Orca
Orca is a free software for all types of QM calculations.
Documentation and tutorials are here: https://www.orcasoftware.de/tutorials_orca
The current version is 5.0.3.
It is installed on Aurora:
module add GCC/11.2.0 OpenMPI/4.1.1 ORCA/5.0.3-static
Then, it is run by
orca input_file >output
Avogadro is a good option to illustrate Orca output
This is a simple sample input file:
! RHF def2-SVP # Level of theory.
!
SP
# Single-point energy calculation; it is default or
!
OPT
# Geometry optimisation
* xyz 0
1
# Charge, and multiplicity followed by coordinates in Å (can be changed to a.u. by %coords Units bohrs)
h
1.57623125918282
-1.40098816005358 1.92944524289998
c
3.11804788185000
-1.26044723466300 3.33347664459600
h
4.63927730299500
-2.45475405971100 2.62293967273200
h
3.85126156558200
0.66329382213900 3.40150678020000
h
2.59270405690800
-1.91429242685700 5.21564372964000
*
Alternatively, internal coordinates can be used:
* int 0 2
O 0 0 0 0.0 0.0 0.0
H 1 0 0 0.9903 0.0 0.0
*
Alternatively, an xyz file can be used:
* xyzfile 0 2 hydroxide.xyz
File hydroxide.xyz:
2 # number of atoms; next line blank or title
O 0 0 0
H 0 0 0.9903
Alternatively, an pdb file can be used:
* pdbfile 0 2 hydroxide.pdb
It seems that the pdb file must contain at least one row with occupancy
and B-factors; otherwise, you get strange error messages:
HETATM 1 O
2 2 -20.282
7.868 -0.800 1.00 0.00
Input file is not case sensitive.
Constraints:
%geom
Constraints
{B 0 1 1.25 C} # Bond length constraint
end
end
Cartesian coordinate constraints:
%geom
Constraints
{C 3 C } # Atom 4 is fixed
{C 10:17 C} # A list of atoms is also allowed
end
end
Note that Orca number atoms starting with 0, which may be very confusing in the beginning.
Options
Use different basis sets for different atoms
! B3LYP def2-SVP
%basis
NewGTO C "def2-TZVP" end # Applies TZVP to all C atoms
NewGTO 6 "def2-TZVP" end # Applies TZVP to all C atoms
end
Unfortunately, such simple input cannot be used for individual atoms (a
number is interpreted as an element number, not an atom number.
For individual atoms, it needs to be given in the coordinate input, e.g.:
! TPSS D4 DEF2-SV(P)
* xyz -1 1
H 2.384 3.207 1.496
S -0.935 0.285 2.326 newgto "ma-def2-SV(P)" end
H -2.837 -2.703 1.492
*
Strangely, it seems that the coordinates then must be in the main input
file, not in a file reference. You can have it in the pdb file, but it
is ignored.
However, you may use fragments to change basis sets of certain atoms
(note that the fragment definition changed between Orca 6.0 and 6.1):
! TPSS D4 DEF2-SV(P)
%PAL NPROCS 24 END
%basis
FragBasis 1 "def2-SV(P)"
FragBasis 2 "ma-def2-SV(P)"
end
* pdbfile -1 1 coord.pdb
%frag
Definition
1 {0:25 27:107 113:114 116:146 150:164} end
2 {26 108:112 115 147:149} end
end
end
Use RI and RIJCOSX (exchange)
!B3LYP def2-SVP def2/J RIJDX RIJCOSX
In fact, this is default for DFT; to turn it off, use !NORI and !NOCOSX
Dispersion correction
!D3 or !D4
Increase amount printed out (e.g. to print orbitals)
!HF def2-SVP Largeprint
Frequency calculation
!FREQ
!TightOpt or !VeryTightOpt may remove imaginary freqs
Implicit solvent (COSMO is no longer any option)
!CPCM(solvent)
or
%CPCM
EPSILON 80
REFRAC 1.33
END
or
%CPCM SMD TRUE
SMDSolven "solvent"
END
Relativistic corrections
!B3LYP ZORA ZORA-def2-TVP RIJDX SARC/J
DLPNO CC
!DLPNO-CCSD(T) def2-TZVPP def2-TZVPP/C
Change maximum number of geometry steps
%geom
maxiter 1
end
Cartesian optimisation
! COpt
SCF options
%scf
MaxIter 300
CNVDIIS 1
CNVSOSCF 1
end
%scf
guess moread
moinp "TS2-opt.gbw"
maxiter 999
end
Level shift
%scf
CNVShift true # default = true
LShift 0.1 # default = 0.25
ShiftErr 0.1 #default = 0.0
# more convenient:
Shift Shift 0.1 ErrOff 0.1 end
end
Output options
%output
print[p_mos] true
print[p_basis] 5
end
Paralell calculations
%pal
nprocs
20
#Maximum number of cores of your machine.
end
or simply pal16, e.g.
!QMMM PBE0 6-31G* D3ZERO Opt pal16
Point charges with file reference
%pointcharges "pointcharges.pc"
File pointcharges.pc
418 # number of point charges
0.294300
6.494988 -4.096926
-5.179739 # charge and coordinates
0.164200
7.320798 -3.807798
-6.874823
0.164200
6.417509 -5.943188
-4.694079
...
No special ending
Atomic units
Geometry options
%geom
MaxIter 200
TS_search EF
# ! OptTs
TolE 5e-6
TolRMSG 1e-4
TolMaxG 3e-4
TolRMSD 2e-3
TolMaxD 4e-3
inhess GFNFF
end
TS optimisation
!QMMM PBE0 6-31G* D3ZERO OptTS SlowConv TightSCF pal16
Scan a reaction coordinate
%geom scan
B 11 2275 [2.0 1.9 1.8] end
end
Dihedral:
%geom
scan
D N1 N2 N3 N4 = initial-angle, final-angle, Nsteps
end
end
Steps of 10–15º are appropriate, not bigger
Read a wavefunction from an old calculation
! MOREAD
%moinp "myorbitals.gbw"
For single-point calculations, if a *.gbw file of the same name is
found, this file is renamed to *.ges and the orbitals are used as start
orbitals. If this is not descired, set AUTOSTART false
Example for a system that is hard to converge the SCF (nitrogenase)
! TPSS D4 DEF2-SV(P) UKS
! ENGRAD
! NOTRAH
! SlowConv
! TightSCF
%scf
MaxIter 1000
DIISMaxEq 40
DirectResetFreq 1
end
%PAL NPROCS 48 END
*pdbfile -2 1 qm_1_h.pdb
NOTRAH - turns off a newer (failsafe) scf converger
SlowConv - Selects appropriate SCF converger criteria for difficult cases. Most transition metal complexes fall into this category
VerySlowConv - Try this for very difficult cases
%MaxCore 2000
Flip spin
First converge HS state and then flip to BS stat
!UKS DEFGRID3 R2SCAN D4 ZORA
!TightSCF TRAH
%scf
SCFMode Direct
Thresh 1e-15
TCut 1e-15
Flipspin 0 # Here atom number zero is flipped
FinalMs 0.0 # Here the final broken-symmetry state to converge to is selected (here, MS=0)
end
*xyzfile -1 11 fe2h_tzvp.xyz
TD-DFT calculations
! CAM-B3LYP DEF2-SV(P) def2/j RIJCOSX UKS
! Opt
! CPCM
%cpcm
epsilon 4.0
end
%tddft
nroots 100
iroot 1
maxdim 7
maxiter 5000
end
%PAL NPROCS 32 END
*pdbfile 0 1 qm_1_h.pdb
Results are found after ABSORPTION SPECTRUM
Output
File *.in contains the input
*.out the output (very long)
*.engrad energy, gradient and coordinates.
*** FINAL ENERGY EVALUATION AT THE STATIONARY POINT ***
Dispersion correction -0.077894975
FINAL SINGLE POINT ENERGY -2474.907119623929
FINAL SINGLE POINT ENERGY (QM/MM) -2507.427748516620
Scans:
*** OPTIMIZATION RUN DONE ***
RELAXED SURFACE SCAN STEP 6
RELAXED SURFACE SCAN RESULTS
----------------------------
Column 1: NONAME
The Calculated Surface using the 'Actual Energy'
2.00000000 -2507.39966580
1.90000000 -2507.42805085
1.80000000 -2507.42978390
The Calculated Surface using the SCF energy
2.00000000 -2474.80098184
1.90000000 -2474.82795119
1.80000000 -2474.82969327
QM/MM with Orca
Described in the Orca manual under
8.13 ORCA Multiscale Implementation
You need a prmtop file and a pdb file (and preferably a syst1 file)
1. Make an Orca input file:
!QMMM PBE0 6-31G* D3ZERO
%qmmm
ORCAFFFilename "prmtop3.ORCAFF.prms"
QMAtoms { 0:33
642:653
2238:2239
2248:2275
4716:4718 } end
ActiveAtoms { 0:33
642:653
2238:2239
2248:2275
4716:4718 } end
end
*pdbfile 0 1 pdb3.pdb
Made from the syst1 file, but renumbering to start on 0, changing "-" to ":" and removing link atoms.
The link atoms should be removed from QMAtoms list, but not from ActiveAtoms list.
2. Convert prmtop file to Orca format
orca_mm -convff -AMBER prmtop
Gives you the file prmtop3.ORCAFF.prms
It seems to have problems with metals and other two-character elements.
3. Finally start Orca with
orca orca.in >orca.out
This does additive QM/MM and electrostatic embedding.
You may change the charges around the junction atoms (p. 375). Orca
implements the Charge Shift (CS; default), Redistributed charge and
dipole (RCD), as well as the Z0, Z1, Z2 and Z3 methods.
%qmmm
chargeAlteration RCD
end
4. Output (in *.out):
FINAL SINGLE POINT ENERGY (MM) -32.522715848742
FINAL SINGLE POINT ENERGY -2474.898029955347
FINAL SINGLE POINT ENERGY (QM/MM) -2507.420745804089
*** OPTIMIZATION RUN DONE ***
Protein free
!QMMM PBE0 6-31G* D3ZERO OPT
%PAL NPROCS 24 END
%qmmm
ORCAFFFilename "prmtop3.ORCAFF.prms"
QMAtoms { 0:33
642:653
2238:2239
2248:2275
4716:4718 } end
ActiveAtoms { 0:33
642:653
2238:2239
2248:2275
4716:4718 } end
ExtendActiveRegion distance
Dist_AtomsAroundOpt 6.
PrintOptRegionExt true
end
*pdbfile 0 1 pdb3.pdb
If you start from a ComQum calculation, the ActiveAtom list can be
taken from the belly in the sander.in3 file, but it must be extended
also with all QMAtoms and also all junction atoms.
NEB calculations
!QMMM PBE0 6-31G* D3ZERO NEB-TS SlowConv TightSCF pal16
%neb
Product_PDBFile "orca-prod.pdb"
TS_PDBFile "TSGuess.pdb"
NImages 8
NEB_TS false
end
%qmmm
ORCAFFFilename "prmtop3.ORCAFF.prms"
QMAtoms { 0:33
642:653
2238:2239
2248:2275
4716:4718 } end
ActiveAtoms { 0:33
642:653
2238:2239
2248:2275
4716:4718 } end
end
*pdbfile 0 1 orca-reac.pdb
Output in orca.out
*** THE NEB OPTIMIZATION HAS
CONVERGED ***
PATH
SUMMARY
5 4.727
-2507.39972
20.33 0.02832 0.00417
<= CI
INFORMATION ABOUT SADDLE POINT
Energy
.... -2507.39972016 Eh
It seems that Orca requires coordinates of the junction atoms to be the same in all three pdb files (in variance to ComQum).
Useful greps
grep 'FINAL SINGLE' *.out
# Greps for all occurrences of convergence parameters in ORCA as they are displayed after each geom opt step
grep -A8 "Geometry convergence"
grep " MAX gradient"
grep "ENERGY (QM/MM)" $1 | tail -n 1 ;
neb_energies() {
# Gets the energies of the last step
of an ORCA .NEB.log file and creates a temporary path vs energy
file.
# $1: file to grep for QM/MM energies
tail -n 30 $1 | grep energy | tail -n 1 | sed
's/energy : //g'| tr -s ' ' '\n' >
energies ;
tail -n 30 $1 | grep distance $1 | tail -n 1 | sed
"s/distance : //g" | tr -s ' '
'\n' > abscissa ;
paste abscissa energies > tmp_path_energies ;
rm -fr abscissa energies ;
}