I've currently got the same lattice structure as that in chapter 4.6, with
the same layout of supercell (i.e. one point in the middle and a quarter of
a point on each corner), but am not getting the results I'm expecting-I
think the problem lies with either the k_point setting, or an incorrect
phase-if I'm honest I'm not sure what the phase offset should be. Could
someone confirm the correct k-point in terms of the lattice vector and
correct phase offset for an x-polarised source above the plane of the
lattice?

 

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Lydia Fulloway

Scientist

Malvern Optical Ltd

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email:  <mailto:lafullo...@malvernoptical.co.uk>
lafullo...@malvernoptical.co.uk

 

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From: Ardavan Oskooi <ardavan.osk...@gmail.com> 
Sent: 14 October 2020 01:45
To: lafullo...@malvernoptical.co.uk; meep-discuss@ab-initio.mit.edu
Subject: Re: [Meep-discuss] Phase offsets of sources in supercells

 

You can set the relative phase of any two sources using the amplitude
property. Note that if you set the amplitude to a complex value, you will
also likely need to set force_complex_fields=True in the Simulation
constructor since Meep uses real fields by default.

For more details on sources in supercells, see Section 4.6 of our book
chapter: https://arxiv.org/abs/1301.5366.

On 10/13/20 02:11, lafullo...@malvernoptical.co.uk
<mailto:lafullo...@malvernoptical.co.uk>  wrote:

Hi, I've been using a supercell to represent a non-orthogonal lattice. I
know I need to use two sources to counter the effects of band folding in
reflection or transmission measurements, however I'm struggling to get the
correct results out from simulations. The two (Gaussian) sources currently
in the supercell are separated by a lattice vector, but I think the problem
lies with the phase offset between them. Does anyone know how to correctly
use a time delay between the two sources (or any other method) in order to
create the correct phase offset for countering band folding?

 

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