<html><head></head><body style="word-wrap: break-word; -webkit-nbsp-mode: space; -webkit-line-break: after-white-space; ">Sorry for continuously correcting myself... I realized that some PP on the website have atomic wavefunctions corresponding to atomic levels with occupations = 0 (see Au, for instance)... so I don't understand the logic for printing or not the wfcs in the PP file.<div><br></div><div>GS<br><div><div>Il giorno 12/nov/2010, alle ore 09.41, Gabriele Sclauzero ha scritto:</div><br class="Apple-interchange-newline"><blockquote type="cite"><div style="word-wrap: break-word; -webkit-nbsp-mode: space; -webkit-line-break: after-white-space; ">Dear Eduardo,<div><br></div><div> I think that the PP you are using does not include the 4p wavefunctions</div><div><span class="Apple-style-span" style="font-family: Times; "><pre style="word-wrap: break-word; white-space: pre-wrap; "><PP_HEADER>
0 Version Number
Ni Element
US Ultrasoft pseudopotential
T Nonlinear Core Correction
SLA PW PBE PBE PBE Exchange-Correlation functional
10.00000000000 Z valence
-72.87827664100 Total energy
0.0000000 0.0000000 Suggested cutoff for wfc and rho
2 Max angular momentum component
1203 Number of points in mesh
2 6 Number of Wavefunctions, Number of Projectors
Wavefunctions nl l occ
4S 0 1.00
3D 2 9.00
</PP_HEADER></pre><pre style="word-wrap: break-word; white-space: pre-wrap; "><br></pre></span><div>probably because the 4p states have 0 occupation and the ld1.x code stores in the PP file only atomic wavefunctions with occupation > 0. Hence the projections on the 4p atomic wavefunctions cannot be computed because they are not available to the code.</div><div>However, I think that the 4p wavefunctions are still computed by ld1.x when generating the PP, since there are beta projectors on the l=1 channel (grep BETA inside the PP file). You could try to modify the default behavior of ld1.x so that it will include those wavefunctions in the PP. Then the projection code should detect them in the PP data and compute the additional projections.</div><div><br></div><div><br></div><div>HTH</div><div><br></div><div>GS</div><div><br></div><div><div>Il giorno 11/nov/2010, alle ore 21.45, Eduardo Ariel Menendez Proupin ha scritto:</div><br class="Apple-interchange-newline"><blockquote type="cite"><div><div>Hi,</div><div>I am doing a tutorial example of calculation of the projected DOS in Ni. It produces the PDOS projected on S and D states, but not on P. </div><div>There are no bound P valence states in nickel. Is that the cause for not having a P partial DOS? </div>
<div><br></div><div>States with P-symmetry component may be present in an empty band. Is there an option to produce the P-PDOS?</div><div><br></div><div><br></div><div>Support information:</div><div>this is from the help file INPUT_PROJWFC.txt</div>
<div><br></div><div> In the collinear case and the non-collinear, non spin-orbit case</div><div> projected DOS are written to file "filpdos".pdos_atm#N(X)_wfc#M(l),</div><div> where N = atom number , X = atom symbol, M = wfc number, l=s,p,d,f</div>
<div> (one file per atomic wavefunction found in the pseudopotential file)</div></div><div><br></div><div><br></div><div>this is the head of the pseudopotential</div><div><PP_INFO></div><div>Generated using Andrea Dal Corso code (rrkj3) </div>
<div>Author: Andrea Dal Corso Generation date: unknown </div><div>Info: Ni </div><div> 1 The Pseudo was generated with a Scalar-Relativistic Calculation</div>
<div> 1.70000000000E+00 Local Potential cutoff radius</div><div>nl pn l occ Rcut Rcut US E pseu</div><div>4S 1 0 1.00 2.00000000000 2.50000000000 0.00000000000</div>
<div>4S 1 0 0.00 2.00000000000 2.50000000000 0.00000000000</div><div>4P 2 1 0.00 2.40000000000 2.60000000000 0.00000000000</div><div>4P 2 1 0.00 2.40000000000 2.60000000000 0.00000000000</div>
<div>3D 3 2 9.00 1.60000000000 2.50000000000 0.00000000000</div><div>3D 3 2 0.00 1.60000000000 2.50000000000 0.00000000000</div><div></PP_INFO></div><div><br></div><div><br></div>
Thanks<br>-- <br><div><br></div>
<div><br></div>Eduardo Menendez<br>Departamento de Fisica<br>Facultad de Ciencias<br>Universidad de Chile<br>Phone: (56)(2)9787439<br>URL: <a href="http://fisica.ciencias.uchile.cl/~emenendez" target="_blank">http://fisica.ciencias.uchile.cl/~emenendez</a>
<div><br></div>
<div>They did it!</div><br>
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<span class="Apple-style-span" style="border-collapse: separate; font-family: Helvetica; font-size: medium; font-style: normal; font-variant: normal; font-weight: normal; letter-spacing: normal; line-height: normal; orphans: 2; text-indent: 0px; text-transform: none; white-space: normal; widows: 2; word-spacing: 0px; -webkit-border-horizontal-spacing: 0px; -webkit-border-vertical-spacing: 0px; -webkit-text-decorations-in-effect: none; -webkit-text-size-adjust: auto; -webkit-text-stroke-width: 0px; "><div><span class="Apple-style-span" style="color: rgb(126, 126, 126); font-size: 16px; font-style: italic; "><br class="Apple-interchange-newline">§ Gabriele Sclauzero, EPFL SB ITP CSEA</span></div><div><font class="Apple-style-span" color="#7E7E7E"><i> PH H2 462, Station 3, CH-1015 Lausanne</i></font></div></span>
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<span class="Apple-style-span" style="border-collapse: separate; color: rgb(0, 0, 0); font-family: Helvetica; font-size: medium; font-style: normal; font-variant: normal; font-weight: normal; letter-spacing: normal; line-height: normal; orphans: 2; text-align: auto; text-indent: 0px; text-transform: none; white-space: normal; widows: 2; word-spacing: 0px; -webkit-border-horizontal-spacing: 0px; -webkit-border-vertical-spacing: 0px; -webkit-text-decorations-in-effect: none; -webkit-text-size-adjust: auto; -webkit-text-stroke-width: 0px; "><div><span class="Apple-style-span" style="color: rgb(126, 126, 126); font-size: 16px; font-style: italic; "><br class="Apple-interchange-newline">§ Gabriele Sclauzero, EPFL SB ITP CSEA</span></div><div><font class="Apple-style-span" color="#7E7E7E"><i> PH H2 462, Station 3, CH-1015 Lausanne</i></font></div></span>
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