Dear Louis,

Thank you for using the ESM. The figure 1 in the paper shows how does the unit 
cell place in the z-direction. As you see, we need to put enough vacuum region 
on both sides of a slab. Accordingly, the 3rd cell parameter (Lz) becomes 
large. The z0 is not equal to Lz but equal to Lz/2.

There are some example calculations in ESM_examle directory. I recommend you to 
have a look at the Aluminum (001) slab calculations with various boundary 
conditions. 

Best regards,
Minoru

--------------------------------------------------------------------------------------------------------
Minoru Otani
National Institute of Advanced Industrial Science and Technology
Research Centre for Computational Design of Advanced Functional Materials
email : [email protected] <mailto:[email protected]>
---------------------------------------------------------------------------------------------------------

> On Feb 23, 2017, at 21:42, Louis Fry-Bouriaux <[email protected]> wrote:
> 
> Hi there,
> 
>     I am trying to understand the ESM example with bc2 (metal-slab-metal) 
> distributed with QE 6.0 which consists of an Al(001) slab between two 
> electrodes, and at the same time I am trying to replicate the results of 
> Otani and Sugino in their paper (Phys. Rev. B, 73, 115407, 2006) which 
> consists of an Al/Si(111)/Al slab between two screening boundaries.
> 
> I have a few questions:
> 
> ** 1. ** In the QE example the following cell params and atomic positions are 
> specified:
> 
> CELL_PARAMETERS bohr
>  10.82227686   0.00000000   0.00000000
>   0.00000000  10.82227686   0.00000000
>   0.00000000   0.00000000  22.67672253
> ATOMIC_POSITIONS bohr
> Al  0.00000000   0.00000000   0.00000000
> Al  5.41113843   0.00000000   0.00000000 
> Al  0.00000000   5.41113843   0.00000000 
> Al  5.41113843   5.41113843   0.00000000 
> 
> My understanding is that the cell will repeat without overlapping atoms along 
> X and Y. What I'm not clear on is why the 3rd lattice vector is so large?
> 
> The parameter 'esm_w' defaults to zero and is not specified in the example, 
> so does this large value mean that there is a region of vacuum? Or does it 
> just repeat the atoms such that in the Z-direction there are 5 Al layers? I'm 
> guessing that this 3rd cell parameter Z-value corresponds to L_z, which in 
> the paper corresponds to z_0?
> 
> ** 2. ** I have reproduced the 'surface unit cell' from Otani/Sugino's paper 
> using VESTA.
> 
> My concern here is with the correct repetition of atoms in X and Y, and what 
> exactly happens with the Z direction. I realize I must first rotate the unit 
> cell such that the repeated Al atoms lie perpendicular to the Z Cartesian 
> axis which I have not done yet.
> 
> I have tested the repetition of this cell within VESTA along vectors 
> perpendicular to the Al plane. So my most important question is: if the 
> height of the cell along Z is ~14.4281 Angstrom (measured from Al center 
> plane), then the third 'CELL_PARAMETERS' entry (after rotation) should be 
> this value exactly + the 'decay length' of the wavefunction in Z? Then the 
> parameter 'esm_w' is used to set z_1 from the paper I suppose?
> 
> I will generate an xyz file of the surface cell, but if I repeat by 3.816 A 
> along a surface lattice vector, it is a matter of just deleting the entries 
> that cause an overlap of the atoms I suppose?
> 
> Thank you for your time and sorry for the very long email,
> Kindest regards,
> Louis
> 
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