ### Syntax: nwf
> > nl(1) | n(1) | l(1) | oc(1) | jj(1)
> > nl(2) | n(2) | l(2) | oc(2) | jj(2)
> > . . .
> > nl(nwf) | n(nwf) | l(nwf) | oc(nwf) | jj(nwf)
> ### Description of items:
> nwf | INTEGER
> >     number of wavefunctions
> [Back to Top]
> nl | CHARACTER
> >      wavefunction label (e.g. 1s, 2s, etc.)
> [Back to Top]
> n | INTEGER
> >      principal quantum number
> [Back to Top]
> l | INTEGER
> >      angular quantum number
> [Back to Top]
> oc | REAL
> >      occupation number
> [Back to Top]
> isw | INTEGER
> >      the spin index (1-2) used only in the lsda case
> [Back to Top]
> jj | REAL
> >     The total angular momentum (0.0 is allowed for complete
> >     shells: the codes fills 2l states with jj=l-1/2,
> >     2l+2 with jj=l+1/2).
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## Namelist: &INPUTP
zval | REAL
Default: | (calculated)
>     Valence charge.

>     zval is automatically calculated from available data.
>     If the value of zval is provided in input, it will be
>     checked versus the calculated value. The only case in
>     which you need to explicitly provide the value of zval
>     for noninteger zval (i.e. half core-hole pseudo-potentials).
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pseudotype | INTEGER
>     1 ... norm-conserving, single-projector PP
>           IMPORTANT: if pseudotype=1 all calculations are done
>           using the SEMILOCAL form, not the separable nonlocal form

>     2 ... norm-conserving PP in separable form (obsolescent)
>           All calculations are done using SEPARABLE non-local form
>           IMPORTANT: multiple projectors allowed but not properly
>           implemented, use only if you know what you are doing

>     3 ... ultrasoft PP or PAW
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file_pseudopw | CHARACTER
Status: | REQUIRED
>     File where the generated PP is written.

>     * if the file name ends with "upf" or "UPF",
>     or in any case for spin-orbit PP (rel=2),
>     the file is written in UPF format;

>     * if the file name ends with 'psp' it is
>     written in native CPMD format (this is currently
>     an experimental feature); otherwise it is written
>     in the old "NC" format if pseudotype=1, or
>     in the old RRKJ format if pseudotype=2 or 3
>     (no default, must be specified).
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file_recon | CHARACTER
Default: | ' '
>     File containing data needed for GIPAW reconstruction
>     of all-electron wavefunctions from PP results.
>     If you want to use additional states to perform the
>     reconstruction, add them at the end of the list
>     of all-electron states.
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lloc | INTEGER
Default: | -1
>     Angular momentum of the local channel.

>     * lloc=-1 or lloc=-2 pseudizes the all-electron potential
>       if lloc=-2 the original recipe of Troullier-Martins
>       is used (zero first and second derivatives at r=0)
>     * lloc>-1 uses the corresponding channel as local PP

>     NB: if lloc>-1, the corresponding channel must be the last in the
>     list of wavefunctions appearing after the namelist &inputp
>     In the relativistic case, if lloc > 0 both the j=lloc-1/2 and
>     the j=lloc+1/2 wavefunctions must be at the end of the list.
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rcloc | REAL
Status: | Must be specified only if lloc=-1, otherwise the corresponding value of rcut is used.
>     Matching radius (a.u.) for local pseudo-potential (no default).
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nlcc | LOGICAL
Default: | .false.
>     If .true. produce a PP with the nonlinear core
>     correction of Louie, Froyen, and Cohen
>     [PRB 26, 1738 (1982)].
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new_core_ps | LOGICAL
Default: | .false.
Status: | requires nlcc=.true.
>     If .true. pseudizes the core charge with bessel functions.
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rcore | REAL
>     Matching radius (a.u.) for the smoothing of the core charge.
>     If not specified, the matching radius is determined
>     by the condition:  rho_core(rcore) = 2*rho_valence(rcore)
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tm | LOGICAL
Default: | .false.
>     * .true. for Troullier-Martins pseudization [PRB 43, 1993 (1991)]

>     * .false. for Rappe-Rabe-Kaxiras-Joannopoulos pseudization
>       [PRB 41, 1227 (1990), erratum PRB 44, 13175 (1991)]
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rho0 | REAL
Default: | 0.0
>     Charge at the origin: when the Rappe-Rabe-Kaxiras-Joannopoulos
>     method with 3 Bessel functions fails, specifying rho0 > 0
>     may allow to override the problem (using 4 Bessel functions).
>     Typical values are in the order of 0.01-0.02
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lpaw | LOGICAL
Default: | .false.
>     If .true. produce a PAW dataset, experimental feature
>     only for pseudotype=3
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which_augfun | CHARACTER
Default: | `'AE'` for Vanderbilt-Ultrasoft pseudo-potentials and 'BESSEL' for PAW datasets.
>     If different from 'AE' the augmentation functions are pseudized
>     before rmatch_augfun. The pseudization options are:

>     * 'PSQ'        Use Bessel functions to pseudize Q
>                    from the origin to rmatch_augfun.

>     These features are available only for PAW:

>     * 'BESSEL'     Use Bessel functions to pseudize the Q.
>     * 'GAUSS'      Use 2 Gaussian functions to pseudize the Q.
>     * 'BG'         Use original Bloechl's recipe with a single gaussian.

>     Note: if lpaw is true and which_augfun is set to AE real all-
>     electron charge will be used, which will produce extremely
>     hard augmentation.
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rmatch_augfun | REAL
Default: | 0.5 a.u.
Status: | Used only if which_augfun is different from 'AE'.
>     Pseudization radius for the augmentation functions. Presently
>     it has the same value for all L.
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rmatch_augfun_nc | REAL
Default: | .false.
Status: | Used only if which_augfun is 'PSQ'.
>     If .true. the augmentation functions are pseudized
>     from the origin to min(rcut(ns),rcut(ns1)) where ns
>     and ns1 are the two channels for that Q. In this case
>     rmatch_augfun is not used.
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lsave_wfc | LOGICAL
Default: | .false. if .not. lpaw, otherwise .true.
>     Set it to .true. to save all-electron and pseudo wavefunctions
>     used in the pseudo-potential generation in the UPF file. Only
>     works for UPFv2 format.
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lgipaw_reconstruction | LOGICAL
Default: | .false.
>     Set it to .true. to generate pseudo-potentials containing the
>     additional info required for reconstruction of all-electron
>     orbitals, used by GIPAW. You will typically need to specify
>     additional projectors beyond those used in the generation of
>     pseudo-potentials. You should also specify file_recon.

>     All projectors used in the reconstruction must be listed BOTH
>     in the test configuration after namelist &test AND in the
>     all-electron configuration (variable 'config', namelist &inputp,
>     Use negative occupancies for projectors on unbound states). The
>     core radii in the test configuration should be the same as in
>     the pseudo-potential generation section and will be used as the
>     radius of reconstruction. Projectors not used to generate the
>     pseudo-potential should have zero occupation number.
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use_paw_as_gipaw | LOGICAL
Default: | .false.
>     When generating a PAW dataset, setting this option to .true. will
>     save the core all-electron wavefunctions to the UPF file.
>     The GIPAW reconstruction to be performed using the PAW data and
>     projectors for the valence wavefunctions.

>     In the default case, the GIPAW valence wavefunction and projectors
>     are independent from the PAW ones and must be then specified as
>     explained above in lgipaw_reconstruction.

>     Setting this to .true. always implies lgipaw_reconstruction = .true.
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author | CHARACTER
Default: | 'anonymous'
>      Name of the author.
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file_chi | CHARACTER
Default: | ' '
>      file containing output PP chi functions
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file_beta | CHARACTER
Default: | ' '
>      file containing output PP beta functions
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file_qvan | CHARACTER
Default: | ' '
>      file containing output PP qvan functions
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file_screen | CHARACTER
Default: | ' '
>      file containing output screening potential
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file_core | CHARACTER
Default: | ' '
>      file containing output total and core charge
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file_wfcaegen | CHARACTER
Default: | ' '
>      file with the all-electron wfc for generation
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file_wfcncgen | CHARACTER
Default: | ' '
>      file with the norm-conserving wfc for generation
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file_wfcusgen | CHARACTER
Default: | ' '
>      file with the ultra-soft wfc for generation
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## Card: PseudoPotentialGenerationCards
> IF `rel=0 OR rel=2 :`
> > ### Syntax: nwfs
> > nls(1) | nns(1) | lls(1) | ocs(1) | ener(1) | rcut(1) | rcutus(1) | jjs(1)
> > nls(2) | nns(2) | lls(2) | ocs(2) | ener(2) | rcut(2) | rcutus(2) | jjs(2)
> > . . .
> > nls(nwfs) | nns(nwfs) | lls(nwfs) | ocs(nwfs) | ener(nwfs) | rcut(nwfs) | rcutus(nwfs) | jjs(nwfs)
>     * if lloc>-1 the state with lls=lloc must be the last

>     * if lloc>0 in the relativistic case, both states with jjs=lloc-1/2
>       and jjs=lloc+1/2 must be the last two
> ELSE
> > ### Syntax: nwfs
> > nls(1) | nns(1) | lls(1) | ocs(1) | ener(1) | rcut(1) | rcutus(1)
> > nls(2) | nns(2) | lls(2) | ocs(2) | ener(2) | rcut(2) | rcutus(2)
> > . . .
> > nls(nwfs) | nns(nwfs) | lls(nwfs) | ocs(nwfs) | ener(nwfs) | rcut(nwfs) | rcutus(nwfs)
> ### Description of items:
> nwfs | INTEGER
> >      number of wavefunctions to be pseudized
> [Back to Top]
> nls | CHARACTER
> >     Wavefunction label (same as in the all-electron configuration).
> [Back to Top]
> nns | INTEGER
> >     Principal quantum number (referred to the PSEUDOPOTENTIAL case;
> >     nns=1 for lowest s, nns=2 for lowest p, and so on).
> [Back to Top]
> lls | INTEGER
> >      Angular momentum quantum number.
> [Back to Top]
> ocs | REAL
> >      Occupation number  (same as in the all-electron configuration).
> [Back to Top]
> ener | REAL
> >     Energy (Ry) used to pseudize the corresponding state.
> >     If 0.d0, use the one-electron energy of the all-electron state.
> >     Do not use 0.d0 for unbound states!
> [Back to Top]
> rcut | REAL
> >      Matching radius (a.u.) for norm conserving PP.
> [Back to Top]
> rcutus | REAL
> >      Matching radius (a.u.) for ultrasoft PP - only for pseudotype=3.
> [Back to Top]
> jjs | REAL
> >      The total angular momentum (0.0 is allowed for complete shells).
[Back to Top]
## Namelist: &TEST
needed only if iswitch=2 or iswitch=4, optional if iswitch=3
nconf | INTEGER
Default: | 1
>      the number of configurations to be tested. For iswitch = 4 nconf=2
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file_pseudo | CHARACTER
Default: | ' '
Status: | ignored if iswitch=3
>     File containing the PP.

>     * If the file name contains  ".upf" or ".UPF",
>     the file is assumed to be in UPF format;

>     * else if the file name contains ".rrkj3" or ".RRKJ3",
>     the old RRKJ format is first tried;

>     * otherwise, the old NC format is read.

>     IMPORTANT: in the latter case, all calculations are done
>     using the SEMILOCAL form, not the separable nonlocal form.
>     Use the UPF format if you want to test the separable form!
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ecutmin, ecutmax, decut | REAL
Default: | decut=5.0 Ry; ecutmin=ecutmax=0Ry
Status: | specify ecutmin and ecutmax if you want to perform this test
>     Parameters (Ry) used for test with a basis set of spherical
>     Bessel functions j_l(qr) . The hamiltonian at fixed scf
>     potential is diagonalized for various values of ecut:
>     ecutmin, ecutmin+decut, ecutmin+2*decut ... up to ecutmax.
>     This yields an indication of convergence with the
>     corresponding plane-wave cutoff in solids, and shows
>     in an unambiguous way if there are "ghost" states
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rm | REAL
Default: | 30 a.u.
>      Radius of the box used with spherical Bessel functions.
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configts(i), i=1,nconf | CHARACTER
>     A string containing the test valence electronic
>     configuration nc, nc=1,nconf. Same syntax as for "config".
>     If configts(i) is not set, the electron configuration
>     is read from the cards following the namelist.
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lsdts(i), i=1,nconf | INTEGER
Default: | 1
See: | lsd
>     0 or 1. It is the value of lsd used in the i-th test.
>     Allows to make simultaneously spin-polarized and
>     spin-unpolarized tests.
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frozen_core | LOGICAL
Default: | .false.
>     If .true. only the core wavefunctions of the first
>     configuration are calculated. The eigenvalues, orbitals
>     and energies of the other configurations are calculated
>     with the core of the first configuration.
>     The first configuration must be spin-unpolarized.
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rcutv | REAL
Default: | -1.0
>     Cutoff distance (CUT) for the inclusion of LDA-1/2 potential.
>                       Needed (mandatory) only if iswitch = 4
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## Card: PseudoPotentialTestCards
IMPORTANT: this card has to be specified for each missing configts(i)
> IF `lsd=1 :`
> > ### Syntax: nwfts
> > elts(1) | nnts(1) | llts(1) | octs(1) | enerts(1) | rcutts(1) | rcutusts(1) | iswts(1)
> > elts(2) | nnts(2) | llts(2) | octs(2) | enerts(2) | rcutts(2) | rcutusts(2) | iswts(2)
> > . . .
> > elts(nwfts) | nnts(nwfts) | llts(nwfts) | octs(nwfts) | enerts(nwfts) | rcutts(nwfts) | rcutusts(nwfts) | iswts(nwfts)
> ELSEIF `rel=2 :`
> > ### Syntax: nwfts
> > elts(1) | nnts(1) | llts(1) | octs(1) | enerts(1) | rcutts(1) | rcutusts(1) | jjts(1)
> > elts(2) | nnts(2) | llts(2) | octs(2) | enerts(2) | rcutts(2) | rcutusts(2) | jjts(2)
> > . . .
> > elts(nwfts) | nnts(nwfts) | llts(nwfts) | octs(nwfts) | enerts(nwfts) | rcutts(nwfts) | rcutusts(nwfts) | jjts(nwfts)
> ELSE
> > ### Syntax: nwfts
> > elts(1) | nnts(1) | llts(1) | octs(1) | enerts(1) | rcutts(1) | rcutusts(1)
> > elts(2) | nnts(2) | llts(2) | octs(2) | enerts(2) | rcutts(2) | rcutusts(2)
> > . . .
> > elts(nwfts) | nnts(nwfts) | llts(nwfts) | octs(nwfts) | enerts(nwfts) | rcutts(nwfts) | rcutusts(nwfts)
> ### Description of items:
> nwfts | INTEGER
> >      number of wavefunctions
> [Back to Top]
> elts | CHARACTER
> See: | nls
> [Back to Top]
> nnts | INTEGER
> See: | nns
> [Back to Top]
> llts | INTEGER
> See: | lls
> [Back to Top]
> octs | REAL
> See: | ocs
> [Back to Top]
> enerts | REAL
> Status: | not used
> [Back to Top]
> rcutts | REAL
> Status: | not used
> [Back to Top]
> rcutusts | REAL
> Status: | not used
> [Back to Top]
> iswts | INTEGER
> >      spin index (1 or 2, used in lsda case)
> [Back to Top]
> jjts | REAL
> >      total angular momentum of the state
[Back to Top]
> > ### Notes
> >     For PP generation you do not need to specify namelist &test, UNLESS:

> >     1. you want to use a different configuration for unscreening wrt the
> >     one used to generate the PP. This is useful for PP with semicore
> >     states: use semicore states ONLY to produce the PP, use semicore
> >     AND valence states (if occupied) to make the unscreening

> >     2. you want to specify some more states for PAW style reconstruction of
> >     all-electron orbitals from pseudo-orbitals
> > > #### Output files written
> > >     * file_tests            "prefix".test    results of transferability test

> > >     for each testing configuration N:

> > >     * file_wavefunctions    "prefix"N.wfc     all-electron KS orbitals
> > >     * file_wavefunctionsps  "prefix"Nps.wfc   pseudo KS orbitals

> > >     if lsd=1:

> > >     * file_wavefunctions    "prefix"N.wfc.up  all-electron KS up orbitals
> > >     * file_wavefunctions    "prefix"N.wfc.dw  all-electron KS down orbitals

> > >     if rel=2 and lsmall=.true.:

> > >     * file_wavefunctions    "prefix".wfc.small  all-electron KS small component

> > >     if parameters for logarithmic derivatives are specified:

> > >     * file_logder           "prefix"Nps.dlog  all-electron logarithmic derivatives
> > >     * file_logderps         "prefix"Nps.dlog  pseudo logarithmic derivatives

> > >     "N" is not present if there is just one testing configuration.
> > > #### Recipes to reproduce old all-electron atomic results with the ld1 program
> > >     * The Hartree results in Phys. Rev. 59, 299 (1940) or in
> > >       Phys. Rev. 59, 306 (1940) can be reproduced with:

> > >         rel=0,
> > >         isic=1,
> > >         dft='NOX-NOC'

> > >     * The Herman-Skillman tables can be reproduced with:

> > >         rel=0,
> > >         isic=0,
> > >         latt=1,
> > >         dft='SL1-NOC'

> > >     * Data on the paper Liberman, Waber, Cromer Phys. Rev. 137, A27 (1965) can be
> > >     reproduced with:

> > >         rel=2,
> > >         isic=0,
> > >         latt=1,
> > >         dft='SL1-NOC'

> > >     * Data on the paper S. Cohen Phys. Rev. 118, 489 (1960) can be reproduced with:

> > >         rel=2,
> > >         isic=1,
> > >         latt=0,
> > >         dft='NOX-NOC'

> > >     * The revised PBE described in PRL 80, 890 (1998) can be obtained with:

> > >         isic=0
> > >         latt=0
> > >         dft='SLA-PW-RPB-PBC' or 'dft='revPBE'

> > >     * The relativistic energies of closed shell atoms reported in PRB 64 235126 (2001)
> > >     can be reproduced with:

> > >         isic=0
> > >         latt=0
> > >         cau_fact=137.0359895
> > >         dft='sla-vwn' for the LDA case
> > >         dft='PBE'     for the PBE case

> > >     * The NIST results in PRA 55, 191 (1997):

> > >         LDA:
> > >             rel=0
> > >             dft='sla-vwn'

> > >         LSD:
> > >             rel=0
> > >             lsd=1
> > >             dft='sla-vwn'

> > >         RLDA
> > >             rel=2
> > >             rel_dist='average'
> > >             dft='rxc-vwn'

> > >         ScRLDA:
> > >             rel=1
> > >             dft='rxc-vwn'

This file has been created by helpdoc utility on Fri Mar 01 17:58:47 CET 2019.