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Xi’an-CI Program review Xi’an-CI Program Package Review

Xi'an-CI

   Xi’an-CI program generates Multi Reference SDCI (MRCISD) wavefunctions (including internal contracted MRCISD on several different level accuracy), N-electron Valence states Second Order Perturbation Theory (including multi-state NEVPT2 (MS-NEVPT2), N-electron Valence states Third Order Perturbation Theory (NEVPT3), Static-Dynamic-Static Second Order Perturbation Theory (SDSPT2), Static-Dynamic-Static Configuration Interaction (SDSCI), Configuration Based Multi Reference Second Order Perturbation Theory (CB-MRPT2) and Configuration Based Multi Reference Third Order Perturbation Theory (CB-MRPT3). This program is based on hole-particle symmetry based and GUGA for the computation of CI matrix elements. The program can calculate several eigenvectors simultaneously.
   Xi’an-CI program is written by Zhenyi Wen, Yubin Wang, Zhengting Gan, Bingbing Suo and Yibo Lei (Institute of Modern Physics, Northwest University, China). 

Corresponding email

bsuo@nwu.edu.cn (Prof. Bingbing Suo) 
leiyb@nwu.edu.cn (Associate Prof. Yibo Lei) 
wzy@nwu.edu.cn (Prof. Zhenyi Wen)
yubin_wang@hotmail.com (Prof. Yubin Wang)

References

Xi’an-CI Program Package Review 
1.      B. Suo, Y. Lei, H. Han, Y. Wang, Mol. Phys., 116, 1051 (2018).

ucMRCISD program
1.      Y. Wang, G. Zhai, B. Suo, Z. Gan, Z. Wen, Chem. Phys. Lett., 375, 134 (2003).
2.      Y. Wang, Z. Wen, Z. Zhang, Q. Du, J. Comput. Chem, 13, 187 (1992).
3.      Y. Lei, B. Suo, Y. Dou, Y. Wang, Z. Wen,  J. Comput. Chem, 31, 1752 (2010).
4.      B. Suo, G. Zhai, Y. Wang, Z. Wen, X. Hu, L. Li, J. Comput. Chem, 26, 88 (2005).  
5.      Z. Gan, K. Su, Y. Wang, Z. Wen, Sci. China Ser. B-Chem, 42, 43 (1999).

icMRCISD program
1.      Y. Wang, H. Han, Y. Lei, B. Suo, H. Zhu, Q. Song, Z. Wen, J. Chem. Phys., 141, 164114 (2014).
2.      B. Suo, Y. Lei, H. Han, Y. Wang, Mol. Phys., 116, 1051 (2018).

MS-NEVPT2 program
1.      C. Angeli, R. Cimiraglia, S. Evangelisti, T. Leininger, J.P.Malrieu, J. Chem. Phys., 114, 10252 (2001).
2.      Y. Lei, W. Liu, M. R. Hoffmann, Mol. Phys., 115, 2696 (2017).
3.      B. Suo, Y. Lei, H. Han, Y. Wang, Mol. Phys., 116, 1051 (2018).

SDSPT2 program
1.      Y. Lei, W. Liu, M. R. Hoffmann, Mol. Phys., 115, 2696 (2017).
2.      W. Liu, M.R. Hoffmann, Theor. Chem. Acc., 133, 1481 (2014).
3.      W. Liu, M.R. Hoffmann, J. Chem. Theory Comput., 12, 1169 (2016); 12, 3000(E) (2016).

CB-MRPT2 program
1.      Y. Lei, Y. Wang, H. Han, Q. Song, B. Suo, Z. Wen, J. Chem. Phys., 137, 144102 (2012).
2.      A. Li, H. Han, B. Suo, Y. Wang, Z. Wen, Sci. China CHEMISTRY, 53. 933 (2010).
3.      Y. Wang, Z. Gan, K. Suo, Z, Wen, Sci. China Ser. B-Chem, 43, 567 (2000).

General keywords

Comment:

   If no keyword is used, xianci module will read information from mcscf and traint modules and then calculate Fully internal contracted MRCISD. 

Electron

  • CI effective electron Number without electrons of frozen MOs in traint module for MO integral transformation

Example:

Electron
 30

nroot

  • State Number, CASSCF with MixCI method needs to input state number of target CI type.

Example:

Symmetry

  • Symmetry of the target state, CASSCF with MixCI method needs to input irrep of target CI type.

Example:

Spin

  • Spin multiplicity (2S+1), CASSCF with MixCI method needs to input Spin multiplicity of target CI type.

core

  • Number of frozen orbitals in each irreps, which must be missing or set to zero in each irreps if it has frozen MOs in traint module.

Example:

Inactive

  • Number of inactive orbitals in each irreps.

Example:

Active

  • Number of active orbitals in each irreps.

Example:

Comment:

  If the above keywords are not set. the mcscf and traint modules information will be used. 

Maxiter

  • Maximum iteration Number of MRCISD. The default value is 500.

Example:

Maxiter
 50

NODE

  • Maximum DRT node number. The default value is 100000.

Example:

NODE 
 100000

WEI

  • Maximum DRT WEI number. The default value is 500000.

Example:

WEI
 500000

PLOOP

  • Maximum partial LOOP number. The default value is 500000.

Example:

PLOOP 
 500000

SETICF

  • Maximum partial internal CSFs number in active space. The default value is 500.

Example:

SETICF
 500

SETDXY

  • Maximum CI subspace in active space (DXY). The default value is 50000.

Example:

SETDXY
 50000

SETH0

  • Maximum reference CSF number. The default value is 500000.

Example:

SETH0
 500000

MAXLOOP

  • Maximum partial LOOP number for CI acceleration which is larger than or equal to keyword 'PLOOP' set value. The default value is 500000.

Example:

MAXLOOP
 500000

PLBLK

  • Maximum partial LOOP block number. The default value is 500000.

Example:

PLBLK
 500000

CITHR

  • set threshold for CI vector print. The default value is 0.05.

Example:

CITHR 
 0.1

Conv

  • set threshold for CI energy, CI vector and Residual vector of MRCISD, respectively. The default value is set as the following example.

Example:

Conv
1.d-8 1.d-6 1.d-8

UCCI

  • This keyword is set for un-contracted MRCISD.

Example:

 UCCI

FCCI

  • Default for internal contraction module. This keyword is set for Fully internal Contraction module of CSFs, reference CSFs are not contracted for MRCISD calculation, while perturbation theory calculation all CI subspaces are internally contracted.

Example:

 FCCI

NICI

  • This keyword is set for one internal Contraction module of CSFs, only internal CI subspaces are not contracted.

Example:

 NICI

CWCI

  • This keyword is set for one internal Contraction module of CSFs, corresponding to keyword 'mrcic' in Molpro program for Celani-Werner (CW) contraction, where only CI subspaces VV, DV, DDV and VD in hole-particle symmetry are not contracted.

Example:

 CWCI

WKCI

  • This keyword is set for one internal Contraction module of CSFs, corresponding to keyword 'mrci' in Molpro program for Werner-Knowles (WK) contraction, where only CI subspaces with two electron excitation to external spaces are contracted.

Example:

 WKCI

SDCI

  • This keyword is set for one internal Contraction module of CSFs, the accuracy of which is more accurate than CWCI but less than WKCI. In contrast with WKCI module, CI subspaces with two electron excitation from hole space and meanwhile one electron excitation to external space are also contracted.

Example:

 SDCI

Comment:

  If no keyword is set for perturbation theory calculation in the following, xianci module will calculate MRCISD in default. 

NEVPT2

  • set for SS-NEVPT2 and MS-NEVPT2 calculations, where each reference state expands a specific CI space.

Example:

 NEVPT2

MR-NEVPT2

  • set for SS-NEVPT2 and MS-NEVPT2 calculations, where all reference states expand only one multi-states CI space.

Example:

 MR-NEVPT2

NEVPT3

  • set for SS-NEVPT3 calculation, where each reference state expands a specific CI space.

Example:

 NEVPT3

SDSPT2

  • set for SDSPT2 calculation, where all reference states expand only one multi-states CI space.

Example:

 SDSPT2

SDSCI

  • set for SDSCI calculation, where all reference states expand only one multi-states CI space.

Example:

 SDSCI

NOLAN

  • set for SDSPT2 and SDSCI calculations, where no Lanczos wavefunction is used to produce Ps wavefunction in SDSPT2 and SDSCI.

Example:

 NOLAN

NDIMPS

  • set for SDSPT2 and SDSCI calculations, where CASSCF wavefunctions are used to produce Ps wavefunction in SDSPT2 and SDSCI.

Example:

 NDIMPS
  2   # two high-lying CASSCF wavefunctions are used to produce Ps wavefunction in SDSPT2 and SDSCI relative to reference wavefunctions.

Comment:

 If Keyword 'NDIMPS' are not set or set to zero and keyword 'NOLAN' are set, SDSPT2 or SDSCI has no Ps wavefunction. 

CBMRPT2

  • set for CB-MRPT2 calculation, where each reference state expands a specific CI space.

Example:

 CBMRPT2

MR-CBMRPT2

  • set for CB-MRPT2 calculations, where all reference states expand only one multi-states CI space.

Example:

 MR-CBMRPT2 

MR-CBMRPT3

  • set for CB-MRPT3 calculations, where all reference states expand only one multi-states CI space.

Example:

 MR-CBMRPT3 

Examples

Test Example 1

input:

$COMPASS 
Title
 C2H4 Molecule test run
Basis
 cc-pvdz
Geometry
 C             0.000000       1.386400       0.000000    
 C             0.000000      -1.386400       0.000000    
 C             2.099700       2.794200       0.000000    
 C            -2.099700      -2.794200       0.000000    
 H            -1.845200       2.307000       0.000000    
 H             1.845200      -2.307000       0.000000    
 H             3.968500       1.930200       0.000000    
 H            -3.968500      -1.930200       0.000000    
 H             2.015100       4.847500       0.000000    
 H            -2.015100      -4.847500       0.000000    
END geometry
Check
unit
bohr
$END

$xuanyuan
$end

$SCF
RHF
charge
 0
spin
 1
$END

$MCSCF
close
 7   0   0   5
active
 0   2   3   1
actele
 6
spin
 1
symmetry
 1
roots
 3 3 
 1 2 3 
 1 1 1 
mixci
 2  
 1 3
 2 1
 1 4 
ROOTPRT
 1
prtcri
0.1
guess
hforb
$END

$TRAINT
Frozen
 2 0 0 2 0 0 0 0 
Orbital
 mcorb
$END

$XIANCI
nroot
2
spin
1
symmetry
1
$END

$XIANCI
nroot
1
spin
3
symmetry
4
$END

Results:

========================= mcscf results ==============================
    State Averaged ci energy      -154.86258790

    root   1
    energy=     -154.98691206     exe(eV)=    0.0000


    root   2
    energy=     -154.73707954     exe(eV)=    6.7983


    root   3
    energy=     -154.86377210     exe(eV)=    3.3508

 
 ++++++++  DATA CHECK +++++++++++++++++++++++++++++++++
  CHECKDATA:MCSCF:MCENERGY:     -154.9869121     -154.7370795     -154.8637721
 ++++++++++ END DATA CHECK ++++++++++++++++++++++++++++
 
  End   MCSCF Calculation

========================= xianci results ==============================

=============================== For first type of CI with two singlet states ====================================

 Roots of Heff are calculated are listed below: 
 
                        ENE           ENE + Pople       ENE + App Pople       ENE + DAV           ENE + MEISS
  root   1       -155.45209027       -155.52854668       -155.52960628       -155.51383149       -155.51395190
  root   2       -155.19957647       -155.27731997       -155.27842584       -155.26200965       -155.26229526
               MRCISD energyies     Pople Correction  App Pople Correction  Davidson Correction  Meissner correction    

 =====================================================

 MRSDCI CALCULATION CONVERGED

 NROOT      MC ENERGY        CI ENERGY          CI DAV             DAVCOEF
   1     -154.98691206    -155.45209027      -155.51383149         0.867274
   2     -154.73707954    -155.19957647      -155.26200965         0.865008
         MCSCF energyies  MRCISD energyies Davidson Correction  Reference weight   
    
    root   1
    energy=     -155.45209027     exe(eV)=    0.0000


    root   2
    energy=     -155.19957647     exe(eV)=    6.8713

 
 ++++++++  DATA CHECK +++++++++++++++++++++++++++++++++
  CHECKDATA:MRCI:CIENERGY:     -155.4520903     -155.1995765
 ++++++++++ END DATA CHECK ++++++++++++++++++++++++++++

=============================== For second type of CI with one triplet state ====================================
 

 Roots of Heff are calculated are listed below: 
 
                        ENE           ENE + Pople       ENE + App Pople       ENE + DAV           ENE + MEISS
  root   1       -155.32503309       -155.40089070       -155.40194273       -155.38628185       -155.38640551
 
 =====================================================

 MRSDCI CALCULATION CONVERGED

 NROOT      MC ENERGY        CI ENERGY        CI DAV         DAVCOEF
   1     -154.86377210    -155.32503309    -155.38628185    0.867215

    root   1
    energy=     -155.32503309     exe(eV)=    0.0000

 
 ++++++++  DATA CHECK +++++++++++++++++++++++++++++++++
  CHECKDATA:MRCI:CIENERGY:     -155.3250331
 ++++++++++ END DATA CHECK ++++++++++++++++++++++++++++

Test Example 2

input:

$XIANCI
nroot
2
spin
1
symmetry
1
SDSPT2
$END

Results:

=============================== For first type of CI with two singlet states ====================================

 NROOT   MC ENE        SS-NEVPT2 ENE   MS-NEVPT2 ENE     SDSPT2 ENE    SDSPT2+Q1 ENE   SDSPT2+Q2 ENE        SDSPT2+Q3 ENE       DAVCOEF
   1   -154.98691206   -155.47745410   -155.47745446   -155.41455599   -155.47503759   -155.47574313       -155.46512580        0.881748
   2   -154.73707954   -155.21961390   -155.21961354   -155.15793413   -155.21775988   -155.21846183       -155.20789974        0.881276
Energies:   MCSCF       SS-NEVPT2       MS-NEVPT2         SDSPT2    Pople Correction App Pople Correction Davidson Correction Ref. Weight 

Test Example 3

input:

$XIANCI
nroot
2
spin
1
symmetry
1
SDSCI
$END

Results:

=============================== For first type of CI with two singlet states ====================================

 NROOT   MC ENE        SS-NEVPT2 ENE   MS-NEVPT2 ENE     SDSPT2 ENE    SDSPT2+Q1 ENE   SDSPT2+Q2 ENE   SDSPT2+Q3 ENE   DAVCOEF
   1   -154.98691206   -155.47745410   -155.47745446   -155.44006672   -155.51313986   -155.51413050   -155.49935009   0.869176
   2   -154.73707954   -155.21961390   -155.21961354   -155.18843582   -155.26361048   -155.26466844   -155.24894428   0.865941
Energies:   MCSCF       SS-NEVPT2       MS-NEVPT2         SDSCI  Pople Correction App Pople Correction Davidson Correction Ref. Weight 

Test Example 4

input:

$XIANCI
nroot
2
spin
1
symmetry
1
NEVPT3
$END

Results:

=============================== For first type of CI with two singlet states ====================================

 NROOT        MC ENERGY       SS-NEVPT2 ENERGY    MS-NEVPT2 ENERGY    SS-NEVPT3 ENERGY    MS-NEVPT3 ENERGY
   1       -154.98691206       -155.47742562       -155.47742574       -155.51364676       -155.51364676
   2       -154.73707954       -155.21952164       -155.21952152       -155.26247430       -155.26247430
Energies:     MCSCF             SS-NEVPT2            MS-NEVPT2          SS-NEVPT3            Useless

Test Example 5

input:

$XIANCI
nroot
2
spin
1
symmetry
1
CBMRPT2
$END

Results:

=============================== For first type of CI with two singlet states ====================================

 ++++++++  DATA CHECK +++++++++++++++++++++++++++++++++
  CHECKDATA:MRPT2:PT2ENERGY:     -155.5496768     -155.2931467
 ++++++++++ END DATA CHECK ++++++++++++++++++++++++++++

Test Example 6

input:

$XIANCI
nroot
2
spin
1
symmetry
1
MR-CBMRPT3
$END

Results:

=============================== For first type of CI with two singlet states ====================================

 ++++++++  DATA CHECK +++++++++++++++++++++++++++++++++
  CHECKDATA:MRPT3:PT3ENERGY:     -155.5176000     -155.2629435
 ++++++++++ END DATA CHECK ++++++++++++++++++++++++++++

xianci (last edited 2024-11-28 15:07:40 by bsuo)