From e2ab723d66342562b365a31a5c7fb15889e4cd23 Mon Sep 17 00:00:00 2001 From: Luca Ghiringhelli Date: Sun, 4 Feb 2018 22:25:12 +0100 Subject: [PATCH] Edited QSHI yaml --- topological-quantum-phases/QSHI_trivial.demoinfo.yaml | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/topological-quantum-phases/QSHI_trivial.demoinfo.yaml b/topological-quantum-phases/QSHI_trivial.demoinfo.yaml index 33eeab9..ae07408 100644 --- a/topological-quantum-phases/QSHI_trivial.demoinfo.yaml +++ b/topological-quantum-phases/QSHI_trivial.demoinfo.yaml @@ -1,6 +1,6 @@ title: "Prediction of topological quantum phase transitions" logicalPath: "/data/shared/tutorialsNew/topological-quantum-phases/QSHI_trivial.bkr" -authors: ["Ahmetcik, Emre", "Ziletti, Angelo", "Ouyang, Runhai", "Ghiringhelli, Luca", "Scheffler, Matthias"] +authors: ["Mera Acosta, Carlos", "Ahmetcik, Emre", "Carbogno, Christian", "Ouyang, Runhai", "Fazzio, Adalberto", "Ghiringhelli, Luca", "Scheffler, Matthias"] editLink: "/notebook-edit/data/shared/tutorialsNew/topological-quantum-phases/QSHI_trivial.bkr" isPublic: true username: "tutorialsNew" @@ -8,7 +8,7 @@ description: > This tutorial shows how to find descriptive parameters (short formulas) for the prediction of topological phase transitions. As an example, we address the topological classification of two-dimensional functionalized honeycomb-lattice materials, which are formally described by - the $Z_2$ topological invariant, i.e., $Z_2=0$ for trivial (normal) insulators and $Z_2=1$ for two-dimensional + the Z2 topological invariant, i.e., Z2=0 for trivial (normal) insulators and Z2=1 for two-dimensional topological insulators (quantum spin Hall insulators). Using a recently developed machine learning based on compressed sensing, we then derive a map of these materials, in which metals, trivial insulators, and quantum spin Hall insulators are separated -- GitLab