[SIESTA-L] V-I characteristics using LDA+U in Transiesta
Dear all, Can V-I characteristic be studied using LDA/GGA+U formalism in Transiesta and relevant utilities? bests, sonu * and With kind regards,* *S Kumar | PhD.*
Re: [SIESTA-L] OPTIMIZATION(ZnO)
For generating pseudo-potentials (norm-conserving), use ATOM program provided with SIESTA. But, be careful before using them for production runs, rather first test them (I advise to generate pseudopotentials only if it not available or the available one does not serve the purpose you want to use for). bests, kumar *With kind regards,* *S Kumar | PhD.*
Re: [SIESTA-L] Problem in installing siesta-4.0
undefined reference s to the routines of Lapack library are there => means you might not have installed lapack library or location of the libraries is not mentioned. Add the location of this library in arch.make file. Similary other libraries locations are to be added. Also, read about the installation instructions in siesta manual. *With kind regards,* *S Kumar | PhD.*
Re: [SIESTA-L] change DOS as increasing supercell size
Increasing supercell size changes the concentration of defects, that is why you see changes in DOS. bests, sonu *===* With kind regards, Dr. S Kumar, Post doctoral fellow Physical Sciences and Engineering Divison, IBN Sina Building, KAUST, Thuwal, KSA *===* On Tue, Aug 8, 2017 at 3:55 PM, MB MBwrote: > Dear SIESTA users, > > I really need your help. I am studying defects in MoS2 2D structures. > As I increase the size of the supercell from 5*5 to 8*8, the position of > defects states changes in DOS diagram > > I use DZP basis set and default values to create orbitals. > Is there any suggestion why this happens and how to fix it? > > Best regards > Mohammad Bahmani >
Re: [SIESTA-L] [***Posible SPAM***]
Please, make proper Heading of your mail. On Mon, Sep 8, 2014 at 3:13 PM, Manjeet Bhatia manjeetbhati...@gmail.com wrote: Dear Siesta Users, I am doing spin polarized calculations for Pt. I have used GGA pseudopotential provided by siesta but I am getting valance configuration 5d10 in my output file closed shell. initatom: Reading input for the pseudopotentials and atomic orbitals -- Species number:1 Label: Pt_GGA Atomic number: 78 Ground state valence configuration: 5d10 Reading pseudopotential information in formatted form from Pt_GGA.psf and Initializing Density Matrix... initdm: WARNING: atom 1 has a closed-shell and cannot be polarized Could you please let me know what parameters I have to change to get configuration 5d9 6s1 for spin calculation? Thanks.
Re: [SIESTA-L] [***Posible SPAM***]
Dear manjeet, For spin polarized calculations I need pseudopotential of Pt. Pseudo potential does not contain informations about spin, and are not generated with spin. Spin is added by using some tag in SIESTA, please see the spin DFT. Please let me know how can i find pseudopotential of this configuration [Xe] 4f14 5d9 6s1 for Pt? Why do you need f states in valence? d states should be taken in valence. Here is Pt.inp for atom taken from : http://departments.icmab.es/leem/siesta/Databases/Pseudopotentials/Pseudos_LDA_Abinit/Pt_html/Pt.html - pg -- file generated from Pt ps file tm2 Pt ca 0.000 0.000 0.000 0.000 0.000 0.000 124 60 1.000 0.000#6s 61 0.000 0.000#6p 52 9.000 0.000#5d 53 0.000 0.000#5f 2.6 2.73000 2.6 2.6 0.0 0.0 #23456789012345678901234567890123456789012345678901234567890 Ruler -- Clearly, it takes 6s and 5d states as valence states. Try to generate pp form this file, and test it. Also, read the atom manual. hope it helps. sonu Regards, manjeet
Re: [SIESTA-L] Hubbard Parameter
You have to take different values of U/J and see whic h one of them correctly describes physical properties, says Band gap, JT distortion etc. hope it helps!! On Thu, Jun 19, 2014 at 3:46 PM, Anita Rani ranianit...@gmail.com wrote: Hello to all Siesta Users. . Can anyone tell me please about Hubbard (U) Parameter. How we can calculate it from Siesta output files. In some papers it is mentioned that U = The separation of energy level due to coulomb interaction energy between the Majority 3d and minority 3d. In case of Mn it is 5U. because there are 5 valence electrons at 3d levels. i.e. 5U = The separation of energy level due to coulomb interaction energy between the Majority 3d and minority 3d. How we can calculate The separation of energy level due to coulomb interaction energy between the Majority 3d and minority 3d. Please Help me. Thanks -- // \\ Anita Sharma // \\ Assistant Professor in Physics // ... \\Guru Nanak College for Girls // \\ Sri Muktsar Sahib, (Punjab) (9465305760)
Re: [SIESTA-L] GGA pseudopotential of Cr ,Fe ,Mn
Did you try this ? http://departments.icmab.es/leem/siesta/Databases/Pseudopotentials/periodictable-gga-abinit.html!!! regards, sonu On Wed, May 28, 2014 at 9:12 AM, Swati Khatta swati.kha...@gmail.comwrote: Dear siesta Users, I am working on the magnetic properties with GGA approximation using siesta-3.1. But I am not getting good results of my calculations Please provide me the correct input file of GGA pseudopotential of Cr, Fe ,Mn. I'll be thankful of your positive response . Regards swati
Re: [SIESTA-L] Magnetism from Charge Density
HI, To study magnetism, you have to do spin-polarized calculations, where you will get spin up charge density (rho_up(r)) and spin down charge density (rho_down(r)), and then finally magnetization density ~ (rho_up(r)-rho_down(r)). hope it helps !! sonu On Fri, Mar 28, 2014 at 1:11 AM, I. Camps ica...@gmail.com wrote: Hello, Until my knowledge, the charge density is not directly related to magnetism. Magnetism is related to spin distribution, not to charge distribution. []'s, @mps On Thu, Mar 27, 2014 at 1:15 PM, zehab sohbatzadeh zeh...@yahoo.comwrote: Hi suman First you should define in fdf file as attach file and see it with rho2xsf.there are useful information in attach presentation. best regards Zihab Sohbatzadeh, PhD Student, Dept. of Physics, Faculty of Science, Ferdowsi University of Mashhad , Mashhad , Iran . Mobile: +98 9153490795 Phone: +98 511 8818534 Fax : +98 511 8796416 On Thursday, March 27, 2014 4:37 PM, Suman Chowdhury sumanchowdhur...@gmail.com wrote: Dear all, How to estimate magnetism from charge density in siesta? -- *Junior research fellow Dept. of Physics, University of Calcutta Kolkata- 79, West Bengal, India.* * Ph no-+91-9830512232 %2B91-9830512232*
Re: [SIESTA-L] regarding k point sampling
Dear Amar, You can check by yourself as what should be the k-mesh for sampling the k space in your system. For a nano-ribbon, k point grid could be AxAx1, with nano-ribbon along Z direction. where, A range from 2, 3, 50, 60, and so on depending upon the size of the system and convergence conditions. It would be much better, if your read relevant papers about the nano-ribbons. one could be http://arxiv.org/pdf/1001.4407.pdf hope it helps. regards, sonu IITD * * On Fri, Sep 20, 2013 at 10:07 AM, Dr. Amar Bahadur amar.b@gmail.comwrote: Dear siesta users, Is there any helpful link that could provide the k-point sampling of graphene nanoribbon? -- Kind Regards. == Dr. Amar Bahadur (Department of Physics) Kamla Nehru Institute of Physical and Social Sciences, Sultanpur- 228 118 (U.P.) India Email: amar.b@gmail.com amar.b@gmail.com Mob.-+91-9451431428
Re: [SIESTA-L] Re : Defining lattice constant of CrC6
waring of too close atom ,,here is my fdf file plz help me out clearly you have defined your atoms to be close to each other. Check with the xcrysden and any other visualization software. Further, how many formula units of CrC6 are there in your hexagonal cell ? Also, it's better if you paste your input file rather than attaching it. hope it helps. regards, sonu IITD
Re: [SIESTA-L] what should be meshcut off energy
Hi, I think better you start with 70 ryd mesh cutoff, and go for k point convergence test, and then see the convergence of total energy or the properties you are interested in. regards, SKumar IITD On Fri, Jun 1, 2012 at 5:02 PM, Henrik Löfås henrik.lo...@fysik.uu.sewrote: Dear sir, Have you checked which mesh cutoff is actually used? Somewhere in your output file you will find something like InitMesh: Mesh cutoff (required, used) = Probably for the ranges where the total energy is constant the used mesh cutoff will have the same value? The mesh cutoff is not a continuous variable, so when doing the convergence test you have to check which mesh cutoff is actually used. Best regards Henrik 2012/6/1 mamta chauhan mamta_phys...@yahoo.co.in Dear sir Thanks for your reply. The problem that i found in selecting mesh cut of is that the total energy is constant for cetain ranges of mesh cut energy is constant like in 70 Ryd to 110 Ryd it is -296.671577. Then from 120 Ryd to 140 Ryd it is -296.683935 so on. Tahnks Mamta --- On *Fri, 1/6/12, arun dhiman arun242...@yahoo.com* wrote: From: arun dhiman arun242...@yahoo.com Subject: Re: [SIESTA-L] what should be meshcut off energy To: siesta-l@uam.es siesta-l@uam.es Date: Friday, 1 June, 2012, 4:15 PM You can take value more than 110 Ry for which energy converges Arun Kumar Research Scholar Deptt of Physics Himachal Pradesh University Shimla-5 Himachal Pradesh India -- *From:* mamta chauhan mamta_phys...@yahoo.co.in *To:* siesta-l@uam.es *Sent:* Friday, 1 June 2012, 14:58 *Subject:* [SIESTA-L] what should be meshcut off energy Dear Users I am applying the convergence test for NaCl crystal.For that I took mesh cut off energy from 30 Ryd onwards.I found that after 70 Ryd total energy was constant upto 110 Ryd. on increasing the mesh cut off further the total energy became constant. I would like to know what value of mesh cut off should be selected. Thanks Mamta
Re: [SIESTA-L] lattice constant optimization
Dear Nibras Mossa Umran, i do not know whether your message is in urdu or in any other language? Please convey your message in english so that whole of the SIESTA community can understand it. Thank you very much !!! regards, SK IITD,India 2011/12/28 nibras mossa nibrasmo...@gmail.com: السلام عليكم ممكن تتحدث معي بالعربية انا اعمل على نفس الكود اشرح لي مشكلتك بالتفصيل وانشاء الله نستطيع الايجاد الحل لها On Sat, Dec 17, 2011 at 2:47 PM, majid fathiyan mfathiya...@gmail.com wrote: in the name of God I am sorry for not explaining about my question, it is because of my weakness in english, I am working on cu(111) slab. I have 15 layer, and I want to optimize my lattice constant. but I don`t know how to do it correctly. I tried to change my lattice constant and calculate the total energy and draw the diagram of lattice constant according to total energy but the lattice constant which have the smallest total energy is so biger that my experimental lattice constant. so if any body knows how can I optimize my lattice constant please let me know. thank you. -- Nibras Mossa Umran PhD,Research Scholar Panjab University Chandigarh India.
Re: [SIESTA-L] how the solve such problem?
Hi, I would suggest to first try your own generated pseudo-potentials to have a better control over your calculations. ATOM code in siesta doesn't generate psedopotentials with multiple projectors. To add addition projector corresponding to a specific state, you have to use KB projectors flag (if i remember correctly) in your .fdf input file. Please see the manual. Good Luck. S. Kumar IITD On Thu, Dec 15, 2011 at 7:32 AM, aqingchen artingc...@yahoo.com.cn wrote: Hi, everbody, When I use the pseudoptentials file from the ( http://www.icmab.es/dmmis/leem/siesta/Pseudopotentials/periodictable-intro.html) to calculate some cases. But some errors come up as follows: GHOST: No ghost state for L = 3 KBgen: WARNING: Ghost states have been detected KBgen: WARNING: Some parameter should be changed in the KBgen: WARNING: pseudopotential generation procedure. ERROR STOP from Node:0 how to solve this problem? please give me some suggestions ! Thank you !
Re: [SIESTA-L] Water vibrational frequencies
Dear Prathibha Ramaprasad all siesta users, Your Mesh cutoff is very small. Increase it. Long ago i tried to calculated water molecule frequencies. Here is the calculated vibrational frequencies and eigen vectors : k= 0.000.000.00 Eigenvector = 1 Frequency=-0.186036 Eigenmode (real part) 0.6470E+00 -0.6857E+00 0.1405E-02 0.1618E+00 -0.1714E+00 0.3503E-03 0.1618E+00 -0.1714E+00 0.3519E-03 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 -0.E+00 Eigenvector = 2 Frequency= 0.025870 Eigenmode (real part) 0.2328E-02 0.4128E-02 0.9428E+00 0.5820E-03 0.1032E-02 0.2357E+00 0.5820E-03 0.1032E-02 0.2357E+00 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 -0.E+00 Eigenvector = 3 Frequency= 0.240529 Eigenmode (real part) -0.6857E+00 -0.6470E+00 0.4526E-02 -0.1714E+00 -0.1618E+00 0.1130E-02 -0.1714E+00 -0.1617E+00 0.1133E-02 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 -0.E+00 Eigenvector = 4 Frequency=54.689888 Eigenmode (real part) 0.1887E+00 -0.8071E-03 -0.2385E-03 -0.3752E+00 0.5643E+00 0.1524E+00 -0.3797E+00 -0.5611E+00 -0.1514E+00 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 Eigenvector = 5 Frequency=80.272376 Eigenmode (real part) 0.4023E-01 -0.9692E-04 -0.1125E-02 -0.7505E-01 0.1259E+00 -0.6883E+00 -0.8587E-01 -0.1255E+00 0.6928E+00 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 -0.E+00 Eigenvector = 6 Frequency= 331.224078 Eigenmode (real part) -0.1211E-02 -0.2622E-02 0.E+00 0.2838E-02 0.8284E-02 -0.6688E+00 0.2005E-02 0.2205E-02 -0.6644E+00 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 Eigenvector = 7 Frequency= 1558.552499 Eigenmode (real part) -0.1121E-02 -0.2768E+00 -0.2081E-02 -0.3918E+00 0.5558E+00 0.1377E-02 0.3962E+00 0.5513E+00 0.6946E-02 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 -0.E+00 Eigenvector = 8 Frequency= 3718.259590 Eigenmode (real part) -0.1399E-02 -0.1857E+00 -0.1618E-02 0.5899E+00 0.3690E+00 0.7151E-02 -0.5843E+00 0.3739E+00 -0.6774E-03 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 -0.E+00 0.E+00 Eigenvector = 9 Frequency= 3879.361876 Eigenmode (real part) -0.2718E+00 0.1545E-02 -0.1800E-02 0.5445E+00 0.4062E+00 0.6856E-02 0.5426E+00 -0.4124E+00 0.3437E-03 Eigenmode (imaginary part) 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 0.E+00 -0.E+00 with regards, On Thu, Sep 8, 2011 at 1:17 AM, Prathibha Ramaprasad prama...@asu.eduwrote: Hi Andrei, These are the frequencies I get: eigenvalue # 1 omega= -445.13301743729897 eigenvalue # 2 omega= -110.38569520939947 eigenvalue # 3 omega= -46.712013030918499 eigenvalue # 4 omega= -1.12145510233318604E-002 eigenvalue # 5 omega= 1.10614378824742104E-002 eigenvalue # 6 omega= 1.36483674814901548E-002 eigenvalue # 7 omega= 67.336297669281663 eigenvalue # 8 omega= 115.87202534402807 eigenvalue # 9 omega= 317.70618567755037 Zero point energy = 0.031055 eV Also attached here are the input files. Thank you for your help. Prat On Tue, Sep 6, 2011 at 11:03 PM, apost...@uni-osnabrueck.de wrote: Dear Prat: what are your (nine) frequencies, in fact? How close to zero are six of them? 100 Ry cutoff a priori seems too light ... Best regards Andrei Postnikov Hi Siesta users, When I ran a vibra tool for water, I am getting ridiculously low values. From what I see in the code, it seems to be converting the frequencies to cm^-1 before it outputs to the file, but it looks more like the numbers are in THz. I am using GGA, 100Ry mesh cutoff and 1 molecule of water in a 20X20X20 box. Has anyone here able to obtain anything close to expt values? Any pointers? Thank you, Prat == Sonu Kumar Phd Student,Physics Department Indian Institute of Technology ,Delhi-110016, India https://profiles.google.com/1009ukumarweb:-http://www.iitd.ac.in/ ==
Re: [SIESTA-L] unable to reduce stress tensor components below 1.0 GPa ?
Respected Prof. Emilio Artacho, Thank you very much for helpful suggestions. Also, few questions : is it good idea to apply EQUAL confinement to all atomic orbitals of different atoms in a system ? Because we are adding same soft confinement potential to all different atomic Hamiltonians to generate the basis functions and its like equally exciting all pseudo- states in these pseudo-atoms. What criteria should i use to decide the soft confinement potential to generate numerical atomic orbitals in a multi-atom system? To all siesta users, Solution: increase mesh cutoff. You can also add soft confinement to your orbitals. And/or filter them. is there any option related to filtering of atomic orbitals is siesta. I am using siesta-2.0.2. With regards, -- Sonu Kumar Phd Student Physics Department Indian Institute of Technology Delhi-110016, India web:-http://www.iitd.ac.in/
[SIESTA-L] unable to reduce stress tensor components below 1.0 GPa ?
Dear all siesta users, i am trying to relax cell parameters in rhombohedral unit cell. But stress tensor components are not becoming less than 1.0 GPa. However pressure is ~zero. part of output is:- Stress-tensor-Voigt (kbar): -61.58 29.02 32.56 -23.03 -3.31 -13.80 siesta: Pressure (static): siesta: 0.00120848 -0.00280164 kBar I used these options:- MD.MaxStressTol 1.0 GPa MD.TargetPressure 0.0 GPa %block MD.TargetStress -1.0 -1.0 -1.0 0.0 0.0 0.0 %endblock MD.TargetStress What should i do to reduce it? Also, interesting thing is that off diagonal stress components are non-zero, but should be zero. Is this explainable? Thank you. regards, Sonu IITD
[SIESTA-L] Very slow or no convergence of density matrix ?
Dear all siesta users, after varying DM.MixingWeight =0.1, 0.01 ,0.001, DM.NumberPulay 4, 6, 8 DM.NumberKick 0,10, 20,40 DM.KickMixingWeight 0, 0.10, 0.01 scf iterations=400 Meshcutoff=500 Ry and MP grid =6x6x6 is used. i am still not able to get the convergence. Part of output file with very slow convergence : siesta: 284 -31598.9061 -31598.9016 -31598.9016 0.0011 -1.9863 siesta: 285 -31598.9061 -31598.9025 -31598.9025 0.0011 -1.9862 siesta: 286 -31598.9061 -31598.9027 -31598.9027 0.0011 -1.9862 siesta: 287 -31598.9061 -31598.9024 -31598.9024 0.0011 -1.9863 siesta: 288 -31598.9061 -31598.9049 -31598.9049 0.0011 -1.9870 siesta: 289 -31598.9061 -31598.9055 -31598.9055 0.0011 -1.9872 siesta: 290 -31598.9061 -31598.9079 -31598.9079 0.0011 -1.9875 siesta: 291 -31598.9061 -31598.9079 -31598.9079 0.0011 -1.9874 siesta: 292 -31598.9061 -31598.9085 -31598.9085 0.0011 -1.9871 siesta: 293 -31598.9061 -31598.9076 -31598.9076 0.0011 -1.9871 siesta: 294 -31598.9061 -31598.9078 -31598.9078 0.0011 -1.9871 siesta: 295 -31598.9061 -31598.9077 -31598.9077 0.0011 -1.9871 siesta: 296 -31598.9061 -31598.9066 -31598.9066 0.0011 -1.9871 siesta: 297 -31598.9061 -31598.9059 -31598.9059 0.0011 -1.9870 siesta: 298 -31598.9061 -31598.9075 -31598.9075 0.0011 -1.9865 siesta: 299 -31598.9061 -31598.9073 -31598.9073 0.0011 -1.9865 siesta: 300 -31598.9061 -31598.9074 -31598.9074 0.0011 -1.9865 siesta: 301 -31598.9061 -31598.9061 -31598.9061 0.0012 -1.9897 siesta: 302 -31598.9061 -31598.9073 -31598.9073 0.0011 -1.9873 siesta: 303 -31598.9061 -31598.9072 -31598.9072 0.0011 -1.9873 siesta: 304 -31598.9061 -31598.9071 -31598.9071 0.0011 -1.9871 siesta: 305 -31598.9061 -31598.9079 -31598.9079 0.0011 -1.9870 siesta: 306 -31598.9061 -31598.9072 -31598.9072 0.0011 -1.9871 siesta: 307 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9870 siesta: 308 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9872 siesta: 309 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9871 siesta: 310 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9871 siesta: 311 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9871 siesta: 312 -31598.9061 -31598.9071 -31598.9071 0.0011 -1.9870 siesta: 313 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9871 siesta: 314 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 315 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9871 siesta: 316 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9871 siesta: 317 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9871 siesta: 318 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 319 -31598.9061 -31598.9065 -31598.9065 0.0011 -1.9870 siesta: 320 -31598.9061 -31598.9067 -31598.9067 0.0011 -1.9871 siesta: 321 -31598.9061 -31598.9061 -31598.9061 0.0012 -1.9873 siesta: 322 -31598.9061 -31598.9068 -31598.9068 0.0011 -1.9870 siesta: 323 -31598.9061 -31598.9068 -31598.9068 0.0011 -1.9870 siesta: 324 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9871 siesta: 325 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 326 -31598.9061 -31598.9067 -31598.9067 0.0011 -1.9870 siesta: 327 -31598.9061 -31598.9068 -31598.9068 0.0011 -1.9870 siesta: 328 -31598.9061 -31598.9068 -31598.9068 0.0011 -1.9871 siesta: 329 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 330 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 331 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9870 siesta: 332 -31598.9061 -31598.9076 -31598.9076 0.0011 -1.9870 siesta: 333 -31598.9061 -31598.9064 -31598.9064 0.0011 -1.9870 siesta: 334 -31598.9061 -31598.9067 -31598.9067 0.0011 -1.9871 siesta: 335 -31598.9061 -31598.9068 -31598.9068 0.0011 -1.9871 siesta: 336 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 337 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 338 -31598.9061 -31598.9068 -31598.9068 0.0011 -1.9871 siesta: 339 -31598.9061 -31598.9074 -31598.9074 0.0011 -1.9870 siesta: 340 -31598.9061 -31598.9067 -31598.9067 0.0011 -1.9870 siesta: 341 -31598.9061 -31598.9061 -31598.9061 0.0012 -1.9874 siesta: 342 -31598.9061 -31598.9068 -31598.9068 0.0011 -1.9871 siesta: 343 -31598.9061 -31598.9071 -31598.9071 0.0011 -1.9870 siesta: 344 -31598.9061 -31598.9072
Re: [SIESTA-L] Very slow or no convergence of density matrix ?
Dear Marcos, Pablo and Jw , i had used the DM obtained from 1000K and used that with 0K, but i got the error in dimension of maxnd as: iodm: Reading Density Matrix from files chkdim: ERROR: In iodm, dimension maxnd = 94363. It must be at least 109536 Stopping Program from Node:0 chkdim: ERROR: In iodm, dimension maxnd = 82707. It must be at least 95742 chkdim: ERROR: In iodm, dimension maxnd = 78200. It must be at least 90692 chkdim: ERROR: In iodm, dimension maxnd = 55290. It must be at least 66436 chkdim: ERROR: In iodm, dimension maxnd = 58695. It must be at least 64950 Stopping Program from Node:4 chkdim: ERROR: In iodm, dimension maxnd = 62895. It must be at least 71914 Stopping Program from Node:5 Stopping Program from Node:3 Stopping Program from Node:1 Stopping Program from Node:2 with regards, Sonu 2010/6/9 Marcos Veríssimo Alves marcos.verissimo.al...@gmail.com This could be due to degeneracies in your system. The system could be jumping from two different electronic configurations with the same energy and it cannot decide in which one to stay. Follow Pablo's suggestion, raise the electronic temperature - not excessively, especially if you are dealing with spin polarization. Once converged, slowly lower the electronic temperature until you get to the low value you aim for. Marcos On Wed, Jun 9, 2010 at 4:47 PM, jw wei redsky...@gmail.com wrote: The problem have puzzled me for a long times. 2010/6/9, Pablo A. Denis pab...@fq.edu.uy: perhaps increasing the electronic temperature can help. best regards, pablo - Original Message - From: sonu kumar To: siesta-l@uam.es Sent: Wednesday, June 09, 2010 10:37 AM Subject: [SIESTA-L] Very slow or no convergence of density matrix ? Dear all siesta users, after varying DM.MixingWeight =0.1, 0.01,0.001, DM.NumberPulay 4, 6, 8 DM.NumberKick 0,10, 20,40 DM.KickMixingWeight 0, 0.10, 0.01 scf iterations=400 Meshcutoff=500 Ry and MP grid =6x6x6 is used. i am still not able to get the convergence. Part of output file with very slow convergence : siesta: 284 -31598.9061 -31598.9016 -31598.9016 0.0011 -1.9863 siesta: 285 -31598.9061 -31598.9025 -31598.9025 0.0011 -1.9862 siesta: 286 -31598.9061 -31598.9027 -31598.9027 0.0011 -1.9862 siesta: 287 -31598.9061 -31598.9024 -31598.9024 0.0011 -1.9863 siesta: 288 -31598.9061 -31598.9049 -31598.9049 0.0011 -1.9870 siesta: 289 -31598.9061 -31598.9055 -31598.9055 0.0011 -1.9872 siesta: 290 -31598.9061 -31598.9079 -31598.9079 0.0011 -1.9875 siesta: 291 -31598.9061 -31598.9079 -31598.9079 0.0011 -1.9874 siesta: 292 -31598.9061 -31598.9085 -31598.9085 0.0011 -1.9871 siesta: 293 -31598.9061 -31598.9076 -31598.9076 0.0011 -1.9871 siesta: 294 -31598.9061 -31598.9078 -31598.9078 0.0011 -1.9871 siesta: 295 -31598.9061 -31598.9077 -31598.9077 0.0011 -1.9871 siesta: 296 -31598.9061 -31598.9066 -31598.9066 0.0011 -1.9871 siesta: 297 -31598.9061 -31598.9059 -31598.9059 0.0011 -1.9870 siesta: 298 -31598.9061 -31598.9075 -31598.9075 0.0011 -1.9865 siesta: 299 -31598.9061 -31598.9073 -31598.9073 0.0011 -1.9865 siesta: 300 -31598.9061 -31598.9074 -31598.9074 0.0011 -1.9865 siesta: 301 -31598.9061 -31598.9061 -31598.9061 0.0012 -1.9897 siesta: 302 -31598.9061 -31598.9073 -31598.9073 0.0011 -1.9873 siesta: 303 -31598.9061 -31598.9072 -31598.9072 0.0011 -1.9873 siesta: 304 -31598.9061 -31598.9071 -31598.9071 0.0011 -1.9871 siesta: 305 -31598.9061 -31598.9079 -31598.9079 0.0011 -1.9870 siesta: 306 -31598.9061 -31598.9072 -31598.9072 0.0011 -1.9871 siesta: 307 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9870 siesta: 308 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9872 siesta: 309 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9871 siesta: 310 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9871 siesta: 311 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9871 siesta: 312 -31598.9061 -31598.9071 -31598.9071 0.0011 -1.9870 siesta: 313 -31598.9061 -31598.9070 -31598.9070 0.0011 -1.9871 siesta: 314 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9870 siesta: 315 -31598.9061 -31598.9069 -31598.9069 0.0011 -1.9871 siesta
[SIESTA-L] Trivial problem with conversion from fractional to Bohr coordinates?
Dear all siesta Users, sorry fof trivial question... i want to convert fractional coordinates to Bohr coordinates in fcc primitive unit cell. Lattice constant (conventional cell) =10.104 ang. Siesta does following conversion ... siesta: Atomic coordinates (Bohr) and species siesta: 0.0 0.0 0.0 siesta: 7.16018 11.93363 9.54690 siesta: 11.93363 9.54690 7.16018 siesta: 9.54690 7.16018 11.93363 outcoor: Atomic coordinates (fractional): 0.0.0. 0.50000.75000.2500 0.75000.25000.5000 0.25000.50000.7500 But i got .. 0.0 0.0 0.0 6.752 10.1285 3.3762 so on... why this differencecan anyone assist me? with regards, Sonu
[SIESTA-L] not able to download pseudo-potentials from user contributed data base?
hi dear all siesta users, I am not able to download the Psedo-potentials(PPs) from the user contributed database. how can i download them ? With Regards, Sonu Kumar
Re: [SIESTA-L] underestimated zone center frequencies in MgO ?
Dear Sir, *your structure is not exactly cubic* (look at your atoms position). I wonder why you use atomic coordinate which looks like the result of relaxation along with lattice parameters which look like given by hand. Relax either both, or none. 1) i relaxed both atomic coordinates and lattice parameters using variable cell option and got outcoor: Relaxed atomic coordinates (scaled): 0.59930.61100.5744 1 Mg 1 0.485531110.485535230.48553182 2 O 2 outcell: Unit cell vectors (Ang): -0.222.0448032.044814 2.044808 -0.262.044818 2.0448032.044802 -0.21 so i used lattice constant=4.089606~4.09 Ang. 2) when i did study of energy v/s volume, i got minima at 4.10 Ang, with out above relaxation. should i proceed this way, keeping care of symmetry or should i see the final results(freqs) to decide, which one to use (relaxation or no relaxation)? 3) can we use macroscopic polarisation analysis for small band gap materials? sorry, if my question is stupid. With Due Regards, Sonu Kumar Phd Student Indian Institute of Technology Delhi Delhi-110016 web:-http://www.iitd.ac.in/
[SIESTA-L] underestimated zone center frequencies in MgO ?
Hi dear all Siesta Users, i tried to reproduce the zone center frequencies in MgO. But they are not same as shown in JOURNAL OF APPLIED PHYSICS 100, 023533,2006. In this paper, doubly degenerate freq is ~400 cm-1 and other is ~700cm-1 apart from acoustical freqs. But Siesta calculates following freqs : eigenvalue # 1 omega= -5.342383622781044E-002 eigenvalue # 2 omega= 9.129011837545617E-003 eigenvalue # 3 omega= 4.213637115974628E-002 eigenvalue # 4 omega= 397.442968241599 eigenvalue # 5 omega= 413.630587428353 eigenvalue # 6 omega= 413.916231936010 I used the basis and pp for MgO as used by J. Junquera et al., Phys. Rev. B, 64, 235111 (2001), available on siesta site. I am wondering, How can i reproduce them? i am attaching the input file. I need your help to reproduce the correct frequencies. With due Regards, Sonu Kumar Phd Student Indian Institute of Technology Delhi Delhi-110016 web:-http://www.iitd.ac.in/ mgo.fdf Description: application/vnd.fdf
[SIESTA-L] simplex method
hi dear all, Can anybody provide me some study material or any kind of help related to basis optimisation by simplex method? I have problem in understanding the variational parameters ? With Regards, 1009u
Re: [SIESTA-L] how do you change the atomiccoordinatesformat from ang to scaledcartesian? by hand?
Hi Fen Hong, use-- AtomCoorFormatOut ScaledCartesian with type of run=cg and cg steps=0 regards, 1009u On Thu, Jan 28, 2010 at 12:08 PM, Fen Hong gm030...@gmail.com wrote: Hi, everyone I am trying to change the atomiccoordinateformat from ang to scalecartesian. I calculated it by hand. But it seems impossible if the system is too large. How do you change it.Is there some simple way to do it? Example: LatticeConstant8.6514 Ang %block LatticeVectors 1. 0. 0. -0.5 0.8660254 0. 0. 0. 2.00 %endblock LatticeVectors AtomicCoordinatesFormat Ang %block AtomicCoordinatesAndAtomicSpecies 0.0.2.35460760 1 1 Au 1.467001120.84919753 -0.23066334 1 2 Au 2.89953753 -0.029254282.65757611 1 3 Au 4.325690380.832479500. 1 4 Au 5.76513068 -0.002950982.68342880 1 5 Au 7.209483960.832479500. 1 6 Au -1.488233092.498424832.66695348 1 7 Au 0.3.329918010. 1 8 Au 1.346816232.527931722.29986223 1 9 Au 2.883793593.329918010. 1 10 Au 4.371842462.493503082.66713826 1 11 Au 5.767587173.329918010. 1 12 Au -2.884964964.996297582.68129387 1 13 Au -1.441896795.827356510. 1 14 Au -0.016174385.035688592.66152987 1 15 Au 1.441896795.827356510. 1 16 Au 2.899764735.038174712.66126078 1 17 Au 4.325690385.827356510. 1 18 Au
Re: [SIESTA-L] Re:why the forces, energy different in siesta-2.0.2 and beta version?
hi 张广平, I have little knowelge of mpi libraries. May be other experienced SIESTA users help you sort out the problem. Are you sure that PGI works fine? Perhaps code may be changed a little bit like you said, as i have compiled both versions on same computer under same OS. Hopefully some one on the list may help. With Regards, 1009u 2010/1/25 张广平 zgp...@126.com Hi,sonu kumar I compiled the siesta with mpich-1.2.7 copmiled using PGI. But for math LIB,I use mkl,I put the arch.make in the attachment. I guess the difference for mine is caused by the mpich when it communicate data.I think it can be fix by some settings for mpich,but i dont know how to fix it.You use two versions ,I think it maybe the parameters in the code is different type(float or double precision) or they were installed on two different machine or under two different OS. Guangping Zhang -- Original -- *From: * sonu kumar1009uku...@gmail.com; *Date: * Mon, Jan 25, 2010 02:42 AM *To: * siesta-lsiesta-l@uam.es; *Subject: * Re: [SIESTA-L] Re:why the forces, energy different in siesta-2.0.2 and beta version? hi 张广平, I have compiled both the versions using gnu-fortran compiler (gfortran). You can have a look at arch.make files of these versions for serial run . I could have checked these differences for parallel versions, also. but, i don't have intel fortran compiler 10.0 and mkl10.1 to compile beta version. 1009u 2010/1/24 张广平 zgp...@126.com Hi,sonu kumar I have encountered the same problem,but mine was because of serial or parallel mode.I compiled me siesta with mpich on the REHEL-5.4.when I run a task using 1 or 8 or other,the results differed from each other after 4-6 decimal places. Are you compiled the two version with the same parameters?
[SIESTA-L] why the forces, energy different in siesta-2.0.2 and beta version?
hi SIESTA users, I am getting different forces,energy ( after 4-6 decimal places) in stable and beta version of siesta. Both the packages are compiled with gfortran compiler in serial mode and, then, tested for fe.fdf file in tests/fe. Parts of both outputs are as follows: for stable version: siesta: E_KS(eV) = -782.2432 siesta: Atomic forces (eV/Ang): Tot -0.21 -0.01 -0.00 Max0.21 Res0.12sqrt( Sum f_i^2 / 3N ) Max0.21constrained Target enthalpy (eV/cell) -782.2458 siesta: Eharris = -782.242590 siesta: Etot= -782.243177 siesta: FreeEng = -782.245753 xxx-- beta version siesta: E_KS(eV) = -782.2434 siesta: Atomic forces (eV/Ang): Tot -0.260.170.12 Max0.26 Res0.19sqrt( Sum f_i^2 / 3N ) Max0.26constrained Target enthalpy (eV/cell) -782.2460 siesta: Eharris = -782.242770 siesta: Etot= -782.243427 siesta: FreeEng = -782.246003 - Are these differences reasonable enough to affect the calculations ? Can anybody tell me ? With regards, 1009u
Re: [SIESTA-L] Re:why the forces, energy different in siesta-2.0.2 and beta version?
hi 张广平, I have compiled both the versions using gnu-fortran compiler (gfortran). You can have a look at arch.make files of these versions for serial run . I could have checked these differences for parallel versions, also. but, i don't have intel fortran compiler 10.0 and mkl10.1 to compile beta version. 1009u 2010/1/24 张广平 zgp...@126.com Hi,sonu kumar I have encountered the same problem,but mine was because of serial or parallel mode.I compiled me siesta with mpich on the REHEL-5.4.when I run a task using 1 or 8 or other,the results differed from each other after 4-6 decimal places. Are you compiled the two version with the same parameters? arch.make Description: Binary data arch.make Description: Binary data
[SIESTA-L] Zone center phonons with unit cell or Supercell ?
hi dear all I want to calculate the phonons at gamma point of the BZ. 1) Do i need to make the supercell to find the phonons ? is a unit cell is sufficient for it? 2) which unit cell i mean whether primitive or conventional unit should i use? with regards, 1009U
[SIESTA-L] Stress components during atomic relaxation and Auxiliary supercell ?
Hi dear all I am doing *atomic relaxation* of a system containing 7 atoms in the primitive unit cell (conventional unit cell contains 21 atoms) 1) i got the max. force tolerance 0.0002 eV/Ang, but stress components seems to be large as follows: Stress-tensor-Voigt (kbar): -5.09 16.77 19.82 -12.79 -3.98 -8.53 Here i set variable cell option false . What should be the max tolerance of the stress components? 2) if i take supecell =unit cell, even then SIESTA takes an internal auxiliary supercell, here 6x6x5=180 atoms with non zero kgrid cutoff. Although with zero value of kgrid cutoff, it doesn't take internal auxiliary supercell. how does it happen? Is it because of periodic boundary condition? but boundary condtion in SIESTA is not mentioned in the manual. can anybody help me? With Kind Regards, 1009U
[SIESTA-L] can not do OrderN with K-points
hi dear all, i am doing a FC run over a system with 189 atoms in the unit cell (formed by making use of Supercell). but i got the error.probably bcoz of memory? can anybody help me.? last part of my output file is: siesta: == Begin FC step = 0 Undisplaced coordinates == superc: Internal auxiliary supercell: 2 x 2 x 2 = 8 superc: Number of atoms, orbitals, and projectors: 1512 17928 22680 outcell: Unit cell vectors (Ang): 15.510.000.00 10.062640 11.8026450.00 10.0626404.643694 10.850486 outcell: Cell vector modules (Ang) : 15.51 15.509969 15.509792 outcell: Cell angles (23,13,12) (deg): 49.5514 49.5494 49.5499 outcell: Cell volume (Ang**3): 1986.2793 InitMesh: MESH = 192 x 192 x 192 = 7077888 InitMesh: Mesh cutoff (required, used) = 500.000 553.018 Ry * Maximum dynamic memory allocated = 880 MB *Cannot do O(N) with k-points.* Stopping Program from Node:0 forrtl: severe (174): SIGSEGV,* segmentation fault occurred* Image PCRoutineLineSource *libc.so.6* 7FDBED094A04 Unknown Unknown Unknown siesta 006E37B3 UnknownUnknown Unknown siesta 00629ACF Unknown Unknown Unknown siesta 0056DC54 Unknown Unknown Unknown siesta 0052930E UnknownUnknown Unknown siesta 00403B7C Unknown Unknown Unknown libc.so.6 7FDBED036586 UnknownUnknown Unknown * *siesta 00403A79 Unknown Unknown Unknown 1009u