# 4.2.4. CASVB¶

This program can be used in two basic modes:

variational optimization of quite general types of nonorthogonal MCSCF or modern valence bond wavefunctions

representation of CASSCF wavefunctions in modern valence form, using overlap- (

*relatively inexpensive*) or energy-based criteria.

For generating representations of CASSCF wavefunctions, the program is invoked by the command CASVB. For variational optimization of wavefunctions it is normally invoked inside RASSCF by the sub-command VB (see the RASSCF documentation).

Bibliography: see [38][39][40][41].

## 4.2.4.1. Dependencies¶

The CASVB program needs the JOBIPH file from a RASSCF calculation, and in addition also the ONEINT and ORDINT files from SEWARD.

## 4.2.4.2. Files¶

### 4.2.4.2.1. Input files¶

CASVB will use the following input files: ONEINT, ORDINT, RUNFILE, JOBIPH, (for more information see Section 4.1.1.2), and VBWFN with valence bond wavefunction information (orbital and structure coefficients).

### 4.2.4.2.2. Output files¶

- JOBIPH
On exit, the RASSCF interface file is overwritten with the CASVB wavefunction.

- VBWFN
Valence bond wavefunction information (orbital and structure coefficients).

## 4.2.4.3. Input¶

This section describes the input to the CASVB program. The input for each module is preceded by its name like:

```
&CASVB
```

### 4.2.4.3.1. Keywords¶

Optional keywords

- END of Input
This marks the end of the input to the program.

Optional keywords to define the CASSCF wavefunction. Not generally required because values stored in the job interface file or used by the RASSCF program will normally be appropriate.

- FROZen
Specifies frozen orbitals, as in the RASSCF program.

- INACtive
Specifies inactive orbitals, as in the RASSCF program.

- NACTel
Specifies the number of active electrons, as in the RASSCF program.

- RAS2
Specifies RAS2 orbitals, as in the RASSCF program.

- SPIN
Specifies the total spin, as in the RASSCF program.

- SYMMetry
Specifies the CASSCF wavefunction symmetry, as in the RASSCF program.

Optional keywords to define the VB wavefunction

- CON
The spatial VB configurations are defined in terms of the active orbitals, and may be specified using one or more CON keywords:

CON n1 n2 n3 n4 ...

The configurations can be specified by occupation numbers, so that \(n_i\) is the occupation of the \(i\)th valence bond orbital. Alternatively a list of \(N_{\text{act}}\) orbital numbers (in any order) may be provided — the program determines which definition applies. The two specifications

`1 0 1 2`

and`1 3 4 4`

are thus equivalent.Input configurations are reordered by CASVB, so that configurations have non-decreasing double occupancies. Configurations that are inconsistent with the value for the total spin are ignored.

If no configurations are specified the single “covalent” configuration \(\phi_1\phi_2\cdots\phi_{N_{\text{act}}}\) is assumed.

- COUPle
COUPLE key

`key`

may be chosen from`KOTANI`

(default),`SERBER`

,`RUMER`

,`PROJECT`

or`LTRUMER`

, specifying the scheme for constructing the spin eigenfunctions used in the definition of valence bond structures.`PROJECT`

refers to spin functions generated using a spin projection operator,`LTRUMER`

to Rumer functions with the so-called “leading term” phase convention.- WAVE
WAVE N S1 S2 ...

This keyword can be used to specify explicitly the number of electrons and spin(s) to be used with a configuration list. If \(N\) is less than the present number of active electrons, the input wavefunction fragment is assumed to form part of a direct product. Otherwise, the spins specified may be greater than or equal to the SPIN value specified as input to the RASSCF program. Defaults, for both \(N\) and \(S\), are the values used by RASSCF.

Optional keywords for the recovery and/or storage of orbitals and vectors

- STARt
START key-1=filename-1 key-2=filename-2 ...

Specifies input files for VB wavefunction (

`key-i`

=VB), CASSCF CI vector (`key-i`

=CI) and/or CASSCF molecular orbitals (`key-i`

=MO). By default, the required information is taken from the file JOBOLD.- SAVE
SAVE key-1=filename-1 key-2=filename-2 ...

Specifies output files for VB wavefunction (

`key-i`

=VB) and/or the VB CI vector (`key-i`

=VBCI). By default, the VB CI vector is written to the file JOBIPH.

Optional keywords to override the starting guess

- GUESs
GUESS key-1 ... key-2 ... ENDGUESs

The GUESS keyword initiates the input of a guess for the valence bond orbitals and/or structure coefficients.

`key-i`

can be either ORB or STRUC. These keywords modify the guess provided by the program. It is thus possible to modify individual orbitals in a previous solution so as to construct the starting guess. The ENDGUESs keyword terminates the guess input.ORB i c1 c2 ... cmact

Specifies a starting guess for valence bond orbital number \(i\). The guess is specified in terms of the \(m_{\text{act}}\) active MOs defining the CASSCF wavefunction.

STRUC c1 c2 ... cNVB

Specifies a starting guess for the \(N_{\text{VB}}\) structure coefficients. If this keyword is not provided, the perfect-pairing mode of spin coupling is assumed for the spatial configuration having the least number of doubly occupied orbitals. Note that the definition of structures depends on the value of COUPLE. Doubly occupied orbitals occur first in all configurations, and the spin eigenfunctions are based on the singly occupied orbitals being in ascending order.

- ORBPerm
ORBPERM i1 ... imact

Permutes the orbitals in the valence bond wavefunction and changes their phases according to \(\phi_j'=\sign(i_j)\phi_{\abs(i_j)}\). The guess may be further modified using the GUESS keyword. Additionally, the structure coefficients will be transformed according to the given permutation (note that the configuration list must be closed under the orbital permutation for this to be possible).

Optional keywords for optimization control

- CRIT
CRIT method

Specifies the criterion for the optimization.

`method`

can be OVERLAP or ENERGY (OVERLAP is default). The former maximizes the normalized overlap with the CASSCF wavefunction:\[\max\left(\frac{\braket{\Psi_{\text{CAS}}}{\Psi_{\text{VB}}}} {\left(\braket{\Psi_{\text{VB}}}{\Psi_{\text{VB}}}\right)^{1/2}}\right)\]and the latter simply minimizes the energy:

\[\min\left(\frac{\braopket{\Psi_{\text{VB}}}{\hat{H}}{\Psi_{\text{VB}}}}{\braket{\Psi_{\text{VB}}}{\Psi_{\text{VB}}}}\right).\]- MAXIter
MAXITER Niter

Specifies the maximum number of iterations in the second-order optimizations. Default is \(N_{\text{iter}}\)=50.

- (NO)CASProj
(NO)CASPROJ

With this keyword the structure coefficients are picked from the transformed CASSCF CI vector, leaving only the orbital variational parameters. For further details see the bibliography. This option may be useful to aid convergence.

- SADDle
SADDLE n

Defines optimization onto an \(n\)th-order saddle point. See also [42].

- (NO)INIT
(NO)INIT`

Requests a sequence of preliminary optimizations which aim to minimize the computational cost while maximizing the likelihood of stable convergence. This feature is the default if no wavefunction guess is available and no OPTIM keyword specified in the input.

- METHod
METHOD key

Selects the optimization algorithm to be used.

`key`

can be one of: FLETCHER, TRIM, TRUSTOPT, DAVIDSON, STEEP, VB2CAS, AUGHESS, AUG2, CHECK, DFLETCH, NONE, or SUPER. Recommended are the direct procedures DFLETCH or AUGHESS. For general saddle-point optimization TRIM is used. Linear (CI only) optimization problems use DAVIDSON. NONE suspends optimization, while CHECK carries out a finite-difference check of the gradient and Hessian.The default algorithm chosen by CASVB will be usually be adequate.

- TUNE
TUNE ...

Enables the input of individual parameters to be used in the optimization procedure (

*e.g.*for controlling step-size selection and convergence testing). Details of the values used are output if`print(3)`

\(\geq\) 3 is specified. For expert use only.- OPTIm
More than one optimization may be performed in the same CASVB run, by the use of OPTIM keywords:

OPTIM [... ENDOPTIM]

The subcommands may be any optimization declarations defined in this section, as well as any symmetry or constraints specifications. Commands given as arguments to OPTIM will apply only to this optimization step, whereas commands specified outside will act as default definitions for all subsequent OPTIM specifications.

The OPTIM keyword need not be specified if only one optimization step is required,

When only a machine-generated guess is available, CASVB will attempt to define a sequence of optimization steps that aims to maximize the likelihood of successful convergence (while minimizing CPU usage). To override this behaviour, simply specify one or more OPTIM keywords. The ENDOPTIm keyword marks the end of the specifications of an optimization step.

- ALTErn
A loop over two or more optimization steps may be specified using:

ALTERN Niter ... ENDALTERN

The program will repeat the specified optimization steps until either all optimizations have converged, or the maximum iteration count, \(N_{\text{iter}}\), has been reached. The ENDALTErn keyword marks the end of the specification of an ALTERN loop.

Optional keywords for definitions of molecular symmetry and any constraints on the VB wavefunction

- SYMElm
Various issues associated with symmetry-adapting valence bond wavefunctions are considered, for example, in [43].

SYMELM label sign

Initiates the definition of a symmetry operation referred to by

`label`

(any three characters).`sign`

can be \(+\) or \(-\); it specifies whether the total wavefunction is symmetric or antisymmetric under this operation, respectively. A value for`sign`

is not always necessary but, if provided, constraints will be put on the structure coefficients to ensure that the wavefunction has the correct overall symmetry (note that the configuration list must be closed under the orbital permutation induced by`label`

for this to be possible). The default for`label`

is the identity.The operator is defined in terms of its action on the active MOs as specified by one or more of the keywords IRREPS, COEFFS, or TRANS. Any other keyword, including optional use of the ENDSYMElm keyword, will terminate the definition of this symmetry operator.

IRREPS i1 i2 ...

The list \(i_1, i_2 \ldots\) specifies which irreducible representations (as defined in the CASSCF wavefunction) are antisymmetric with respect to the

`label`

operation. If an irreducible representation is not otherwise specified it is assumed to be symmetric under the symmetry operation.COEFFS i1 i2 ...

The list \(i_1, i_2 \ldots\) specifies which individual CASSCF MOs are antisymmetric with respect to the

`label`

operation. If an MO is not otherwise specified, it is assumed to be symmetric under the symmetry operation. This specification may be useful if, for example, the molecule possesses symmetry higher than that exploited in the CASSCF calculation.TRANS ndim i1 ... indim c1,1 c1,2 ... cndim,ndim

Specifies a general \(n_{\text{dim}}\times n_{\text{dim}}\) transformation involving the MOs \(i_1, \ldots i_{n_{\text{dim}}}\), specified by the \(c\) coefficients. This may be useful for systems with a two- or three-dimensional irreducible representation, or if localized orbitals define the CASSCF wavefunction. Note that the specified transformation must always be orthogonal.

- ORBRel
In general, for a VB wavefunction to be symmetry-pure, the orbitals must form a representation (not necessarily irreducible) of the symmetry group. Relations between orbitals under the symmetry operations defined by SYMELM may be specified according to:

ORBREL i1 i2 label-1 label-2 ...

Orbital \(i_1\) is related to orbital \(i_2\) by the sequence of operations defined by the

`label`

specifications (defined previously using SYMELM). The operators operate right to left. Note that \(i_1\) and \(i_2\) may coincide. Only the minimum number of relations required to define all the orbitals should be provided; an error exit will occur if redundant ORBREL specifications are found.- (NO)SYMProj
As an alternative to incorporating constraints, one may also ensure correct symmetry of the wavefunction by use of a projection operator:

(NO)SYMPROJ [irrep-1 irrep-2 ...]

The effect of this keyword is to set to zero the coefficients in unwanted irreducible representations. For this purpose, the symmetry group defined for the CASSCF wavefunction is used (always a subgroup of \(D_{2h}\)). The list of irreps in the command specifies which components of the wavefunction should be kept. If no irreducible representations are given, the current wavefunction symmetry is assumed. In a state-averaged calculation, all irreps are retained for which a non-zero weight has been specified in the wavefunction definition. The SYMPROJ keyword may also be used in combination with constraints.

- FIXOrb
FIXORB i1 i2 ...

This command freezes the orbitals specified in the list \(i_1, i_2 \ldots\) to that of the starting guess. Alternatively the special keywords ALL or NONE may be used. These orbitals are eliminated from the optimization procedure, but will still be normalized and symmetry-adapted according to any ORBREL keywords given.

- FIXStruc
FIXSTRUC i1 i2 ...

Freezes the coefficients for structures \(i_1, i_2 \ldots\). Alternatively the special keywords ALL or NONE may be used. The structures are eliminated from the optimization procedure, but may still be affected by normalization or any symmetry keywords present.

- DELStruc
DELSTRUC i1 i2 ...

Deletes the specified structures from the wavefunction. The special keywords ALL or NONE may be used. This specification should be compatible with the other structure constraints present, as defined by SYMELM and ORBREL.

- ORTHcon
ORTHCON key-1 ... key-2 ... ...

The ORTHCON keyword initiates the input of orthogonality constraints between pairs/groups of valence bond orbitals. The sub-keywords

`key-i`

can be any of ORTH, PAIRS, GROUP, STRONG or FULL. Orthogonality constraints should be used with discretion. Note that orthogonality constraints for an orbital generated from another by symmetry operations (using the ORBREL keyword) cannot in general be satisfied. The ENDORTHcon keyword can be used to terminate the input of orthogonality constraints.ORTH i1 i2 ...

Specifies a list of orbitals to be orthogonalized. All overlaps between pairs of orbitals in the list are set to zero.

PAIRS i1 i2 ...

Specifies a simple list of orthogonalization pairs. Orbital \(i_1\) is made orthogonal to \(i_2\), \(i_3\) to \(i_4\), etc.

GROUP label i1 i2 ...

Defines an orbital group to be used with the ORTH or PAIRS keyword. The group is referred to by

`label`

which can be any three characters beginning with a letter a–z. Labels defining different groups can be used together or in combination with orbital numbers in ORTH or PAIRS. \(i_1, i_2 \ldots\) specifies the list of orbitals in the group. Thus the combination GROUP AAA 1 2 GROUP BBB 3 4 ORTH AAA BBB will orthogonalize the pairs of orbitals 1–3, 1–4, 2–3 and 2–4.STRONG

This keyword is short-hand for strong orthogonality. The only allowed non-zero overlaps are between pairs of orbitals (\(2n-1\), \(2n\)).

FULL

This keyword is short-hand for full orthogonality and is mainly useful for testing purposes.

Optional keywords for wavefunction analysis

- CIWEights
For further details regarding the calculation of weights in CASVB, see [44].

CIWEIGHTS key-1 key-2 ... [Nconf]

Prints weights of the CASSCF wavefunction transformed to the basis of nonorthogonal VB structures. For the

`key-i`

options see VBWEIGHTS below. Note that the evaluation of inverse overlap weights involves an extensive computational overhead for large active spaces. Weights are given for the total CASSCF wavefunction, as well as the orthogonal complement to \(\Psi_{\text{VB}}\). The default for the number of configurations requested, \(N_{\text{conf}}\), is 10. If \(N_{\text{conf}} = -1\) all configurations are included.- REPOrt
REPORT [... ENDREPORT]

Outputs orbital/structure coefficients and derived information. The ENDREPOrt keyword can be used to mark the end of the specification of a report step.

- (NO)SCORr
(NO)SCORR

With this option, expectation values of the spin operators \((\hat{s}_\mu+\hat{s}_\nu)^2\) are evaluated for all pairs of \(\mu\) and \(\nu\). Default is NOSCORR. The procedure is described in [45][46][47].

This analysis is currently only implemented for spin-coupled wavefunctions.

- VBWEights
For further details regarding the calculation of weights in CASVB, see [44].

VBWEIGHTS key-1 key-2 ...

Calculates and outputs weights of the structures in the valence bond wavefunction \(\Psi_{\text{VB}}\).

`key-i`

specifies the definition of nonorthogonal weights to be used, and can be one of:- CHIRGWIN
Evaluates Chirgwin–Coulson weights (see [48]).

- LOWDIN
Performs a symmetric orthogonalization of the structures and outputs the subsequent weights.

- INVERSE
Outputs “inverse overlap populations” as in [49].

- ALL
All of the above.

- NONE
Suspends calculation of structure weights.

The commands LOWDIN and INVERSE require the overlap matrix between valence bond structures, so that some additional computational overhead is involved.

Optional keywords for further general options

- PREC
PREC iprec iwidth

Adjusts the precision for printed quantities. In most cases,

`iprec`

simply refers to the number of significant digits after the decimal point. Default is`iprec`

=+8.`iwidth`

specifics the maximum width of printed output, used when determining the format for printing arrays.PRINT i1 i2 ...

Each number specifies the level of output required at various stages of the execution, according to the following convention:

**-1**No output except serious, or fatal, error messages.**0**Minimal output.**1**Standard level of output.**2**Extra output.The areas for which output can be controlled are: \(i_1\)

\(i_1\) Print of input parameters, wavefunction definitions, etc.

\(i_2\) Print of information associated with symmetry constraints.

\(i_3\) General convergence progress.

\(i_4\) Progress of the 2nd-order optimization procedure.

\(i_5\) Print of converged solution and analysis.

\(i_6\) Progress of variational optimization.

\(i_7\) File usage.

For all, the default output level is +1. If \(i_5 \geq 2\) VB orbitals will be printed in the AO basis (provided that the definition of MOs is available).

- SHSTruc
Prints overlap and Hamiltonian matrices between VB structures.

- STATs
STATS

Prints timing and usage statistics.

### 4.2.4.3.2. Input example¶

```
&seward
symmetry
x y
basis set
c.sto-3g....
c 0 0 -0.190085345
end of basis
basis set
h.sto-3g....
h 0 1.645045225 1.132564974
end of basis
&scf
occupied
3 0 1 0
&rasscf
inactive
1 0 0 0
ras2
3 1 2 0
nactel
6 0 0
lumorb
&casvb
```

### 4.2.4.3.3. Viewing and plotting VB orbitals¶

In many cases it can be helpful to view the shape of the converged valence bond orbitals, and Molcas therefore provides two facilities for doing this. For the Molden program, an interface file is generated at the end of each CASVB run (see also Section 4.3.1). Alternatively a CASVB run may be followed by RASSCF to get orbitals (Section 4.2.44) and GRID_IT with the VB specification (Section 4.2.22), in order to generate a three-dimensional grid, for viewing, for example, with LUSCUS program.