Open amdmaniac opened 3 years ago
The SCC can somehow arrive at a non-physical solution for early transition metals. You could try another guess with
$scc
guess=sad
Sometimes this helps to converge the SCC to a physically correct solution for early transition metals.
I have tried
$scc guess=sad $end
and also
$scc guess=gasteiger $end
but with no success. GFN2-xTB as well as GFN1-xTB still behave totally wrong.
If the electronic structure is completely off with the xTB Hamiltonian, it might be worth trying the GFN-FF instead.
GFN-FF and GFN0-xTB work fine. However, I have to check the accuracy of their geometries with respect to PBEh-3c for the physical properties that I am interested in.
Describe the bug
Geometry optimization for C(34)H(36) system with Ti atom introduced in it goes nuts using GFN2-xTB (6.3.3). Please see the attached xtb2.trj.xyz file. The same is also true for GFN1-xTB (6.3.3).
To Reproduce
../xtb input.xyz --gfn 2 --opt tight --uhf 0 --chrg 0 > output.out
The input file input.xyz is attached.
Expected behaviour
The system under consideration is physically relevant as the analogous geometry optimizations with PBE/def2-SVP or PBEh-3c (as implemented in ORCA 4.2.1) are perfectly fine. Please see the attached pbeh-3c.trj.xyz file.
Additional context
In my opinion, there is something wrong with the description of Ti atom. If Ti atom is interchanged with Ni atom (of a similar kind), GFN2-xTB causes no issues.
Files.zip