Hi,
Hmmm...even though the SI file of the paper you have shared does point to using HSE06, it remains not entirely clear whether its parameters were kept default or altered (for all systems together or individually for instance).
There are also differences between what different codes consider as "default" settings. For example, within the code used in the paper (VASP, nice code, no doubt), the defaults for HSE06 read (taken from https://www.vasp.at/wiki/index.php/List_of_hybrid_functionals) :
$$ \omega= 0.2\ \mathring{A} , \quad c = 0.25, \quad \text{correlation}=\text{PBE}, $$ with the first number reading the range separation parameter (omega) and the second the fraction of exact exchange used (c).
Within CRYSTAL (also nice code, no doubt), these read (taken from the manual, page 138):
$$ \omega= 0.11\ a_0^{-1}, \quad c = 0.25, \quad \text{correlation}=\text{PBE}, $$ adopting the same labels.
Not sure about the exact definition of units (perhaps a developer can comment if this is indeed Bohr radius as assumed?), but you can already see the subtle differences having to be taken into account when comparing between codes.
A few other thoughts worth considering:
In the paper, the structure was optimized with PBEsol and on top of that geometry HSE06 was applied as a single-point calculation. Not sure about the exact composition of those ZIFs, but the structural differences could play a significant role as well (planewave codes are very costly when optimizing a structure with hybrid functionals). Here is also a good read on this topic: doi.org/10.1088/2516-1075/aafc4b
One final small comment. Within the PAW formalism implemented in VASP, scalar relativistic effects are included in the pseudopotentials by default. No problem, cool feature, but should be taken into account when comparing results, especially for heavier elements (longer discussion found here https://blog.vasp.at/forum/viewtopic.php?t=902)
Hope this helps!
Cheers,
Aleks
