<div dir="ltr"><div>Dear Lorenzo,</div><div><br></div><div>a calculation of this kind should work in principle: to include spin-orbit effects, at least one atomic species must be described with a fully relativistic pseudopotential, so using a fully relativistic pseudopotential for the substrate and a scalar-relativistic one for the overlayer is a reasonable way to test how much of the effect comes from the overlayer SOC itself.<br>That said, if the goal is to make a reliable statement about the physical origin of the splitting, I would still recommend using fully relativistic pseudopotentials for all species in the final calculations. In many systems the enhancement is not due purely to the heavy atom’s intrinsic SOC, nor purely to symmetry lowering, but to their interplay. The overlayer can modify the symmetry of the surface or interface and at the same time hybridize with the surface state, transferring spin-orbit character to it. A well-known example is graphene/WSe2, where even a relatively weak van der Waals interaction leads to mixing between graphene pi states and spin-orbit-active WSe2 states. The interface symmetry then determines which kind of induced SOC terms can appear, for example Rashba-like terms when inversion symmetry is broken, and in some systems valley-Zeeman-like terms.<br>I would also pay attention to the bonding mechanism between the surface and the overlayer. If the interaction is weak, a proper treatment of van der Waals forces may be important, since the induced spin-orbit effects can be very sensitive to interlayer distance and hybridization.</div><div><br></div><div>Giovanni</div><div><div dir="ltr" class="gmail_signature" data-smartmail="gmail_signature"><div dir="ltr"><span style="color:rgb(0,0,0)">-- <br><br>Prof. Giovanni Cantele<br>Dipartimento di Fisica "Ettore Pancini"<br>Universita' degli Studi di Napoli "Federico II"<br>Complesso Universitario M. S. Angelo - Ed. 6<br>Via Cintia, I-80126, Napoli, Italy<br>e-mail: <a href="mailto:giovanni.cantele@unina.it" target="_blank">giovanni.cantele@unina.it</a><br>Phone: +39 081 676910<br><br>Web page: </span><a href="https://sites.google.com/view/giovanni-cantele/home" style="color:rgb(17,85,204)" target="_blank">https://sites.google.com/view/giovanni-cantele/home</a><br></div></div></div><br></div><br><div class="gmail_quote gmail_quote_container"><div dir="ltr" class="gmail_attr">Il giorno mer 25 mar 2026 alle ore 11:26 Lorenzo Sponza <<a href="mailto:lorenzo.sponza@onera.fr">lorenzo.sponza@onera.fr</a>> ha scritto:<br></div><blockquote class="gmail_quote" style="margin:0px 0px 0px 0.8ex;border-left:1px solid rgb(204,204,204);padding-left:1ex"><div style="font-size:10pt;font-family:Verdana,Geneva,sans-serif">
<p>Dear Users and Developers,</p>
<p>I am studying the electronic structure of a surface covered by a heavy metal overlayer. I have reasons to think that the interaction between the two elements enhances the spin-orbit splitting of a particular surface state. I would like to understand which is the dominating effect in such an enhancement : is it mainly due to symmetry changes induced by the overlayer or to the spin-orbit carried by the overlayer's atoms?</p>
<p>To this aim, I'm planning to run a simulation with a full-relativistic pseudopotential for the substrate element, and a scalar-relativistic one for the overlayer atoms. My questions are (1) Is that a safe procedure, i.e. does QE handle such a mixed kind of simulation? (2) Is there any other delicate aspects I should be aware of when carrying out a simulation like this?</p>
<p>Many thanks in advance. Cheers </p>
<div id="m_9204430877285132577signature">-- <br>
<div style="margin:0px;padding:0px;font-family:monospace">Dr. Lorenzo Sponza<br><br>Chargé de Recherche au CNRS<br>Université Paris-Saclay, ONERA, CNRS Laboratoire d'étude des microstructures (LEM)<br>29 Avenue de la division Leclerc, 92322 Châtillon<br>Tel: +33146734464<br><br>ETSF Research Team Leader <br>European Theoretical Spectroscopy Facility<br><a href="https://sites.unimi.it/etsf/" rel="noopener noreferrer" target="_blank">https://sites.unimi.it/etsf/</a></div>
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