Self Consistent Field (SCF)

The SCF procedure searches for a self-consistent density. The self-consistent error is the square root of the integral of the squared difference between the input and output density of the cycle operator. When the SCF error is below a certain criterion, controlled by subkey Criterion of block key Convergence, convergence is reached. In case of bad convergence the SCF looks at the subkeys Mixing, and Degenerate, and the subkeys of block key DIIS.

See also

Troubleshooting: SCF does not converge

SCF block

SCF
   Eigenstates [True | False]
   Iterations integer
   Method [DIIS | MultiSecant]
   Mixing float
   PMatrix [True | False]
   Rate float
   VSplit float
End
SCF
Type:Block
Description:Controls technical SCF parameters.
Eigenstates
Type:Bool
Description:The program knows two alternative ways to evaluate the charge density iteratively in the SCF procedure: from the P-matrix, and directly from the squared occupied eigenstates. By default the program actually uses both at least one time and tries to take the most efficient. If present, Eigenstates turns off this comparison and lets the program stick to one method (from the eigenstates).
Iterations
Type:Integer
Default value:300
GUI name:Maximum number of cycles
Description:The maximum number of SCF iterations to be performed.
Method
Type:Multiple Choice
Default value:DIIS
Options:[DIIS, MultiSecant]
Description:Choose the general scheme used to converge the density in the SCF. In case of scf problems one can try the MultiSecant alternative at no extra cost per SCF cycle. For more details see the DIIS and MultiSecantConfig block.
Mixing
Type:Float
Default value:0.075
Description:Initial ‘damping’ parameter in the SCF procedure, for the iterative update of the potential: new potential = old potential + mix (computed potential-old potential). Note: the program automatically adapts Mixing during the SCF iterations, in an attempt to find the optimal mixing value.
PMatrix
Type:Bool
Description:If present, evaluate the charge density from the P-matrix. See also the key Eigenstates.
Rate
Type:Float
Default value:0.99
Description:Minimum rate of convergence for the SCF procedure. If progress is too slow the program will take measures (such as smearing out occupations around the Fermi level, see key Degenerate of block Convergence) or, if everything seems to fail, it will stop
VSplit
Type:Float
Default value:0.05
Description:To disturb degeneracy of alpha and beta spin MOs the value of this key is added to the beta spin potential at the startup.

Convergence

All options and parameters related to the convergence behavior of the SCF procedure are defined in the Convergence block key. Also the finite temperature distribution is part of this

Convergence
   Criterion float
   Degenerate string
   ElectronicTemperature float
   InitialDensity [rho | psi]
   LessDegenerate [True | False]
   NoDegenerate [True | False]
   SpinFlip integer_list
   startwithmaxspin [True | False]
End
Convergence
Type:Block
Description:Options and parameters related to the convergence behavior of the SCF procedure.
Criterion
Type:Float
Description:Criterion for termination of the SCF procedure. The default depends on the NumericalQuality and on the number of atoms in the system.
Degenerate
Type:String
Default value:default
Description:Smooths (slightly) occupation numbers around the Fermi level, so as to insure that nearly-degenerate states get (nearly-) identical occupations. Be aware: In case of problematic SCF convergence the program will turn this key on automatically, unless the key ‘Nodegenerate’ is set in input. The smoothing depends on the argument to this key, which can be considered a ‘degeneration width’. When the argument reads default, the program will use the value 1e-4 a.u. for the energy width.
ElectronicTemperature
Type:Float
Default value:0.0
Unit:a.u.
Description:Simulates a finite-temperature electronic distribution using the defined energy. This may be used to achieve convergence in an otherwise problematically converging system. The energy of a finite-T distribution is different from the T=0 value, but for small T a fair approximation of the zero-T energy is obtained by extrapolation. The extrapolation energy correction term is printed with the survey of the bonding energy in the output file. Check that this value is not too large. Build experience yourself how different settings may affect the outcomes. Note: this key is meant to help you overcome convergence problems, not to do finite-temperature research! Only the electronic distribution is computed T-dependent, other aspects are not accounted for!
InitialDensity
Type:Multiple Choice
Default value:rho
Options:[rho, psi]
Description:The SCF is started with a guess of the density. There are the following choices RHO: the sum of atomic density. PSI: construct an initial eigensystem by occupying the atomic orbitals. The guessed eigensystem is orthonormalized, and from this the density is calculated/
LessDegenerate
Type:Bool
Default value:False
Description:If smoothing of occupations over nearly degenerate orbitals is applied (see Degenerate key), then, if this key is set in the input file, the program will limit the smoothing energy range to 1e-4 a.u. as soon as the SCF has converged ‘halfway’, i.e. when the SCF error has decreased to the square root of its convergence criterion.
NoDegenerate
Type:Bool
Default value:False
Description:This key prevents any internal automatic setting of the key DEGENERATE.
SpinFlip
Type:Integer List
GUI name:Flip spin for atoms
Description:List here the atoms for which you want the initial spin polarization to be flipped. This way you can distinguish between ferromagnetic and anti ferromagnetic states. Currently, it is not allowed to give symmetry equivalent atoms a different spin orientation. To achieve that you have to break the symmetry.
startwithmaxspin
Type:Bool
Default value:True
Description:To break the initial perfect symmetry of up and down densities there are two strategies. One is to occupy the numerical orbitals in a maximum spin configuration. The alternative is to add a constant to the potential. See also Vsplit key.

DIIS

The DIIS procedure to obtain the SCF solution depends on several parameters. Default values can be overruled with this block.

DIIS
   Adaptable [True | False]
   CHuge float
   CLarge float
   Condition float
   DiMix float
   NCycleDamp integer
   NVctrx integer
   Variant [DIIS | LISTi | LISTb | LISTd]
End
DIIS
Type:Block
Description:Parameters for the DIIS procedure to obtain the SCF solution
Adaptable
Type:Bool
Default value:True
Description:Change automatically the value of dimix during the SCF.
CHuge
Type:Float
Default value:20.0
GUI name:No DIIS (but damping) when coefs >
Description:When the largest coefficient in the DIIS expansion exceeds this value, damping is applied
CLarge
Type:Float
Default value:20.0
GUI name:Reduce DIIS space when coefs >
Description:When the largest DIIS coefficient exceeds this value, the oldest DIIS vector is removed and the procedure re-applied
Condition
Type:Float
Default value:1000000.0
Description:The condition number of the DIIS matrix, the largest eigenvalue divided by the smallest, must not exceed this value. If this value is exceeded, this vector will be removed.
DiMix
Type:Float
Default value:0.2
GUI name:Bias DIIS towards latest vector with
Description:Mixing parameter for the DIIS procedure
NCycleDamp
Type:Integer
Default value:1
GUI name:Do not start DIIS before cycle
Description:Number of initial iterations where damping is applied, before any DIIS is considered
NVctrx
Type:Integer
Default value:20
GUI name:Size of DIIS space
Description:Maximum number of DIIS expansion vectors
Variant
Type:Multiple Choice
Default value:DIIS
Options:[DIIS, LISTi, LISTb, LISTd]
Description:Which variant to use. In case of problematic SCF convergence, first try MultiSecant, and if that does not work the LISTi is the advised method. Note: LIST is computationally more expensive per SCF iteration than DIIS.

Multisecant

For more detais on the multisecant method see ref [1].

MultiSecantConfig
   CMax float
   InitialSigmaN float
   MaxSigmaN float
   MaxVectors integer
   MinSigmaN float
End
MultiSecantConfig
Type:Block
Description:Parameters for the Multi-secant SCF convergence method.
CMax
Type:Float
Default value:20.0
GUI name:Max coeff
Description:Maximum coefficient allowed in expansion
InitialSigmaN
Type:Float
Default value:0.1
GUI name:Initial
Description:This is a lot like a mix factor: bigger means bolder
MaxSigmaN
Type:Float
Default value:0.3
GUI name:Max
Description:Upper bound for the SigmaN parameter
MaxVectors
Type:Integer
Default value:20
GUI name:Number of cycles to use
Description:Maximum number of previous cycles to be used
MinSigmaN
Type:Float
Default value:0.01
GUI name:Min
Description:Lower bound for the SigmaN parameter

DIRIS

In the DIRIS block, which has the same options as the DIIS block, you can specify the DIIS options to be used in the Dirac subprogram, for numerical single atom calculations, which constructs the radial tables for the NAOs.

[1]L. D. Marks and D. R. Luke, Robust mixing for ab initio quantum mechanical calculations, Phys. Rev. B 78, 075114 (2008)