Hi Giu, it worked!

Jonas Baltrusaitis
Posts
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fractional coordinate entry -
fractional coordinate entryHi all, I am not getting the right geometry inputs for 1/3 and 2/3 positions. For example, for the structure below, I am trying to enter for the group 164:
CRYSTAL
0 0 0
164
3.186 4.653
3
27 0.0 0.0 0.0
1 0.333 0.6666 0.4134
8 0.3333 0.666 0.2128and it ends up being incorrect stoichiometry, which tells me these fractional positions were not parsed correctly.
CRYSTAL CALCULATION
(INPUT ACCORDING TO THE INTERNATIONAL TABLES FOR X-RAY CRYSTALLOGRAPHY)
CRYSTAL FAMILY : HEXAGONAL
CRYSTAL CLASS (GROTH - 1921) : DITRIGONAL SCALENOHEDRALSPACE GROUP (CENTROSYMMETRIC) : P -3 M 1
LATTICE PARAMETERS (ANGSTROMS AND DEGREES) - CONVENTIONAL CELL
A B C ALPHA BETA GAMMA
3.18600 3.18600 4.65300 90.00000 90.00000 120.00000NUMBER OF IRREDUCIBLE ATOMS IN THE CONVENTIONAL CELL: 3
INPUT COORDINATES
ATOM AT. N. COORDINATES
1 27 0.000000000000E+00 0.000000000000E+00 0.000000000000E+00
2 1 3.330000000000E-01 6.666000000000E-01 4.134000000000E-01
3 8 3.333000000000E-01 6.660000000000E-01 2.128000000000E-01
<< INFORMATION >>: FROM NOW ON, ALL COORDINATES REFER TO THE PRIMITIVE CELL
LATTICE PARAMETERS (ANGSTROMS AND DEGREES) - PRIMITIVE CELL
A B C ALPHA BETA GAMMA VOLUME
3.18600 3.18600 4.65300 90.00000 90.00000 120.00000 40.903006COORDINATES OF THE EQUIVALENT ATOMS (FRACTIONAL UNITS)
N. ATOM EQUIV AT. N. X Y Z
1 1 1 27 CO 0.00000000000E+00 0.00000000000E+00 0.00000000000E+00
2 2 1 1 H 3.33000000000E-01 -3.33400000000E-01 4.13400000000E-01
3 2 2 1 H 3.33400000000E-01 -3.33600000000E-01 4.13400000000E-01
4 2 3 1 H 3.33600000000E-01 -3.33000000000E-01 4.13400000000E-01
5 2 4 1 H -3.33600000000E-01 3.33400000000E-01 -4.13400000000E-01
6 2 5 1 H -3.33000000000E-01 3.33600000000E-01 -4.13400000000E-01
7 2 6 1 H -3.33400000000E-01 3.33000000000E-01 -4.13400000000E-01
8 2 7 1 H -3.33000000000E-01 3.33400000000E-01 -4.13400000000E-01
9 2 8 1 H -3.33400000000E-01 3.33600000000E-01 -4.13400000000E-01
10 2 9 1 H -3.33600000000E-01 3.33000000000E-01 -4.13400000000E-01
11 2 10 1 H 3.33600000000E-01 -3.33400000000E-01 4.13400000000E-01
12 2 11 1 H 3.33000000000E-01 -3.33600000000E-01 4.13400000000E-01
13 2 12 1 H 3.33400000000E-01 -3.33000000000E-01 4.13400000000E-0114 3 1 8 O 3.33300000000E-01 -3.34000000000E-01 2.12800000000E-01
15 3 2 8 O 3.34000000000E-01 -3.32700000000E-01 2.12800000000E-01
16 3 3 8 O 3.32700000000E-01 -3.33300000000E-01 2.12800000000E-01
17 3 4 8 O -3.32700000000E-01 3.34000000000E-01 -2.12800000000E-01
18 3 5 8 O -3.33300000000E-01 3.32700000000E-01 -2.12800000000E-01
19 3 6 8 O -3.34000000000E-01 3.33300000000E-01 -2.12800000000E-01
20 3 7 8 O -3.33300000000E-01 3.34000000000E-01 -2.12800000000E-01
21 3 8 8 O -3.34000000000E-01 3.32700000000E-01 -2.12800000000E-01
22 3 9 8 O -3.32700000000E-01 3.33300000000E-01 -2.12800000000E-01
23 3 10 8 O 3.32700000000E-01 -3.34000000000E-01 2.12800000000E-01
24 3 11 8 O 3.33300000000E-01 -3.32700000000E-01 2.12800000000E-01
25 3 12 8 O 3.34000000000E-01 -3.33300000000E-01 2.12800000000E-01 -
Is there a software to create DOS/BAND input?wonderful, thank you both
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Is there a software to create DOS/BAND input?thank you, this is very useful for me
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TREATMENT OF DISORDERED SYSTEMS / SOLID SOLUTIONS - perovskite structureHi, we synthesized a complex material something along the lines of LaFex Niy Coz Cuu Mnv O3 where x+y+z+u+n=1. I know it is not trivial, but I would like to attempt using configuration analysis in TREATMENT OF DISORDERED SYSTEMS / SOLID SOLUTIONS module to generate possible configurations. The parent compound is LaFeO3 perovskite structure. It is Pnma symmetry
Lattice (Primitive)
a 5.60 Å, b 5.66 Å, c 7.94 Å, α 90.00 º, β 90.00 º, ɣ 90.00 ºWyckoff Element x y z
4b Fe 1/2 0 1/2
4c La 0.009381 0.961741 3/4
4c O 0.08612 0.478265 1/4
8d O 0.712594 0.287975 0.453725so all the atom substitutions of Ni, Co, Cu and Mn will go into that 4b Fe site. From the analysis, it has 4 symmetry equivalent sites:
5 T 26 FE 0.000000000000E+00 0.000000000000E+00 -5.000000000000E-01 6 F 26 FE -5.000000000000E-01 0.000000000000E+00 -3.095458132887E-17 7 F 26 FE -5.000000000000E-01 -5.000000000000E-01 2.220446049250E-16 8 F 26 FE 0.000000000000E+00 -5.000000000000E-01 -5.000000000000E-01
I know the Fe composition, it is 20 %, the rest are Ni, Co, Cu and Mn, all at the same 20 % compositions - this simplifies the problem. But then I have 4 equivalent Fe sites and 5 elements to fit. Am I correct that I need to construct a supercell here? Ultimately, I would like this module to return me possible combinations of all 20% five elements, but not sure what size of supercell to create
see the attached test structure input.out INPUT.d12
thank you
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Is there a software to create DOS/BAND input?I admit I am not very good conceptualizing these symetry unique points on Brillouin zone or expressing them in .d3 file as a path. I have two structures below that I fully optimized and calculated vibrational frequencies. Now my task is DOS/BAND. Is there a GUI that would help me read the optimized structures and prepare .d3 file? Or can I use my optimization file somehow to extract those unique points?
SPACE GROUP (CENTROSYMMETRIC) : P 21/N
LATTICE PARAMETERS (ANGSTROMS AND DEGREES) - CONVENTIONAL CELL
A B C ALPHA BETA GAMMA
7.40400 21.53400 5.65700 90.00000 91.05000 90.00000and
SPACE GROUP (CENTROSYMMETRIC) : P -1
LATTICE PARAMETERS (ANGSTROMS AND DEGREES) - CONVENTIONAL CELL
A B C ALPHA BETA GAMMA
10.70800 10.11400 6.41000 91.30000 88.30000 91.00000 -
lots of negative energy DE in crystal with good gradientsDear all, I optimized a crystal, got good gradients, but numerical displacements are already suspect as they generate lots of negative energies, it's a big system, I am still running it but decided to preemptively ask why this can be the case?
SYMMETRY ALLOWED FORCES (COORDINATE, FORCE)
1 -7.1019812E-07 2 2.6847537E-07 3 1.7714543E-06 4 1.5380909E-06 5 -8.5713887E-07 6 -7.6313741E-07 7 -1.3777999E-06 8 -4.2292032E-07 9 3.7330006E-07 10 -1.0186152E-07 11 7.8436370E-08 12 -1.0666144E-07
13 7.6024231E-07 14 1.2549944E-07 15 -3.8114243E-07 16 8.3483245E-07
17 1.2719080E-06 18 1.3589256E-07 19 -1.2770755E-06 20 -1.7657611E-06
21 -6.7831105E-07 22 -2.8553633E-06 23 -2.5801301E-06 24 1.6190965E-06
25 2.7986374E-07 26 1.6445538E-06 27 1.5791380E-06 28 3.4913230E-06
29 7.5492284E-07 30 -3.2944974E-06 31 -2.9919538E-06 32 1.2296182E-06
33 4.5466078E-07 34 -1.8564773E-07 35 9.3158783E-07 36 -1.4184621E-07
37 2.8763484E-06 38 -1.7874331E-06 39 -3.3548919E-07 40 -1.0246636E-06
41 7.3025290E-07 42 -7.4914105E-07 43 -1.5527795E-07 44 -5.9189571E-07
45 1.1402401E-07 46 1.1445077E-07 47 5.0641463E-07 48 2.6720325E-07
49 3.9382990E-07 50 1.9265418E-07 51 -5.0025563E-07 52 -1.4722329E-07
53 -3.9032570E-07 54 -1.8660950E-07 55 -3.7294087E-08 56 2.7903845E-07
57 -1.1262719E-07 58 -1.4056720E-06 59 -7.2814440E-07 60 -4.2360016E-07
61 9.6760468E-07 62 -1.1476558E-06 63 5.7400637E-08 64 8.2334616E-07
65 1.7677814E-06 66 1.1935613E-06 67 -5.3996977E-07 68 5.3577787E-07
69 -5.5566146E-07 70 2.5231789E-07 71 -6.3487986E-07 72 7.2284427E-07
73 -8.4328694E-08 74 -5.8224781E-07 75 -1.6946265E-07 76 1.0209263E-06
77 2.9716506E-07 78 2.3838462E-07 79 1.7955521E-06 80 4.0804899E-07
81 1.2100282E-07 82 -1.5099145E-06 83 2.9006726E-07 84 -2.2790446E-07
85 1.4325087E-06 86 -6.8494225E-07 87 -3.3477344E-07 88 -2.2149944E-07
89 1.3328321E-07 90 -1.8330282E-08ATOM MAX ABS(DGRAD) TOTAL ENERGY (AU) N.CYC DE SYM
CENTRAL POINT -5.463640944184E+03 0 0.0000E+00 8
1 O DX 6.5777E-04 -5.463640944692E+03 11 -5.0781E-07 1
1 O DY 8.9722E-04 -5.463640943824E+03 12 3.6002E-07 1
1 O DZ 2.7715E-03 -5.463640938222E+03 13 5.9626E-06 1
9 O DX 1.4159E-03 -5.463640942796E+03 11 1.3886E-06 1
9 O DY 2.4328E-03 -5.463640939470E+03 13 4.7142E-06 1
9 O DZ 7.5341E-04 -5.463640944273E+03 10 -8.8837E-08 1
17 N DX 3.3298E-03 -5.463640936786E+03 9 7.3979E-06 1
17 N DY 2.6834E-03 -5.463640938932E+03 10 5.2525E-06 1
17 N DZ 2.2061E-03 -5.463640940002E+03 10 4.1826E-06 1
25 H DX 5.8163E-04 -5.463640944625E+03 10 -4.4035E-07 1
25 H DY 9.7068E-04 -5.463640943311E+03 9 8.7315E-07 1
25 H DZ 1.3265E-03 -5.463640942408E+03 11 1.7757E-06 1
33 H DX 1.9126E-03 -5.463640940840E+03 12 3.3445E-06 1
33 H DY 9.0051E-04 -5.463640944155E+03 9 2.8878E-08 1
33 H DZ 6.4300E-04 -5.463640945217E+03 9 -1.0328E-06 1
41 N DX 3.4011E-03 -5.463640936782E+03 10 7.4018E-06 1
41 N DY 2.7133E-03 -5.463640938661E+03 12 5.5236E-06 1
41 N DZ 2.8802E-03 -5.463640937601E+03 11 6.5830E-06 1
49 H DX 1.5489E-03 -5.463640941848E+03 10 2.3365E-06 1
49 H DY 3.3487E-04 -5.463640945255E+03 9 -1.0709E-06 1
49 H DZ 8.9868E-04 -5.463640943999E+03 9 1.8543E-07 1
57 N DX 2.4112E-03 -5.463640939472E+03 9 4.7126E-06 1
57 N DY 3.5207E-03 -5.463640936173E+03 10 8.0110E-06 1
57 N DZ 3.2454E-03 -5.463640936926E+03 12 7.2582E-06 1
65 H DX 4.2444E-04 -5.463640945298E+03 10 -1.1135E-06 1
65 H DY 1.4990E-03 -5.463640942117E+03 10 2.0672E-06 1
65 H DZ 9.8569E-04 -5.463640943558E+03 7 6.2581E-07 1
73 H DX 8.8996E-04 -5.463640943796E+03 11 3.8818E-07 1
73 H DY 4.0635E-04 -5.463640945249E+03 9 -1.0646E-06 1
73 H DZ 1.5526E-03 -5.463640941922E+03 11 2.2623E-06 1
81 N DX 3.0237E-03 -5.463640937800E+03 12 6.3840E-06 1
81 N DY 3.1621E-03 -5.463640937605E+03 12 6.5795E-06 1
81 N DZ 3.3672E-03 -5.463640936782E+03 11 7.4017E-06 1
89 H DX 3.5908E-04 -5.463640945209E+03 8 -1.0249E-06 1
89 H DY 1.0305E-03 -5.463640943313E+03 13 8.7074E-07 1
89 H DZ 1.3452E-03 -5.463640942571E+03 10 1.6132E-06 1
97 H DX 1.1682E-03 -5.463640943082E+03 10 1.1022E-06 1
97 H DY 1.4461E-03 -5.463640941923E+03 12 2.2616E-06 1output.out attached
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running JSmolI profusely apologize, but how do I visualize vibrations on my browser using JSMol? I know it sounds silly but I have no idea how to install or launch it. Your webpage below did it very well, I can't follow any of the Java related instructions on the developers website, I would like to be able to run JSmol on my home computer on a browser, can somebody give me a brief instruction how to do that?
Your tutorial page does that very well
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help with substitutional defects -
help with substitutional defectsHi Alessandro, working hard on this one. Scenario 3 seemed trivial (but did not converge). I assumed some JT distortion, so I used distortion along z axis argument and I shifted dxz down and assumed this is the double populated one. So far no luck in convergence
EIGSHIFT
5
1 8 1 -.5 .5
1 8 2 -.5 -.5
1 8 3 -.5 .5
1 8 4 -.5 .5
1 8 5 -.5 .5 -
help with substitutional defectsAlessandro,
I am making a large 450 atom supercell of MgNH4PO4*6H2O to study Fe ion incorporation. We experimntally observe about 5% Mg atoms substituted with Fe - we do not know the oxidation state. So my supercell is big and I optimize this ionic solid with PBE-D3. My question is long and related on how to obtain required electronic state and converge in some instances. See below my diagram. I am exploring 3 different substitutional scenarios.
Scenario 1 is substituting Fe3+ and removing one proton to make it neutral. I am getting excellent SCF convergence, my guess is that this octahedral symmetry is broken somehow by removal of proton which helps SCF convergnce but crystal field with nearly 5 inpaired electrons is still preserved after the convergence with PBE-D3/pobDZVP.
Scenario 2 is an SCF problem. To charge balance it I remove NH4+. Immediately I get problems with SCF becoming conducting, I guess it does not want to be perfectly Oh symmetry and needs some distortion. I managed to converged it with PBE-D3/STO-3G in hopes that it will optimize to some solution which I can further optimize with PBE-D3/pobDZVP. But if I wanted to bias it with EIGENSHIFT and start with a large basus set, what would be my logic here? Robert Orlando used to very elegantly explain these things to me in the past.
Scenario 3 I haven't run yet. Seems like perfect Oh symmetry with the corresponding crystal field splitting and 4 unpaired electrons but my guess is it will run into the same problems as Scenario 2 and will need some biasing.
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No space left on deviceI mean… those are huge HPC nodes… they can’t be possibly out of disk… But certainly I will try this, will it affect my convergence or calculation speed?
Thank you Alessandro
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No space left on deviceSo on my main supercomputer I am getting this error during write problem. Admins do not know why it happens. It only happes with CRYSTAL and sporadically.
CYC 23 ETOT(AU) -2.276909751322E+04 DETOT -2.19E-06 tst 4.04E-07 PX 2.29E-04
TTTTTTTTTTTTTTTTTTTTTTTTTTTTTT DIIS TELAPSE 20527.44 TCPU 20346.34
DIIS TEST: 0.38681E-05 AT SCF CYCLE 23 - DIIS ACTIVE - HISTORY: 23 CYCLES
forrtl: No space left on device
forrtl: severe (38): error during write, unit 8, file /90daydata/urea_kinetics/struvite/Fedoped/PBE_D3/2x2x2_FeOH/fort.8.pe280
Image PC Routine Line Source
Pcrystal 0000000007376772 Unknown Unknown Unknown
Pcrystal 00000000073744DB Unknown Unknown Unknown
Pcrystal 0000000001BA179E Unknown Unknown Unknown
Pcrystal 000000000069D509 Unknown Unknown Unknown
Pcrystal 0000000000695494 Unknown Unknown Unknown
Pcrystal 0000000000992FCD Unknown Unknown Unknown
Pcrystal 0000000000609584 Unknown Unknown Unknown
Pcrystal 0000000000605881 Unknown Unknown Unknown
Pcrystal 0000000000405540 Unknown Unknown Unknown
Pcrystal 00000000004053FD Unknown Unknown Unknown
libc.so.6 0000148B7AA295D0 Unknown Unknown Unknown
libc.so.6 0000148B7AA29680 __libc_start_main Unknown Unknown
Pcrystal 0000000000405315 Unknown Unknown Unknown -
ERROR **** PGGP **** G-VECTOR NOT FOUND IN PREVIOUS DENSITY MATRIXIt makes sense, thank you.
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ERROR **** PGGP **** G-VECTOR NOT FOUND IN PREVIOUS DENSITY MATRIXaerba I do not think this is true now that I have spent so much time restarting. I tried restarting frequency job with the old input (e.g. if I do PREOPTGEOM and it is optimized) and restart normally proceeds. I can take the last coordinate file and do EXTARENAL in the restart but in my experience did not matter, frequency restart always proceeds either way
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pov-TZVP vs old school basis setsAlessandro, the setback is temporary. What I really appreciate is that you gave CRYSTAL more life via user support than it ever had. I am very grateful for it
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pov-TZVP vs old school basis sets59 S 0.802 -8.631 2.894
567 S
6.070E+04 5.470E-04 0.000E+00 0.000E+00
9.103E+03 4.230E-03 0.000E+00 0.000E+00
2.071E+03 2.175E-02 0.000E+00 0.000E+00
5.860E+02 8.510E-02 0.000E+00 0.000E+00
1.906E+02 2.480E-01 0.000E+00 0.000E+00
6.763E+01 4.670E-01 0.000E+00 0.000E+00
2.513E+01 3.643E-01 0.000E+00 0.000E+00
568 S
1.126E+02 2.167E-02 0.000E+00 0.000E+00
3.480E+01 9.360E-02 0.000E+00 0.000E+00
6.512E+00-2.607E-01 0.000E+00 0.000E+00
569 S
3.240E+00 1.284E+00 0.000E+00 0.000E+00
1.548E+00 6.604E-01 0.000E+00 0.000E+00
570 S
4.487E-01 1.000E+00 0.000E+00 0.000E+00
571 S
1.553E-01 1.000E+00 0.000E+00 0.000E+00
572- 574 P
5.644E+02 0.000E+00 2.480E-03 0.000E+00
1.334E+02 0.000E+00 1.968E-02 0.000E+00
4.247E+01 0.000E+00 8.998E-02 0.000E+00
1.562E+01 0.000E+00 2.571E-01 0.000E+00
6.109E+00 0.000E+00 4.352E-01 0.000E+00
575- 577 P
2.036E+00 0.000E+00 1.000E+00 0.000E+00
578- 580 P
4.338E-01 0.000E+00 1.000E+00 0.000E+00
581- 583 P
1.305E-01 0.000E+00 1.000E+00 0.000E+00 -
pov-TZVP vs old school basis setsahem
pob-TZVP-rev2 -
Error in RESTART of FREQCALC calculationaerba said in Error in RESTART of FREQCALC calculation:
Hi,
I have run some calculations on your case following my step-by step recipe (as described at https://forum.crystalsolutions.eu/post/339, which I have now edited to include the intensity step), and the restart now works just fine (i.e. without the annoying "possibly conducting state", and with a nice convergence of the further SCFs upon restart).
This is what I did:
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I took the optimized geometry from your original output file and I created a new input file for a single-point calculation. I ran it and obtained the wavefunction external file (i.e. fort.9 unit);
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I prepared an input file to run the harmonic frequency calculation, I ran it and I killed it in the middle of the construction of the Hessian. From this incomplete frequency calculation, I obtained the FREQINFO.DAT file and the external unit with the density matrix, i.e. fort.13 unit;
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I prepared an input file to restart the frequency calculation and provided the FREQINFO.DAT and fort.13 files from the previous step and the fort.9 (renamed as fort.20) from the first step, and ran it. The calculation of the Hessian restarted correctly, with the new SCFs converging nicely (see the attached SCFOUT.LOG file). I then stopped the calculation not to use too much compute power on my cluster.
If you follow this step-by-step process you'll be able to safely restart your frequency calculations.
Hope this helps,
thank you and I am trying to do that
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pov-TZVP vs old school basis setsMy current activity on this forum is due to the need to calculate Raman spectra. This one is not a problem but more of an observation. For the longest time I thought that CRYSTAL had a basis set problem where basis sets were seemingly randomly optimized and there were many falvors of them and they wer nore standartized in terms of contractions (e.g. 6-31G*). I was very happy to find out that standard basis sets by Peintinger were created, e.g. pob-TZVP which I can simply specify with BASISSET. So in all of my recent work on Raman spectra I used them for simplicity and uniformity.
Fast forward, my calculated Raman peaks just do not have the right position. I understand there will be an intrinsic error in the calculated peak positions, but the peaks ere 150-200 cm-1 too low for a sulfate ion. So I looked back at CRYSTAL references that did Raman including Roberto's and noticed at that time they still used these old school basis sets. I was curious and for B3LYP-D3 (I have molecular crystals or ionic crystals) with pob-TZVP I recalculated everything with these large 8611 basis sets. Much to my dismay, these old school basis sets yielded calculated Raman peaks in the vicinity of the experimental, e.g. 150-200 cm-1 higher than pob-TZVP with everything else in the input the same.
This is not a cimplaint, I understand that frequency outcome will depend on the calculation setup, e.g. functional and basis set, but why would pob-TZVP be so spectacularly bad at these Raman vibrations?
See attached, blue is 86111 old school basis set and orange is pob-TZVP basis set - I have much more data with pob-TZVP (unfortunately).
Experimental SO4 vibration is around 920 cm-1 in this particular mineral