<div dir="ltr">Dear Jürg,<div><br></div><div><br></div><div>thank you for your detailed answer. This was very useful information,</div><div>in particular how to get an estimate of the total cutoff value,</div><div>this is very good to know. A number of things to try out now.</div><div><br></div><div><br></div><div>Cheers</div><div><br></div><div><br></div><div>Tobias</div><div><br></div><div><br><br>On Wednesday, June 11, 2014 1:46:55 PM UTC+1, jgh wrote:<blockquote class="gmail_quote" style="margin: 0;margin-left: 0.8ex;border-left: 1px #ccc solid;padding-left: 1ex;">Hi
<br>
<br>some info on cutoffs:
<br>
<br>- The relative cutoff is the minimal cutoff that is used to
<br> integrate a Gaussian with exponent 1. This scales linearly.
<br> Exponent a -> a*RelCutoff.
<br> 40 Rydberg usually gives reasonable results.
<br> 60 Rydberg should be close to 'convergence'.
<br> 80 Rydberg should always be converged.
<br> !!! Remember, convergence tests always also depend on other
<br> factors, like the Max. Cutoff, number of grids, how subgrids are
<br> calculated.
<br>
<br>- Estimate of total cutoff: Max. exponent in your basis set=a
<br> Cutoff = 2*a*Rel_cutoff
<br> This is usually way too high but can be used to work your way down
<br> to smaller cutoffs.
<br>
<br>- For larger systems (many atoms and electrons) and dense systems,
<br> CPU time is not dominated by the cutoff
<br>
<br>- For some GGA functionals convergence with Cutoff can be slow.
<br> Dirty trick: use one of the smoothing options (XC_GRID)
<br> Better: use higher cutoff for XC calculation only(testing needed)
<br>
<br>- Sometimes slow convergence with cutoff points to a problem with
<br> the GTH pseudopotentials and GGA functionals.
<br> There are NLCC pseudos available that solve this issue.
<br> -> more testing needed
<br>
<br>regards
<br>
<br>Juerg
<br>------------------------------<wbr>------------------------------<wbr>--
<br>Juerg Hutter <wbr> Phone : ++41 44 635 4491
<br>Institut für Chemie C FAX : ++41 44 635 6838
<br>Universität Zürich E-<wbr>mail: <a href="javascript:" target="_blank" gdf-obfuscated-mailto="BWbsbKuPFhEJ" onmousedown="this.href='javascript:';return true;" onclick="this.href='javascript:';return true;">hut...@chem.uzh.ch</a>
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<br>CH-8057 Zürich, Switzerland
<br>------------------------------<wbr>------------------------------<wbr>---
<br>
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<br>From: Tobias Kraemer <<a href="javascript:" target="_blank" gdf-obfuscated-mailto="BWbsbKuPFhEJ" onmousedown="this.href='javascript:';return true;" onclick="this.href='javascript:';return true;">161br...@gmail.com</a>>
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<br>Date: 06/10/2014 07:06PM
<br>Subject: [CP2K:5389] CUTTOFF and REL_CUTTOFF for large molecular system
<br>
<br>Dear CP2K group,
<br>
<br>
<br>being a relatively new cp2k user, I was wondering if this group could give me some advice on the choice of (REL) CUTOFF values.
<br>The system I am considering is a somewhat extended molecular crystal structure, containing organometallic fragments (basically a rhodium phosphine complex with additional ligand plus large borate counteranions (BArF4-).The full system contains about 600+ atoms in the unit cell, basically 4 cation/anion pairs
<br>(asymmetric units). I think the system cannot be reduced in size, and the full unit cell has to be taken into account.I have attached a cif file which gives you
<br>an idea about the kind of system (not exactly the one used in the calculation below, but very much related)
<br>
<br>The basic idea behind determining the CUTOFF is clear to me and I have done the tutorial on bulk Si. I have used the same protocol for my system
<br>(running a series of calculations with varying CUTOFF and REL_CUTOFF values). In contrast to the suggested method in the tutorial, I have
<br>fully converged the SCF cycle) Below are the (first) results of this series. The energy appears to be converging towards higher CUTOFF values (some more calculations are currently running)
<br>
<br>(1) I wonder if choosing such a large value for the cutoff is reasonable? It should also increase the accuracy of the calculations, but also the cost.
<br>Also, with respect to the number of Gaussian being mapped onto the finest grid, what would one need to look for?
<br>In the tutorial the decision was based on the fact that "the distribution of Gaussian functions on the grids are reasonable". Could somebody elaborate on this
<br>and give me some guidance how to decide this?
<br>(2) How does the size of the CUTOFF value correlate with the system size, if there is any correlation?
<br>(3) Are there some rule of thumbs as how to choose the REL_CUTOFF with respect to the CUTOFF? For now I have tried 30, 60 and 100 Ry.
<br>But I may need to go to higher numbers in this particular case.
<br>
<br>
<br>
<br># Grid cutoff vs total energy
<br># Date: Tue Jun 10 17:26:55 BST 2014
<br># REL_CUTOFF = 60
<br># Cutoff (Ry) | Total Energy (Ha) | Charge | SCF | | NG on grid 1 | NG on grid 2 | NG on grid 3 | NG on grid 4
<br> 50.00 -4583.1402739393 -8.4046446120 200 1623260 248362 2112 0
<br> 100.00 -4477.8479306771 -0.0745436930 128 1264867 519816 89051 0
<br> 150.00 -4479.5978060995 -0.0191170935 128 1150415 472845 248362 2112
<br> 200.00 -4478.5030451759 0.0008175249 128 905641 531280 432781 4032
<br> 250.00 -4478.4529157377 -0.0000917804 128 838757 500556 523109 11312
<br> 300.00 -4478.4141842105 -0.0000534995 128 796882 467985 519816 89051
<br> 350.00 -4478.3827319182 -0.0000170792 128 748308 474790 454036 196600
<br> 400.00 -4478.3597765363 0.0000003328 128 679828 499675 489931 204300
<br> 450.00 -4478.3498795935 0.0000000149 128 621687 528728 472845 250474
<br> 500.00 -4478.3399690553 0.0000000147 128 567997 416013 600098 289626
<br> 550.00 -4478.3338555119 -0.0000000007 128 485909 446314 559882 381629
<br> 600.00 -4478.3312330111 0.0000000007 128 442629 463012 531280 436813
<br> 650.00 -4478.3291405214 0.0000000006 128 399089 473084 554024 447537
<br> 700.00 -4478.3308119206 0.0000000008 128 375655 473218 509402 515459
<br> 750.00 -4478.3298871109 0.0000000008 128 365399 473358 500556 534421
<br> 800.00 -4478.3266993684 0.0000000007 128 353459 468098 461722 590455
<br> 850.00 -4478.3266987930 0.0000000007 128 348184 458373 472494 594683
<br> 900.00 -4478.3273848891 0.0000000007 128 336984 459898 467985 608867
<br> 950.00 -4478.3277135782 0.0000000007 128 309758 476872 469877 617227
<br> 1000.00 -4478.3277705414 0.0000000008 128 291089 482269 455857 644519
<br> 1050.00 -4478.3278605666 0.0000000007 128 229036 519272 474790 650636
<br>
<br>Some further questions;
<br>
<br>(4) Could you recommend some literature (books) which explains the theory of solid state calculations, k-sampling, planewaves?
<br>
<br>(5) As a next step I would like to manipulate the structure, i.e. rotate/move ligands around? Is there a good visualizer that can do such
<br>things for periodic systems? The problem I am facing is that I would like to do these things simultaneously for all 4 asymmetric units.
<br>I think it becomes impracticable to do this for each unit separately. I have started using GDIS but I am a little bit uncertain about its
<br>abilities (great program though!!). Has anyone experience with VESTA? I am particularly looking for free software.
<br>
<br>
<br>Thank you very much for your help, this is very much appreciated. There are a lot of questions right a the beginning, and it is not always easy to
<br>find some answers.
<br>
<br>Best
<br>
<br>
<br>Tobias
<br>
<br>
<br> Dr. Tobias Kraemer
<br> Research Associate
<br> Institute of Chemical Sciences
<br> School of Engineering & Physical Sciences
<br> Heriot-Watt University
<br> Edinburgh EH14 4AS
<br> United Kingdom
<br>
<br>
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<br>
<br>
<br>[attachment "input_test.inp" removed by Jürg Hutter/at/UZH]
<br>[attachment "PCCPiBu_NBA.cif" removed by Jürg Hutter/at/UZH]
<br></blockquote></div></div>