Appendices¶
Extended XYZ file format¶
The .xyz
file format is a simple text based format for molecular geometries.
.xyz
files have the number of atoms in the first line, followed by a comment
line, followed by one line per atom, specifying the element as well as the x, y,
and z coordinates of this atom.
However, the standard .xyz
file format does not include lattice vectors. AMS
therefore uses an extended .xyz
file format which is also suitable for
periodic systems. In this extended format the lattice vectors are specified at
the end of the .xyz
file via the keys VEC1
, VEC2
and VEC3
. For
1D periodic systems (chains) only VEC1
is needed. For 2D periodic systems
(slabs) only VEC1
and VEC2
are needed. An example extended .xyz
for
graphene looks like this:
2
C 0.0 0.0 0.0
C 1.23 0.71014 0.0
VEC1 2.46 0.0 0.0
VEC2 1.23 2.13042 0.0
Note that the extended .xyz
format is also understood by the AMS GUI for
importing and exporting geometries from/to .xyz
files.
Developer options¶
Print
Timers [None | Normal | Detail | TooMuchDetail]
End
Print
- Type
Block
- Description
This block controls the printing of additional information to stdout.
Timers
- Type
Multiple Choice
- Default value
None
- Options
[None, Normal, Detail, TooMuchDetail]
- Description
Printing timing details to see how much time is spend in which part of the code.
EngineDebugging
AlwaysClaimSuccess Yes/No
CheckInAndOutput Yes/No
ForceContinousPES Yes/No
IgnoreGradientsRequest Yes/No
IgnorePreviousResults Yes/No
IgnoreStressTensorRequest Yes/No
NeverQuiet Yes/No
RandomFailureChance float
RandomNoiseInEnergy float
RandomNoiseInGradients float
RandomStopChance float
End
EngineDebugging
- Type
Block
- Description
This block contains some options useful for debugging the computational engines.
AlwaysClaimSuccess
- Type
Bool
- Default value
No
- Description
If an engine fails, pretend that it worked. This can be useful when you know that an SCF might fail.
CheckInAndOutput
- Type
Bool
- Default value
No
- Description
Enables some additional checks on the input and output of an engine, e.g. for NaN values.
ForceContinousPES
- Type
Bool
- Default value
No
- Description
If this option is set, the engine will always run in continuous PES mode. For many engines this disables the use of symmetry, as this one always leads to a discontinuous PES around the symmetric points: Basically there is jump in the PES at the point where the symmetry detection starts classifying the system as symmetric. Normally the continuous PES mode of the engine (often disabling the symmetry) is only used when doing numerical derivatives, but this flag forces the engine to continuously run in this mode.
IgnoreGradientsRequest
- Type
Bool
- Default value
No
- Description
If this option is set, the engine will not do analytical gradients if asked for it, so that gradients will have to be evaluated numerically by AMS.
IgnorePreviousResults
- Type
Bool
- Default value
No
- Description
If this option is set, the engine will not receive information from previous calculations. Typically this information is used to restart the self consistent procedure of the engine.
IgnoreStressTensorRequest
- Type
Bool
- Default value
No
- Description
If this option is set, the engine will not calculate an analytical stress tensor if asked for it, so that the stress tensor will have to be evaluated numerically by AMS.
NeverQuiet
- Type
Bool
- Default value
No
- Description
Makes the engine ignore the request to work quietly.
RandomFailureChance
- Type
Float
- Default value
0.0
- Description
Makes the engine randomly report failures, even though the results are actually fine. Useful for testing error handling on the application level.
RandomNoiseInEnergy
- Type
Float
- Default value
0.0
- Unit
Hartree
- Description
Adds a random noise to the energy returned by the engine. The random contribution is drawn from [-r,r] where r is the value of this keyword.
RandomNoiseInGradients
- Type
Float
- Default value
0.0
- Unit
Hartree/Angstrom
- Description
Adds a random noise to the gradients returned by the engine. A random number in the range [-r,r] (where r is the value of this keyword) is drawn and added separately to each component of the gradient.
RandomStopChance
- Type
Float
- Default value
0.0
- Description
Makes the engine randomly stop. Can be used to simulate crashes.
Symmetry¶
Schönfliess symbols and symmetry labels¶
A survey of all molecular point groups that are recognized by AMS is given below. The table contains the Schönfliess symbols together with the names of the subspecies of the irreducible representations as they are used by AMS to label normal modes.
Point |
Schönfliess |
Irreducible representations |
Group |
Symbol in AMS |
|
C1 |
NOSYM |
A |
C∞v |
C(LIN) |
Sigma Pi |
D∞h |
D(LIN) |
Sigma.g Sigma.u Pi.g Pi.u |
I |
I |
A T1 T2 G H |
Ih |
I(H) |
A.g A.u T1.g T1.u T2.g T2.u G.g G.u H.g H.u |
O |
O |
A1 A2 E T1 T2 |
Oh |
O(H) |
A1.g A1.u A2.g A2.u E.g E.u T1.g T1.u T2.g T2.u |
T |
T |
A E T |
Th |
T(H) |
A.g A.u E.g E.u T.g T.u |
Td |
T(D) |
A1 A2 E T1 T2 |
Ci |
C(I) |
A.g A.u |
Sn |
S(N) |
n=4: A B E |
n=6: A.g A.u E.g E.u |
||
n=8: A B E1 E2 E3 |
||
Cn |
C(N) |
n=2: A B |
n=4: A B E |
||
even n: A B E1 E2 … |
||
n=3: A E |
||
odd n: A E1 E2 … |
||
Cnv |
C(NV) |
n=2: A1 A2 B1 B2 |
n=4: A1 A2 B1 B2 E |
||
even n: A1 A2 B1 B2 E1 E2 … |
||
n=3: A1 A2 E |
||
odd n: A1 A2 E1 E2 … |
||
Cs |
C(S) |
A’ A’’ |
Cnh |
C(NH) |
n=2: A.g A.u B.g B.u |
n=4: A.g A.u B.g B.u E.g E.u |
||
even n: A.g A.u B.g B.u E1.g E1.u E2.g E2.u … |
||
n=3: A’ A’’ E’ E’’ |
||
odd n: A’ A’’ E1’ E1’’ E2’ E2’’ … |
||
Dn |
D(N) |
n=2: A B1 B2 B3 |
n=4: A1 A2 B1 B2 E |
||
even n A1 A2 B1 B2 E1 E2 … |
||
n=3: A1 A2 E |
||
odd n: A1 A2 E1 E2 … |
||
Dnd |
D(ND) |
n=2: A1 A2 B1 B2 E |
even n: A1 A2 B1 B2 E1 E2 … |
||
n=3: A1.g A1.u A2.g A2.u E.g E.u |
||
odd n: A1.g A1.u A2.g A2.u E1.g E1.u E2.g E2.u … |
||
Dnh |
D(NH) |
n=2: A.g A.u B1.g B1.u B2.g B2.u B3.g B3.u |
n=4: A.g A.u B1.g B1.u B2.g B2.u B3.g B3.u E.g E.u |
||
even n: A.g A.u B1.g B1.u B2.g B2.u B3.g B3.u E1.g E1.u E2.g E2.u … |
||
n=3: A1’ A1’’ A2’ A2’’ E’ E’’ |
||
odd n: A1’ A1’’ A2’ A2’’ E1’ E1’’ E2’ E2’’ … |
The symmetry labeling may depend on the choice of coordinate system. For instance, B1 and B2 representations in Cnv are interchanged when you rotate the system by 90 degrees around the z-axis so that x-axis becomes y-axis and vice-versa (apart from sign).
Molecular orientation requirements¶
In order that AMS recognizes the (sub)symmetry of a molecule, the molecule has to have a specific orientation in space.
The origin is a fixed point of the symmetry group.
The z-axis is the main rotation axis.
xy is the \(\sigma\)h -plane (axial groups, C(s)).
The x-axis is a C2 axis (D symmetries).
The xz-plane is a \(\sigma\)v -plane (Cnv symmetries).
In Td and Oh the z-axis is a fourfold axis (S4 and C4 , respectively) and the (111)-direction is a threefold axis.
If the system is symmetrized (and no symmetry is given in the System block key) the molecular structure is rotranslated into this standard orientation.
Molecular orientation conventions¶
The molecular requirements for AMS may not fully determine the orientation of the molecule, like for D2h molecules. See Mulliken 1 for standard conventions on the molecular orientation and notation. A few of these conventions are listed below:
in planar C2v molecules the x axis is perpendicular to the plane of the molecule.
in planar D2h molecules the x axis is perpendicular to the plane of the molecule and the z-axis passes through the greatest number of atoms. If the last condition is not decisive, the z-axis should pass through the greatest number of bonds.
in planar D4h and D6h molecules the C2-axis passes through the greatest number of atoms. If the last condition is not decisive, the C2-axis should pass through the greatest number of bonds.
- 1
R.S Mulliken, Report on Notation for the Spectra of Polyatomic Molecules, Journal of Chemical Physics 23, 1997 (1955)