Dear Jan,

Just to complement  Joseph's answer:
For the conductance calculation, this would be very easy to do with a recursive Green's function algorithm:
You need to use the concept of non-uniform leads and apply the generalized Fisher-Lee formula [1] and then you just  will  need  to update one self energy for each new length.
I have done this  for scanning gate microscopy simulations where we need to change the position of a scatterer at each step (So larger system at each step).

Kwant uses a different approach to get the conductance and the scattering matrix, so if it is just a matter of time, it is better to keep using kwant than writing a new recursive code.

If you need help with the second approach let me know.

I hope  this helps. 
Adel 

[1] https://journals.aps.org/prb/abstract/10.1103/PhysRevB.81.155422

On Mon, Oct 30, 2017 at 3:43 PM, Jan Behrends <jb@pks.mpg.de> wrote:
Dear all,

I'm looking for a workaround for a problem I currently face: when computing the two-terminal conductance for a system of length L, is there a way to get the conductance for the same system of length 1,2,..L-1 on the fly (while keeping everything else the same, i.e., same width, same disorder configuration etc.)?

As far as I understand how the scattering matrix calculation works internally, it shouldn't take much longer to compute these intermediate values than just getting the final conductance.

Best,

Jan

--
Jan Behrends
Max-Planck-Institut für Physik komplexer Systeme
Nöthnitzer Straße 38, 01187 Dresden, Germany
E-Mail: jb@pks.mpg.de




--
Abbout Adel