The algorithms in Spartan will typically perform well on most systems when solving
quantum mechanical equations.
However, there are times when one may see "convergence problems".
What to do when this occurs? The following
covers the typical areas to examine when a calculation has
The first question to ask is "Am I having problems converging
the geometry, or the wavefunction?" The answer to this question
will lead to different sections of this FAQ below.
The first section "General Issues" covers some topics which are
relevant to both geometry and wavefunction (SCF) convergence.
Some common convergence issues:
If you've made it this far, you have examined your molecule and
believe everything is correct in the calculation setup. Now it's
time to delve deeper
into the calculation. The first thing to do is determine whether
problems are related to the geometry optimization or the
self-consistent field calculation (SCF) of the wave function. If
you have one or more geometry cycles displayed in the output
dialogue, the problem is likely related to geometry optimization.
(Of course, there may be exceptions, so examine the error
Examine the molecule carefully. Try the same calculation at
a simpler theory level or with a smaller basis set. If the lower
theories work, they are likely good starting points for
advanced theories. (For quantum chemical calculations, theoretical approaches are listed in order of increasing complexity: Semi Empirical < Hartree-Fock < Density Functional < Configuration Interaction and Moller Plesset < Advanced Correlated).
Examine the molecule's current geometry carefully; do the
bond distances and angles seem correct? (Or nearly correct?)
Molecular Mechanics can sometimes produce strange results when metals
are involved. Semi-empirical is fast and often very good, but it
also may also suffer from poor approximations, and may not be good
enough for your molecule.
Another common problem is that the
current geometry may have a symmetry that is not
a reasonable energy minima in the theory you are attempting
to use. Turning "Symmetry" off is sometimes
appropriate; this can be done by using the
Sometimes it is also necessary to physically break symmetry
by slightly changing bond distances or angles. (Watch the
symmetry label in the bottom right of the screen to determine if
your changes are large enough.)
Make sure to count electrons and look for radicals in your
molecule. The charge and number of unpaired electrons
specified in the
Calculation Dialogue must be consistent with the
- Unpaired Electrons
Are there unpaired
electrons? If so, you may want to choose an unrestricted
calculation by typing either SCF=UNRESTRICTED or
keyword in the options field in the Calculations dialogue.
If your system includes a metal atom, ask yourself if the
metal is in a high or low spin state. Hemoglobin
complexing with Carbon-dioxide and molecular Oxygen are
where spin states need to be accounted for. Make sure
the multiplicity is consistent with the state you desire.
In questionable configurations one may need to try differing
number of unpaired electrons to see which one has the lowest
calculated energy. (i.e. 0,2,4... or
1,3,5... etc. depending on
whether there is an even or odd total number of electrons.)
The use of symmetry can dramatically speed up calculations on
small symmetric molecules. However attempting to use symmetry
can sometimes cause difficulty in convergence. Use the
IGNORESYMMETRY keyword to disable the use of symmetry.
As mentioned in the
it is sometimes useful to physically break symmetry.
The following section includes several references to "keywords". Keywords are type-in options, to be entered in the "Options" field in
Spartan's Calculation dialogue. Keywords are NOT case sensitive. Multiple keywords are separated
- Re-examine the geometry.
If the starting geometry is poor, some
new chemistry might be occurring that you do not anticipate.
For example, if a hydrogen is too close to a
nitrogen, a bond may form (that you don't want) Recall
that the bonds drawn on the screen mean absolutely nothing to
the quantum calculations.
At times the job may be converging normally, just slowly, and
one only needs to resubmit a job that has 'run out
of cycles'. But before you resubmit, examine the current
conformation of the molecule.
Jobs that run out of cycles do so because atoms have
moved a lot during the geometry optimization. Chances are
that some chemistry is occurring (a bond forming or breaking)
that you may not desire.. This could be due to poor
initial geometry (see above) or a poor initial Hessian
Adding the GEOMETRYCYCLES=xxx or OPTCYCLE=xxx
(where xxx is some large number) keyword should keep the job
from terminating early.
It is also possible that the algorithm is seeking the minima
(or transition state) at a higher level of precision than
you need. You can change the precision criteria by
using the GRADIENTTOLERANCE=x or
DISTANCETOLERANCE=x. (TOLG=x or TOLD=x
are shorter versions of these keywords.)
- Check the Hessian
The most common problem with
geometry optimizations is that the default Hessian is poor.
Usually a molecular mechanics Hessian saves many geometry optimization
steps for standard systems, and semi-empirical Hessians are
good for transition searches. (These are the defaults). But
these defaults can sometimes be poor approximations for molecules
outside their range of parameterization.
You can choose a
conservative Hessian with the HESS=UNIT keyword. While
this will typically avoid bad modes in the Hessian, it does
slow the optimization procedures.
The best Hessian is one generated at the same theory level
as the one you are attempting use for optimization. Often this is too
expensive (from a time perspective) to calculate, but if you
are having trouble you may
want to generate this high quality Hessian. This can be
accomplished by doing an energy calculation with the
IR button checked. (This will generate a
Hessian.) When this completes you can resubmit the job as a
geometry optimization (or transition state optimization).
- Start simple
It is always good advice to start by using
a lower theory level. In general we suggest using the
Minimizer (the Minimize button in the Spartan interface uses
molecular mechanics to reduce strain energy and 'clean up'
molecules that have been constructed by hand), and then
(perhaps) doing a
quick geometry optimization at a simple level of theory such
as semi-empirical or Hartree-Fock with a small basis (3-21G*).
There are, however, instances when this might not be a good idea; for
example, one should NOT typically use the Minimizer before
submitting a Transition State Geometry optimization. There are
also cases where a lower level theory level may simply produce poor
results on your type of molecule. After some hands-on experience you
will know better than anyone else what works for your favorite
class of molecules.
Another approach is useful when building large
You can repeat this procedure until the full molecule
is complete. The above approach is often useful when
searching for transition states.
- Start with a small core of your molecule and
optimize it at the theory you desire.
- Then add some atoms to the
core, (perhaps minimizing the new atoms with molecular
mechanics, while 'freezing' the original core)
- Optionally, you may want to freeze the core atoms and
minimize the new atoms at a lower theory level.
You can use molecular mechanics in the Spartan interface
(the Minimize button), or any other
theory from the Calculations dialogue. (Make sure to
select the "Frozen Atoms" box
next to the words "Subject To:" in the
- Then submit the entire molecule for a final
geometry optimization. Make sure to deselect "frozen
atoms" in the calculations dialogue.
- A word ab coordinates
While the simplest coordinate system for geometry optimization
is Cartesian, Spartan will commonly use an internal coordinate
system (sometimes referred to as
“redundant internal coordinates” [RIC] or
“delocalized internal coordinates”).
This takes into account the standard bonding of tetrahedral sp3
and planar-like sp2 systems.
This also speeds up geometry optimizations by more than a factor
of 2 for typical organic systems. There are cases where the internal
coordinate system can cause a problem, particularly when the
geometry changes significantly during the optimization or in
some high-coordination systems. In these cases you may want
to turn the default behavior off by using the
(entered into the Options line of the Calculations dialogue).
Spartan treats Transition State searches as a special case of geometry
optimizations. Because of the flat nature of the potential
and other unique characteristics of transition states,
transition state geometry tasks can be
more difficult to perform than the typical ground state
The above discussion on geometry optimizations holds for
transition state geometries. The strategy of starting small
and working up to larger molecules and methods applies to
transition state searching. However, for efficient transition
state searches the importance of a good starting geometry and a
good Hessian are especially critical.
A good starting geometry can be found using Spartan's
transition state builder/searching feature. A number of
examples of using this can be found in Chapter 11 of our
Spartan '16 Tutorial and User's Guide. (Also see the sections
on Spartan Reaction Database and Transition States
in Chapter 23 for additional information on these features.)
Setting up an Energy Profile calculation is another way of getting a
good starting point for transition state geometry tasks.
Once a good starting point is found a good Hessian is
required. Often Spartan's default Hessian (a semi-empirical
guess) is good enough.
The best Hessian is obtained from an initial IR/frequency
i.e. First do a single point energy calculation with the IR
property checked. When this completes, examine the
vibrations (Display Menu > Spectra).
Ideally there is one negative frequency (noted with an "i" in
front of the frequency), and upon animating,
this should look like motion along the reaction coordinate
associated with the transition state.
If largest imaginary
frequency is not what you expect, or there are no imaginary
frequencies, the starting geometry is not close enough to the
In very difficult cases I sometimes force
a complete analytical/exact Hessian every few cycles. For
example assuming the geometry is close to the actual transition
- Do a single point energy with IR selected.
- Check to make sure there is only 1 negative eigenvalue, and
that it looks right by animating it.
- Run a TS with the keyword OPTCYCLE=5 (or some small
number). This job will (most likely) run out of optimization
- Go back to step 1 to get the real/exact hessian and repeat.
If at any point in step 2 you discover that there is no longer
a good negative eigenvalue you need to adjust the geometry.
One useful strategy is to do an energy profile calculation to
find a rough
TS. The SN2 Reaction of Bromide and Methyl Chloride
tutorial and the Thermodynamic vs. Kinetic Control
tutorial (from Chapter 11 of the Spartan '16 Tutorial
and User's Guide provide good examples of this strategy.